CA2246545A1 - Optical fiber with light extractor - Google Patents

Abstract

A light extractor is provided which comprises a disperse phase of polymeric particles disposed within a continuous birefringent matrix. The extractor is oriented, typically by stretching, in one or more directions. The size and shape of the disperse phase particles, the volume fraction of the disperse phase, the film thickness, and the amount of orientation are chosen to attain a desired degree of diffuse reflection and total transmission of electromagnetic radiation of a desired wavelength in the resulting extractor.

Description

OPTICAL FIBER WITH LIGHT EXTRACTOR

Field of the Invention This invention relates to optical materials which contain structures suitable for controlling optical char~ctPri~tics, such as reflectance and tr~n~mi~ion. In a further aspect, it relates to the use of such m~tt-ri~lc as light extractors ~or optical fibers.

Background Optical films are known to the art which are constructed from i~ ions dispersed within a continuous matrix. The ~~h~r~-~teri~tics of these inclusions can be manipulated to provide a range of reflective and tr~n.~mi~cive ~r~ ,. Lies to the 15 film. These ch~r~rt~ri~tics include inclusion size with respect to wavelengthwithin the film, inclusion shape and ~ nm~ont, inclusion volumetric fill factor and the degree of l~rldc~i~re index mi~m~t~h with the continuous matrix along the film's three orthogonal axes.
Conventional absorbing (dichroic) polarizers have, as their inclusion phase, 20 inorganic rod-like chains of light-absorbing iodine which are aligned within a polymer matrix. Such a filrn will tend to absorb light polarized with its electric field vector aligned parallel to the rod-like iodine chains, and to L~1s~1liL light polarized perpendicular to the rods. Because the iodine chains have two or more ~limen~ions that are small co111pd-~d to the wavelength of visible light, and because 2s the number of chains per cubic wavelength of light is large, the optical ~1op.,.~ies of such a filrn are pred~ 1h1dlely specular, with very little diffuse tr~n~mi~inn through the film or diffuse reflection from the film sllrf~rPc- Like most other comm~rcially available pol~ri~rs, these pol~ri7in~ films are based on polarization-selective absorption.
Films filled with inorganic inclusions with dirr~l~,.lL characteristics can provide other optical tr~n~mi~ion and reflective ~ ellies. For example, coated CA 02246545 l998-08-l7 mica flakes with two or more ~lim~ inns that are large compared with visible wavelengths, have been incol~ol~lcd into polymeric films and into paints to impart a metallic glitter. I hese flakes can be manipulated to lie in the plane of the film, thereby hll~ling a strong directional depencl~n~ e to the reflective appearance.5 Such an effect can be used to produce security screens that are highly reflective for certain viewing angles, and tr~n~mi~ive for other viewing angles. Large flakes having a coloration (specularly selective reflection) that depends on ~lignm~nt with respect to inci~l~nt light, can be incorporated into a film to provide evidence of L~llpeL;llg. In this application, it is n~ces~ that all the flakes in the film be 10 similarly aligned with respect to each other.
However, optical films made from polymers filled with il,o.ga. ic in~ sions suffer from a variety of infinnitiçs Typically, adhesion bc;lwecll the~llOlgi~ic particles and the polymer matrix is poor. Consequently, the optical P1~JP~-L Lies of the film decline when stress or strain is applied across the matrix, 15 both be~,ause the bond bt;Lw~:cll the matrix and the inclusions is colllp.~ ised, and becilu:je the rigid inorganic inclusions may be Çld~Lulcd. Fullllc~lllore, ~lipnm~nt of inorganic inclusions le.lu-~es process steps and concid~r~tions that cr mplic~t~
m~nllf:~r*lrin~
Other films, such as that fii~-~losefl in U.S. 4,688,900 (Doane et. al.), 20 consists of a clear light~ ; . .g continuous polymer matrix, with droplets of light mo~31l1~tin~ liquid crystals dispersed within. Stretching of the m~teri~l l~ ~JolLcdly results in a distortion of the liquid crystal droplet from a sph~ri~l to an ellipsoidal shape, with the long axis of the ellipsoid parallel to the direction of stretch. U.S. 5,301,041 (Konuma et al.) make a similar rli~clos lre, but achieve the 2s distortion of the liquid crystal droplet Llllou~ll the application of ~ Ult;. A.
Aphonin, "~ptical Properties of Stretched Polymer Dispersed Liquid Crystal Films: Angle-Dependent Polarized Light Sc;~ ., Liauid Crvstals. Vol. 19, No.
4, 469-480 (1995), ~ c~ ç~ the optical ~ Lies of stretched films con~i.ctin~ of Iiquid crystal droplets disposed within a polymer matrix. He reports that the 30 elon~ti~-n of the droplets into an ellipsoidal shape, with their long axes parallel to the stretch direction, imparts an ori~nt~l birefringence (~crld ;li~e index dif~erence among the rlim~n~ional axes of the droplet) to the droplets, res-llting in a relative refractive index mi~m~trh between the dispersed and continuous phases along certain film axes, and a relative index match along the other film axes. Such liquid crystal droplets are not small as compared to visible wavelengths in the film, and s thus the optical ~.o~l Lies of such films have a substantial diffuse component to ~ their reflective and tr~n~mi~ive plv~c~lies. ~ph(min suggests the use of these materials as a pols~ri7ing diffuser for backlit twisted nematic LCDs. However, optical films employing liquid crystals as the disperse phase are ~llb~L~lLiallylimited in the degree of refractive index mi~m~tch between the matrix phase and 0 the dispersed phase. Furth~rmore, the birefringence of the liquid crystal colll~o~ of such filrns is typically sensitive to Lt;lll~laLule~
U. S. 5,268,225 (lsayev) discloses a composite l~ e made from t_ermokopic liquid crystal polymer blends. The blend consists of two liquid crystal polymers which are immi~rible with each other. The blends may be cast 5 into a film c~ n~i~tin~ of a ~ pP~rserl inrl~ n phase and a contimlous phase. When t_e film is stretched, the fii~per~P~ phase forms a series of fibers whose axes are aligned in the direction of stretch. While the film is ~lesrribe~ as having improved ".~ jrsll pl~p~ ies, no mP.ntinn iS made ofthe optical pl.~p~,lLies ofthe film.
.. . ..

Other optical films have been made by incorporating a dispersion of inclusions of a first polymer into a second polymer, and then stretching the resulting composite in one or two directions. U. S. 4,871,784 (Otonari et al. ) is exemplative of this technology. The polymers are selected such that there is low5 adhesion beL~V~e~1 the dispersed phase and the surrounding matrix polymer, so that an elliptical void is formed around each inclusion when the film is stretched. Such voids have dirnensions of the order of visible wavelength~ The refractive index mi~m~tch between the void and the polymer in these "microvoided" films is typically quite large (about 0.5), c~ inp ~ub:jL~lLial diffuse reflection. However, 0 the optical ~loL,~,.Lies of microvoided m~t.oris~l~ are difficult to control because of variations of the geo,ntL.~ of the int~rf~ce~ and it is not possible to produce a film axis for which .~L~ iv-e indices are relatively m~tchr~l as would be useful for pol~ri7~ti~ n s~lsiLiv~ optical ~ Lies. Ft~~ ...ore, t_e voids in such m~teri~l can be e~ily collapsed through ~ Jo~u-~ to heat and ~lei,~ulc~
Optical films have also been made wll~,.cin a dispersed phase is detennini~tir~lly arranged in an ordered pattern within a c~ ous matrix. U. S.
5,217,794 (Schrenk) is exemplative ofthis tçcl~n- logy. There, a l~mrll~r polymeric film is ~i~closecl which is made of polymeric incl~ n~ which are largec~,my~ d with wavelength on two axes, disposed within a continuous matrix of 20 another polymeric m~t~n~l The refractive index of the dispersed phase differssigmficantly from that of the continll- us phase along one or more of the l~ 1 e's axes, and is relatively well m~trhr<l along another. Rer~tlee of the ordering of the dispersed phase, films of this type exhibit strong irir1esc~onre (i.e., interference-based angle depPn-lrnt coloring) for in~t~nces in which they are ~ lly 2s reflective. As a result, such films have seen limited use for optical applications where optical diffusion is desirable.
There thus remains a need in the art for an optical m~teri~l con~i.ctin~ of a continuous and a dispersed phase, wherein the refractive index mi~m~trll betweenthe two phases along the m~t~ori~l's three ~l;.. L--i;onal axes can be conveniently and 30 p~ .lIy ~ ipulated to achieve desirable degrees of diffuse and spect~lar reflection and triqn~miq~ion, wherein the optical m~ten~l is stable with respect to -stress, strain, temperature differences, and electric and m~gn~tic fields, and wherein the optical m~t.ori~l has an in~ignificant level of iriclescen~ e These and other needs are met by the present invention, as hereinafter disclosed s Brief Description of the l~ s FIG 1 is a schem~tic drawing illustrating an optical body made in accordance with the present invention, wherein the disperse phase is arranged as a series of elongated masses having an çcc~nti~lly circular cross-section;
FIG. 2 is a srh~tic drawing illustrating an optical body made in accordance with the present invention, wherein the di~ e phase is arranged as a series of e]on~t~A masses having an çssenti~lly elliptical cross-section, FIGS. 3a-e are sch~m~tic drawings illu~Lldlillg various shapes of the di~. .~e phase in an optical body made in accordal1ce with the present invention, FIG 4a is a graph of the bidirectional scatter distribution as a function of 15 sc~U~ d angle for an oriented film in accoldace with the present invention for light polarized perp~nt1ic~ r to o.ienl~Lion direction, FIG 4b is a graph of the bidirectional scatter distribution as a function of sc~ d angle for an ~rient~l film in accord~.ce with the present invention for light polarized parallel to orientation direction;
FIG. S is a s~ ;c rep.~se.. L~Lion of a multilayer film made in accordance with the present invention;
FIGS. 6a and 6b are electron micrographs of optical films made in accor~ce with the present invention;
FIG. 7 is a perpendicular tr~n~mi~ n ~e ;L ul.- for films made in 25 acco.d~.ce with the present invention;
FIG 8 is a s~ . hl;c diagram ilh1~tr~ting the use ofthe films ofthe present invention as high efficiency light extractors for optical fibers; and FIGS 9A and 9B are graphs showing re}ative gain as a function of angle for the films of the present invention and for a con.~ iially available optical film, 30 ~ e-;Li~rely S~ ~ry of the Invention In one aspect, the present invention relates to a diffusely reflective film or other optical body comrrixin~ a birefringent continuous polymeric phase and a subst~nti~lly nonbirefringent disperse phase disposed within the continuous phase.
s The indices of refraction of the continuous and disperse phases are~substantially mi.cm:lteh~l (i.e., differ from one another by more than about 0.05) along a first of three mutu~lly orthogonal axes, and are sllhst~nti~lly m~tl~.h~d (i.e., differ by less than about 0.05~ along a second of three mutually orthogonal axes. In some emboAil"r.,l~;, the indices of refraction ofthe continuous and Aiep~rsÇ phases can lo be ~,ul~ lly m~tchecl or mix~l~n~ pfl along, or parallel to, a third of threem~ lly orthogonal axes to produce a mirror or a polarizer. Tnr;~ nt light polari_ed along, or parallel to, a miem~trh~A axis is sc~L~..,d, ~ in ei~nifiç~nt diffuse reflection- Tn~ nt light polari~d along a m~trh~A axis is sc~L~ ,d to a much lesser degree and is significantly spectrally ~ llxln;l leA These ls p.o~c.~ies can be used to mal~e optical films for a variety of uses, including low loss (signifie~ntly nollal~soll,mg~ reflective polarizers for which polslri7~fione of light that are not .ei~nifir~ntly l l n~ P~l are diffusely refl~ctefl In a related aspect, the present invention relates to an optical film or other optical body c- mrrieing a birefringçnt continuous phase and a ~liepprse phase, 20 wh~ the indices of refraction of the cnntinll~ us and Aier~rse phases are Yllbs~n--l;~lly m~teh~A (i.e., wherein the index diL~ ce between the C~ ;....nuxand d,sl.~,.xe phases is less than about 0.05) along an axis perp~n~lir~ r to a surface of the optical body.
In another aspect, the present invention relates to a composite optical body 25 ct~mpriein~ a polymeric continU~us birefringent first phase in which the disperse second phase may be bilciLm~ellL, but in which the degree of match and 1-- ix...,. l~ h in at least two orthogonal directions is primz~rily due to the birefringçn~e of the first phase.
In still another aspect, the present invention relates to a method for 30 obtaining a diffuse reflective polarizer, co...~ ;..g the steps of: providing a first resin, whose degree of birefrin~nre can be altered by application of a force field, WO 97132230 PCT/US97/03l30 as through dimensional orientation or an applied electric field, such that the resulting resin material has, for at least two orthogonal directions, an index of refraction difference of more than about 0.05; providing a second resin, dispersed within the first resin; and applying said force field to the composite of both resins s such that the indices of the two resins are ~ o~imately m~t~.he~l to within less than about 0.05 in one of t~,vo directions, and the index difference between first and second resins in the other of t~,vo directions is greater than about 0.05. In a related embodiment, the second resin is dispersed in the first resin after imposition of the force field and subsequent alteration of the birefringence of the first resin.
o In yet another aspect, the present invention relates to an optical body acting as a reflective polarizer with a high e~tinf tion ratio. In this aspect, the index difference in the match direction is chosen as small as possible and the diLl~,,e.~ce in the mi~;ms~tf~h direction is ..,~x;.,.;,~(l The volume ~rtior~, thiel~nes~, and disperse phase particle size and shape can be chosen to ...s.x;,..;~ the e~rtin- ti~n 5 ratio, although the relative hl~o~ ce of optical tr~n~mi~ion and reflection for the dil~el~llL pol~ri7s/ti~ns may vary for dirr~ applications.
In another aspect, the present invention relates to an optical body c--mpri~ing a cor~tinllons phase, a rli~p~or~e phase whose index of refraction differs from said continuous phase by greater than about 0.05 along a first axis and by less 20 than about 0.05 along a second axis orthogonal to said first axis, and a dichroic dye. The optical body is ~l~r, .~bly oriented along at least one axis. The dichroic dye improves the extinction coefficiçnt of the optical body by absorbing, in addition to S~ ;..g, light polarized parallel to the axis of orient~tion.
In another aspect of the present invention, an optical body is provided 2s which has at least first and second phases that are co-contin~ous along at least one axis. The index of refraction of the first phase differs from that of the second phase by greater than about 0.05 along a first axis and by less than about 0.05 along a second axis orthogonal to said first axis. In other embo~liment~, three or more co-continuous phases may be used to achieve the same or similar m~tf hes and 30 mi~m~tch~s along mlltn~lly perpendicular axes.

In still another aspect of the present invention, an optical body is provided which comprises a film having a continuous and disperse phase, with an antireflective layer disposed thereon. Such films exhibit a flat tr~ncmieeion curve as a function of the wavelength of light, which tends to m;nimi7~ any rh~nge~ ins color to a r~snlt~nt display device into which the reflective polarizer is incull,oldLcd.
In the various aspects of the present invention, the reflection and L~ - iq~ion properties for at least two orthogonal polarizations of incident light are ~lçtPrminPri by the selection or manipulation of various p;~ ctPr~e~ including o the optical indices of the c~)ntinnc)us and disperse phases, the size and shape of the disperse phase particles, the volume fraction of the lis~e~se phase, the thict~nP~s of the optical body through which some fr~ction of the inr,ident light is to pass, and the wavelength or wavcle~ Lh band of electrom~nPtic r~ tion of interest.
The m~gni~ldç ofthe index match or miem~t~h along a particu~ar axis will 15 directly affect the degree of sc~ of light polarized along that axis. In general, sr7~ power varies ~ the square of the index ~ "I,.I~h Thus, the larger the index .,li~.,l, Icl~ along a particular axis, the stronger the sc;~ of light polarized along that axis. Conversely, when the miem~trh along a particular axis is small,light polarized along that axis is sc~ d to a lesser extent and is thereby 20 ~ specularly through the volurne of the body.
The size of the ~liepPree phase also can have a eignifiç~nt effect on sc .1~ If the dis~ ph~e particles are too small (i.e., less than about 1/30 the wavelength of light in the ~~e~ of interest) and if there are many particlesper cubic wavel~n~h, the optical body behaves as a mP~ m with an effective 2s index of refraction somewhat bcLwcell the indices of the two phases along anygiven axis. In such a case, very little light is sc~LLeled~ If the particles are too large, the light is specnl~r1y reflectPrI from the particle sllrf~rç, with very little diffilsion into other directione When the particles are too large in at least two orthogonal directions, undesirable iri~lPsc.once effects can also occur. Practical 30 lirnits may also be reached when particles become large in that the thickness of the optical body becomes greater and desirable mechanical ~rop~Lies are CO~ )lolllised.
The shape of the particles of the disperse phase can also have an effect on the scattering of light. The depolarization factors of the particles for the elech~ic s field in the index of refraction match and mi.cm~t-~h directions can reduce or enhance the amount of ~r~ Ig in a given direction. The effect can either add or detract from the amount of sc~L~ g from the index mi~m~tch, but gent?r~lly has asmall influence on sc ~hterinP in the plerel.ed range of plO~. lies in the present invention.
0 The shape of the particles can also inflnence the degree of diffusion of light scattered from the particles. This shape effect is generally small but hlcl~ases as the aspect ratio of the geomptric~l cross-section of the particle in the plane e~..l;c~ r to the direction of incidence of the light increases and as the particles get relatively larger. In general, in the operation of this invention, the disperse 5 phase particles should be sized less than several wavelengthe of light in one or two mnhl~lly orthogonal ~;nnen~iOnS if diffuse, rather than specular, rçflection is plcfe.l~d.
~ imenci- nz~ nnn~nt is also found to have an effect on the seS~ -g behavior of the di:i~CI ~e phase. In particular, it has been observed, in optical 20 bodies made in accordance with the present invention, that aligned scatterers will not scatter light syrnmPtric~lly about the directions of specular tr~ncmi~ion orreflection as randomly aligned scatterers would. In particular, inclll~ion!~ that have been elongated by ori~nt~ti~n to resemble rods scatter light prim~rily along (ornear) a cone centered on the ~ l ;on direction and having an edge along the 2s specularly ~ ",;lle-1 direction. For example, for light in~ nt on such an elongated rod in a direction perpendicular to the orientation direction, the scahtered light appears as a band of light in the plane perpendicular to the orientation direction with an hlLell~iLy that decreases with increasing angle away from the spec~ r directions. By tdiloring the geometry of the inclll~ion~, some control over 30 the distribution of scdL~ d light can be achieved both in the tr~n~mi~ive hemi~phere and in the reflective hemi~pht?re.

The volume fraction of the disperse phase also affects the s~ ; r-g of light in the optical bodies of the present invention. Within certain limits, increasing the volurne fraction of the disperse phase tends to increase the amount of sc~ ring that a light ray expçrien~,e after entering the body for both the match and s miems-f~h directions of polarized light. This factor is hllpulL~lL for controlling the reflection and tr~nemieeion ~l u~ ies for a given application. However, if the volume fraction of the di~ e phase becomes too large, light sc~ g f~iminiehe$ Without wishing to be bound by theory, this appears to be due to thefact that the disperse phase particles are closer together, in terms of the wavelength o of light, so that the particles tend to act together as a smaller null~b~,. of large effective particles.
The thickn-oee of the optical body is also an illl~Ul L~L control parameter which can be manipulated to affect reflection and ~ ie~ion ~ropelLies in the present invention. As the thir~neee of the optical body iL.,l~a3es, diffuse reflection 15 also illcleases, and tranemieeion~ both specular and diffilse, dec ~ases.
While the present invention will o~ten be described herein with reference to the visible region of the ~e-;h.ull, various embo-lim~nte of the present invention can be used to operate at L~ wavel~ngthe (and thus L~ ,ies) of cle~ n~tic radiation through ~L)~G~ e scaling of the c~ lpolle~lLs of the 20 optical body. Thus, as the wavelength increases, the linear size of the components of the optical body are increased so that the ~iimeneions, measured in units of wavelength, remain a~l!loxlmately con~ . Another major effect of ch~nginf~
wavelength is that, for most m~tPri~le of interest, the index of refraction and the absorption coefficient change. However, the principles of index match and 25 miem~t- h still apply at each wavelength of interest.

Detailed De i~ion of the I v~ -As used herein, the terms "specular reflection" and "specular reflect~nre"
30 refer to the reflect~nr,e of light rays into an emergent cone with a vertex angle of 16 degrees centered around the specular angle. The terms "diffuse reflection" or "diffuse reflect~nre" refer to the reflection of rays that are outside the specular cone defined above. The terms "total reflectance" or "total reflection" refer to the combined reflect~nce of all light from a surface. Thus, total reflection is the sum of specular and diffuse reflection.
Similarly, the terms "specular tr~n~mi~cion" and "specular tr~ncmitt~n- e"
are used herein in lcfere~ce to the tr~ncmiccion of rays into an emergent cone ~,vith a vertex angle of 16 degrees centered around the specular direction. The terms "diffuse tr~nemiccjon" and "diffuse l~ ..ce" are used herein in reference to the tr~n.cmi.cci~n of a~l rays that are outside the specnl~r cone defined above. The 0 tenns "total tr~ncmi~cion77 or "total l~ "ce" refer to the combined tr~ncmiccion of all light through an optical body. Thus, total tr~ncmic.~ion is the sum of specular and diffuse tr~ncmiceion As used herein, the term "extinction ratio" is defined to mean the ratio of total light l . i~ 1 in one polarization to the light ll ~ d in an orthogonal pol ~ri~7~tion FIGS. 1-2 illllet~fç a first embo~limpnt of the present invention. In accol~u~ce with the invention, a dirrusely reflective optical film 10 or other optical body is produced which consists of a biremn~nt matrix or continuous phase 12 and a discu.ltilluuus or ~ e phase 14. The birefringence of the contin-lnus phase is typically at least about 0.05, preferably at least about 0.1, more preferably at least about 0.15, and most preferably at least about 0.2.
The indices of rPt;~ction ofthe contiml~us and ~lieptqrse phases are snhst~nti~lly m~t ~hecl (i.e., differ by less than about 0.05~ along a first of three mlltll~lly orthogonal axes, and are ~ bt~ lly mi~m~teh~-1 (i.e., differ by more than about 0.05~ along a second of three mllt~l~lly orthogonal axes. Preferably, the indices of refraction of the continuous and disperse phases differ by less than about 0.03 in the match direction, more preferably, less than about 0.02, and most preferably, less than about 0.01. The indices of refraction of the continuous and rPr~e phases p.~ir~ly differ in the mi~m~tc~h direction by at least about 0.07, 30 more preferably, by at least about 0.1, and most ~ r~ably, by at least about 0.2.

The micm~trh in refractive indices alon_ a p~ticiilar axis has ule effect t;l~t incident light polarized along that axis will be substantially scaKered, resulting in a significant arnount of reflection. By contrast, incident light polarized along an axis in which the refracti~e indices are matched v.ill be spectrall~; transmitted or reflected with a much lesser degree of scaKering. This ef~ect can be utilized tomake a variety of optical devices, including refiective polarizers and mirrors.
The present invention provides a practical and simple optical body and method for ma~cing a reflective polarizer, and also provides a means of obtaining a continùous range of optical properties according to the principles described herein.
lo Also, very efficient low loss polarizers can be obtained with high extinction ratios. .-Other advantages are a wide range of practical materials for the disperse phase and r the continuous phase, and a high degree of control in providing optical bodies of consistent and predictable high quality perfo.,~ se ~ Z Q ~
Effect of Index Match/~uicln~t~h In the p.efe.l~1 embodiment, the materials of at least one of the continuous and disperse phases are of a type that undergoes a change in refractive index upon orientation. Consequently, as the film is oriented in one or more directions, refractive index matches or mi~m~rhes are produced along one or more axes. By careful manipulation of o;ientation pararneters and other pr~cessing conditions, the positive or negative birefringence of the matrix can be used to induce diffuse reflection or tr~ncmicsion of one or botn polarizations of light along a given axis.
J The relative ratio ~l~.~,e~ tr~ncmicsion and diffuse reflection is ~lep-~n~l~nt on the Col~rP ~ 1 ;on of the disperse phase inclusions, the thickness of the filrn, the square of the difference in the index of refraction b~ the corltinl1ous and disperse phases, the size and geometry of the disper_e phase inclusions, an~ the wavelengt'n or wavelength band of the incident radiation.
The magnitude of the index match or micm~t~h along a particular axis directly affects the de~ree of sca~ hlg of light polarized along that axis. In general, scattering power varies as the square of the index micm~tch Thus, the larger the index micm~tch along a particular axis, the stronger the scau~.Lng of AMENI:)ED S~T

CA 02246~4~ 1998-08-17 12a In an inventive device comprising an inven~ive optical film or optical body at least about 5 to 70~ o, light of a first polarlzation ls difIusely extracted.
The continuous phase or flrst phase 12 can be comprised of a thermoplastic resin. It can be a copolymer of at least one diol and a monomer selected from the group consisting of naphthalene dicarboxylic acid, isophthalic acid, dimethyl isophthalic acid, terephthalic acid and dimethyl terephthalic acid.
The discontinuous or disperse phase or second phase 14 can comprise a plurality of elongated masses whose major axes are substantially aligned along a common axis.
The optical body as an extractor can be stretched in at least one direction, wherein at least about 40~ of light of a first polarization is diffusely transmitted through said optical body (10), and wherein said diffusely transmitted rays are distributed primarily along or near the surface of a cone whose surface contains the spectrally transmitted direction and whose axis is centred on the stretch direction.
Furthermore, an optical body usable as an elliptical polariser is provided wherein the absolute value of the difference in index of refraction of said first and second phases is ~ n1 along a first axis and ~ n2 along a second axis orthogonal to sa~d first axis, wherein the absolute value of the difference between ~ nl and~n2 is at least about 0.05, and wherein the diffuse reflectivity of said first and second phases ta~en together along at least one axis for at least one polarization of electromagnetic radiation is at least about 30%.
J In this connection, the absolute value of the difference between ~n1 and ~n2 is at least about 0.1.
The first phase 12 can be a larger birefringence than the second phase (14) wherein the birefringence of the first phase is at least 0.02 greater than the birefringence of the second phase (14).
The optical body can also consist of a plurality of layers (20), wherein at least one of said layers comprises a first phase having a birefringence of at least about 0.05 and a second phase wh-ch is discontinuous along at least two of any th-ee mutua ~y orthogonal axes.

A~ nED S~l~

light polarized along that axis. Conversely, when the mi.~m~tch along a particular axis is small, light polarized along that axis is scattered to a lesser extent and is thereby Ll, ...~.",i(~ed specularly through the volurne ofthe body.
FIGS. 4a-b demonstrate this effect in oriented films made in accordance 5 with the present invention. There, a typical Bidirectional Scatter Distribution - Function (BSDF) measurement is shown for norrnally inri-lrnt light at 632.8 nrn.
The BSDF is described in J. Stover, "Optical Sc~ttering Me~u~ lll and Analysis" (1990). The BSDF is shown as a function of scattered angle for polarizations of light both perpendicular and parallel to the axis of orientation. A
o sc~ .ed angle of zero colre,~onds to 11n~c~ red (spectrally 1.,-..c.,.ill~d) light.
For light polarized in the index match direction (that is, perp~nrlic111~r to the orient~tion direction) as in FIG. 4a, there is a ~i~nifir~nt specularly L~ Lcd peak with a sizable colll~ol~lll of diffusely ll~ ;L~ed light (s~ ing angle b~lwccll 8 and 80 degrees), and a small component of diffusely reflçctrd light 15 (sc~ g angle larger than 100 degrees). For light polarized in the index 1rh direction (that is, parallel to the orirnt~tion direction) as in FIG. 4b, tnere is n~g1iEihle specul~rly ~ rd light and a greatly reduced colll~olle~lL of diffusely 1.,...~..li~t~cl light, and a sizable di~usely reflecte~t con~vll~,~L It should be noted that the plane of sc~ , ;llg shown by these graphs is the plane 20 perpendicular to the n- ~ nl ;on direction where most of the sc~Ll~d light exists for these elongated inclusions. Sc~ lcd light contributions outside of this plane are greatly reduced.
If the index of refraction of the inr~ ions (i.e., the ~ p~rse phase) ms~trhrs that of the collLillu~>us host media along some axis, then incid~nt light polarized 25 with electric fields parallel to this axis will pass lh~oll~h ~ cnll- .cd regardless of the size, shape, and density of inclusions. If the indices are not m~t ~ed alongsome axis, then the inclusions will scatter light polarized along this axis. ForSC~:IL~cl:~ of a given cross-sectional area with ~1im~n~jons larger than a~loxhllaLely ~/30 ( where ~ is the wavelength of light in the media), the strength 30 of the sc~cling is largely det~rminrd by the index mi~m~tc1~ The exact size, shape and ~1i nmrnt of a mi~m~trhr~ inclusion play a role in ~~ ;llp how much light will be scattered into various directions from that inclusion. If thedensity and thickness of the sc~ttering layer is sli-mcient, according to multiple sc~ttering theory, incident light will be either reflected or absorbed, but not tr~nemittt-A, regardless of the details of the scatterer size and shape.
s When the m~t.ori~l is to be used as a polarizer, it is preferably processed, as by stretching and allowing some flimenei~nal relaxation in the cross stretch in-plane direction, so that the index of refraction diLre.bnce between the co~tin-lous and disperse phases is large along a first axis in a plane parallel to a surface of the material and small along the other two orthogonal axes. This results in a large optical anisokopy for elecL,~ gnPtic radiation of ~lirr~ cllL pol~ri7~tiollc Some of the polarizers within the scope of the present invention are elliptical pol~ri7Prs In general, elliptical polarizers will have a difference in index of refraction be~ ,n the rliQ~P~rse phase and the continuous phase for both the stretch and cross-stretch directions. The ratio of r~l ~d to back sc~Lhl;ng is as fi~pP~ nt on the diLL~ l~nce in l~fi~siLiv~ index belw~ell the ~iicpprce and continuous phases, the con~ G~ n of the r1icpPrce phase, the si_e and shape of the ~ p~P-rse phase, and the overall thi~ nP~c of the film. In general, elliptical ~liffilcPr~c have a relatively small difference in index of refr~cti~ r- b~l~J~ the particles ofthe ~licpprse and continuous phases. By using a bh~r ;-.gr. l polymer-based ~limlc~r, highly elliptical polari_ation sensitivity (i.e., diffuse reflectivity depending on the pol~ri7~tion of light~ can be achieved. At an ~L~ lC, where theindex of refraction of the polymers match on one axis, the ellipt~ polarizer will be a diffuse reflecting polarizer.

2s Methods of Obtaining Index Match/l~liQ~~ ' The materials selected for use in a polarizer in accordance with the present invention, and the degree of oriellt~tion ofthese ~t~ri~lc~ are preferably chosen so that the phases in the fini~he-l polarizer have at least one axis for which the associated indices of refraction are sllbst~nti~lly equal. The match of refractive indices associated with that axis, which typically, but not .~ce~.;ly, is an axis -a4-transverse to the direction of orientation, results in substantially no reflection of light in that plane of polarization.
The disperse phase may also exhibit a decrease in the refractive index associated with the direction of orientation after stretching. If the birefringence of s the host is positive, a negative strain in~1ure(1 birefringence of the disperse phase has the advantage of increasing the difference between indices of refraction of the adjoining phases associated with the orient~tion axis while the reflection of light with its plane of polarization perpçnrlic~ r to the orientation direction is still n~gligible. Differences bclvv~ell the indices of refraction of adjoining phases in the 1 o direction orthogonal to the o~;c.llalion direction should be less than about 0.05 after orientation, and ~.~.cLbly, less than about 0.02.
The di:j~c.~e phase may also exhibit a posiLive strain inr1llred birefrin~enre However, this can be altered by means of heat tre~tment to match the refractive index of the axis ~ ;1l licular to the onent~tiC)n direction of the continuous phase.
5 The tt;lll~ .a~ of the heat tre~tm~ont should not be so high as to relax the birefi ingence in the continllous phase.

Size of D~ Phase The size of the ~iicpf-rse phase also can have a signific~nt effect on 20 scS~ ..g If the d~c;lse phase particles are too small (i.e., less than about 1/30 the wavelength of light in the m--Aillm of interest3 and if there are many particles per cubic wavele~gth, the optical body behaves as a m.o~lillm with an effective index of refi~c tion sOll.~ vvh~l bcLwccll the indices of the two phases along any given axis. In such a case, very little light is sc~lh .ed. If the particles are too 25 large, the light is specularly reflected from the surface of the particle, with very little diffusion into other directions. When the particles are too large in at least two orthogonal directions, nn-i~cir~ble inde~c~.lce effects can also occur. Practical limits may also be reached when particles become large in that the thickness of the opticalbody becomesgreateranddesirable ,n.?rh~l~ic~ iesare 30 colll~lolllised.

_15_ The flimen~ions of the particles of the disperse phase after ~lignment can vary depending on the desired use of the optical mz~teri~l Thus, for example, the ~limencions of the particles may vary depending on the wavelength of electrom~gnPtic radiation that is of interest in a particular application, with s different ~lim~n~ions required for reflecting or tr~n~milting visible, ultraviolet, infrared, and _icrowave radiation. Generally, however, the length of the particles should be such that they are approximately greater than the wavelength of electromagnetic radiation of interest in the medium, divided by 30.
Pl~ f~,.~ly, in applications where the optical body is to be used as a low o loss reflective polarizer, the particles will have a length that is greater than about 2 tirnes the wavelength of the cle~ h-,-n~gn~tic r~ tion over the wavelength range of interest, and preferably over 4 times the vvavel~n~th The average ~ met~?r of the particles is preferably equal or less than the wavelength of the electrom~gnçticradiation over the wavelength range of interest, and preferably less than 0.5 of the 5 desired wavel~on th While the riim~n~iQIl~ of the disperse phase are a seco~
c~-n~i(ler~tion in most applications, they become of greater hll~olL~ce in thin film applications, where there is c.~ p~ ely little diffuse reflçctinn Geometly of D..,l._, ~ L Phase While the index mi~m~tf h is the pred~ .,1 factor relied upon to promote sc~ in the films of the present invention (i.e., a diffuse mirror or polalizer made in acco~d;~lce with the present invention has a s~-bst~nti~l mi~m~t~h in the indices of refraction of the continuous and .li~p. ~se phases along at least one axis), the geometry of the particles of the disperse phase can have a secondary effect on S~ g. Thus, the depolarization factors of the particles for the electric field in the index of r~ction match and mi.~m~h directions can reduce or enhance the arnount of sc~ nn~ in a given direction. For eY~mrl~, when the disperse phase iselliptical in a cross-section taken along a plane perpendicular to the axis of olic.lk~Lion, the elliptical cross-sectional shape of the disperse phase contributes to the asymmetric diffusion in both back scattered light and f~l ~v~.l scattered light.
The effect can either add or detract from the amount of sr~tt~rin~ from the index wo 97/32230 PCT/USg7/03130 micm~tf~h, but generally has a small influence on scattering in the preferred range of properties in the present invention.
The shape of the disperse phase particles can also influence the degree of diffusion of light scattered from the particles. This shape effect is generally small 5 but increases as the aspect ratio of the geometrical cross-section of the particle in the plane perpendicular to the direction of ineici~nee of the light increases and as the particles get relatively larger. In general, in the operation of this invention, the disperse phase particles should be sized less than several wavelengths of light in one or two mlltn~lly orthogonal iimçncions if diffuse, rather than specular, 0 reflection is l~cr~ ;d.
Plcr~.dl)ly, for a low loss reflective polarizer, the ~ r~cd embodiment consists of a iicperse phase disposed within the continuous phase as a series ofrod-like structures which, as a conse-luence of orient~tion, have a high aspect ratio which can enhance reflection for polarizations parallel to the orientation direction 5 by increasing the sc~ strength and ~ii.cper,cion for that polarization relative to po1~ri7~tinnc perp~nriic~ r to the orientation direction. However, as in ~ tçd in FIGS. 3a-e, the disperse phase may be provided with many different gen, . .e! I ;es Thus, the disperse phase may be disk-shaped or ei~mg~t~d disk-shaped, as in FIGS.
3a-c, rod-shaped, as in FIG. 3d-e, or sph~ic~l Other embo~l;.... ~l~; are 20 co~ .,pl~t~cl wh~ the rlicp~rse phase has cross sections which are ~roxi~ cly elliptical (inr.lll~ling circular), polygonal, irregular, or a combination of one or more of these shapes. The cross-sectional shape and size of the particles of the disperse phase may also vary from one particle to another, or from one region of the film to another (i.e., from the surface to the core).
In some embo~li"~ i, the di~cl~e phase may have a core and shell coll:iL..l~;Lion, wh~ hl the core and shell are made out of the same or difrcl~
m~tPri~lc, or wh~,.c;ll the core is hollow. Thus, for e~r~mrle, the disperse phase may consist of hollow fibers of equal or random length~, and of ulPiro~ or non-Ullifc,llll cross section. The interior space of the fibers may be empty, or may be - 30 occupied by a suitable mediurn which may be a solid, liquid, or gas, and may be organic or hlOl~al~iC. The refractive index of the medium may be chosen in consideration of the refractive indices of the disperse phase and the continuousphase so as to achieve a desired optical effect (i.e., reflection or polarization along a given axis~.
The geometry of the disperse phase may be arFived at through suitable s orientation or procç~ing of the optical m~t~ri~l, through the use of particles having a particular geometry, or through a combination of the two. Thus, for example, adisperse phase having a substAnti~11y rod-like structure can be produced by o~ien~in~ a film con~i~ting of ~ oxi~ t~iy spherical disperse phase particles along a single axis. The rod-like structures can be given an elliptical cross-section 0 by ~rient;ng the film in a second direction perpendicular to the first. As a further example, a disperse phase having a s17hstAntiAlly rod-like structure in which the rods are rect.7ng711~r in cross-section can be produced by orienting in a singledirection a filrn having a ~ e phase co~ of a series of e~nti~711y ular flakes.
SLI~ g is one convenient ma7mer for a7Tiving at a desired geometry, since ~lletcllil-g can also be used to induce a diLr ~c..ce in indices of rÇ~ctiQn within the m~t~riA1 As inrli~At~fl above, the orientation of films in accordance with the invention may be in more than one direction, and may be sequential or .cimll1tAneous.
In another example, the co~ ol~llL~ of the continuous and disperse phases may be extruded such that the di~ ..,e phase is rod-like in one axis in the ~mnrient~ film. Rods with a high aspect ratio may be g~--f .,.~,1 by orienting in the direction of the major axis of the rods in the extruded film. Plate-like structures may be gen~l dLed by ~ . "; l ,~v in an orthogonal direction to the major axis of the 25 rods in the extruded film.
Ihe 7L1U~;LUI~, in FIG. 2 can be produced by asyn~netric biaxial orientation of a blend of e ~?ntiA11y spherical particles within a cont~nuous matrix.
~ltf rn~tively, the structure may be obtained by hlcol~Gldlillg a plurality of fibrous structures into the matrix m~teriA1, A1ipning the structures along a single axis, and 30 oriçntin~ the 111iXLU~C in a direction Lld~ l.,e to that axis. Still another method for obtaining this structure is by controlling the relative vi~cositiçs, shear, or surface tension of the components of a polymer blend so as to give rise to a fibrous disperse phase when the blend is extruded into a film. In general, it is found that the best results are obtained when the shear is applied in the direction of extrusion.

5 D- - ~ional Alignment of Disperse Phase Dimensional ~71ignm~nt is also found to have an effect on the sc~ g behavior of the ~7i~perse phase. In particular, it has been observed in optical bodies made in accordance with the present invention that aligned sc~Ll~,rc~ will not scatter light symmetrically about the directions of specular ll,~ ion or 10 reflection as randomly aligned scaLL~ would. In particular, inclusions that have been elqngs7te~1 through orientS7tiQn to resemble rods scatter light rrims7rily along ~or near) the surface of a cone e~lLt;lLil on the orientS7tion direction and along the specn1S7r1y h~ ec~ direction. This may result in an anisotropic distribution of scall~ d light about the spec171Slr reflection and specular l . ~ ;on directions.
15 For example, for light in~ lent on such an elongated rod in a direction perpenr1iruls7r to the ~1- ;G. . ~ ~l ;f n direction, the sc~ cd light appears as a band of light in the plane p~ licular to the orient~til~n direction with an intensity that declG~ses with h~~ ~ angle away from the specular directions. By tailoring the geometry of the inclusions, some control over the distribution of sc~lLGled light can 20 be achieved both in the L1~ ;VG h~mi~phere and in the reflective h~mieph~re.

D - - of Dii,~ r e Phase ln applications where the optical body is to be used as a low loss reflective polari7er, the structures of the disperse phase ~,ere~ably have a high aspect ratio, 25 i.e., the structures are ~ub ~ is711y larger in one ~li...P..~;on than in any other .7imen~ion. The aspect ratio is ~l~,r~lably at least 2, and more preferably at least 5.
The largest ~7im~?n~ion (i.e., the length) is preferably at least 2 times the wavelength of the electromS~gnetic radiation over the wavelength range of interest, and more preferably at least 4 times the desired wavelength. On the other hand, the smaller 30 (i.e., cross-sectional) ~im~n~ions of the :,L- ~u;Lules of the disperse phase are , CA 02246545 l99X-08-17 preferably less than or equal to the wavelength of interest, and more preferably less than û.5 times the wavelength of interest.

Volume ~raction of Disperse Phase The volume fraction of the disperse phase also affects the sc~ r;~-~ of light in the optical bodies of the present invention. Within certain limits, increasing the volurne fraction of the disperse phase tends to increase the amount of sc~LLL~ gthat a light ray expt~rirnr~c after entering the body for both the match and mi~m~trh directions of polanzed light. This factor is illl~ol~l for controlling the 0 refl~cti~m and tr~ncmicei~n properties for a given application.
The desired volume fraction of the di~, ,c phase will depend on many factors, including the specific choice of m~teri~lc for the co~tinnl-us and disperse phase. However, the volurne fraction of the disperse phase will typically be at least about 1% by volume relative to the continuous phace, more preferably within the range of about 5 to about 15%, and most preferably within the range of about 15 to about 3~%.

Co-C~c ~. - Phases When the volume fraction for binary blends of high polymers of roughly 20 equivalent viscosity approaches 50%, the ~1ictinrtion bcl~,n the ~licperce and co..l;....ous phases becom~s difficult, as each phase becomes continuous in space.
Depending upon the ms~trri~l~ of choice, there may also be regions where the first phase appears to be dispersed within the second, and vice versa. For a description of a variety of co-co~ luous morphologies and for methods of ev~ tin~, analyzing, and rh~r~rt~ri~ing them, see Sperling and the references cited therein (L.H. Sperling, "Mic~ hase Structure", Encyclopedia of Polymer Science and En~ineerin~. 2nd Ed., Vol. 9, 760-788, and L.H. Sperling, Chapter I
~ L~L~.,l,ctrating Polymer Networks: An Overview"~ Interpenetratin Polymer Networks, edited by D. Kl~mpn~r, L.~I. Sperling, and L.A. Utracki, Advances in - 30 Chemist~y Series #239, 3-38, 1994).

_ Materials having co-contin~ us phases may be made in accordance with the present invention by a nurnber of different methods. Thus, for example, the polymeric first phase m~t~ri~l may be mechanically blended with the polymeric second phase mz~t~ri~l to achieve a co-continuous system. Examples of co-continuous morphologies achieved by blending are described, for example, in D.
Bourry and B.D. Favis, "Co-Continuity and Phase Inversion in HDPE/PS Blends:
The Role of Interfacial Modification", 1995 Annual Technical Conference of the Societv of Plastics F.n~in~.~?rs ANTEC. Vol. 53, No. 2, 2001-2009 (poly~Ly~ e/polyethylene blends), and in A. Leclair and B.D. Favis, "The role ofo ;-1l. . r~ci~l contact in immi~r;~le binary polymer blends and its infl~lenre on merh~nic~l u~c uel~ies", PolYmer. Vol. 37, No. 21, 4723-4728, 1996 (polycarbonatelpolyethylene blends~.
Co-continuous phases may also be formed in accordance with the present invention by first by dissolving them out of ~uyt:l~;lilical fluid extractions, such as that disclosed for blends of poly~lyl~lle and poly(methyl m~ll.A~ late) in U.S.
4,281,084, and then allowing them to phase ~u;~ following exposure to heat and/or m~rh~ni~l shear, as described by in N. ~el~hilef, B.D. Favis and P.J.
Carreau, "Morphological Stability of Poly~lyl~,ne Polyethylene Blends", 1995 Annual Technical Conference of the Society of Plastics Fn~in~ers ANTEC. Vol.
53, No. 2, 1572-1579).
A further method of producing co-continl-c us ph~ses in accordance with the present invention is through the creation of illL~ aLillg polymer networks (IPNs). Some of the more important IPNs include ~imlllt~n~ous IPNs, sequential IPNs, gr~qAi~nt IPNs, latex IPNs, thermoplastic IPNs, and semi-IPNs. These and other types of IPNs, their physical urope~lies (e.g., phase ~ m.c), and methods for their ~ ~alion and ch~r~ ;nn, are described, for ç~z~mple, in L.H.
Sperling and V. Mishra, "Current Status of Inl.,~ d~ Polymer Networks", Polvmers for Advanced Technolo~ies. Vol. 7, No. 4, 197-208, April 1996, and in L.H. Sperling, "Il1tel uelletrating Polymer Networks: An Overview", - 30 ~ e~Ue11Cl~A~ Polymer Networks. edited by D. Klempner, L.H. Sperling, and WO 97/32230 PCT/USg7/03130 L.A. Utracki, Advances in Chemistry Series #239, 3-38, 1994). Some of the major methods for ~ ~hlg these systems are ~ i below.
Simnlt~neous IPNs may be made by mixing together the respective monomers or prepolymers, plus the crosslinkers and activators, of two or more s polymer networks. The respective monomers or prepolymers are then reacted .~imnlt~neously, but in a non-illle f~.hlg manner. Thus, for ex~mple, one reaction may be made to proceed by way of chain polymeri7~fion kin~tics, and the other reaction may be made to proceed through step poly . . ~ i ion kinetics.
Sequential IPNs are made by first forming an initial polymer network.
lo Then, the monomers, cro~s~linker~ and a~;livaLol~ of one or more ;~ iitinn~l nGLw~ are swollen into the initial polymer net~,vork, where they are reacted in situ to yield ~ iitionz~i polymer networks.
Gradient IPNs are sy.~ i in such a ~ that the overall composition or crosslink density of the IPN varies macroscopically in the mzlt~ris~l 5 from one location to another. Such ~y:,Leuls may be made, for example, by forming a fLrst polymer network prerlo~ y on one surface of a film and a second polymer ncLwulk preci~....;..~..lly on another surface of the film, with a ~radient in composition Ih~ou~hout the interior of the film.
Latex IPNs are made in the form of latexes (e.g., with a core and shell 20 ~LLU~LU1G). In some v~ri~ti~)ne~ two or more latexes may be mixed and formed into a film, which clos~ ks the polymers.
I'hermopl~tic IPNs are hybrids bGL~ polymer blends and IPNs that involve physical crosslinks instead of ~h-?mi~ l cro~link~. As a result, these m~t~ri~l~ can be made to flow at elevated le~ GS in a manner similar to that2s of Lh~,~,llo~lastic ç~ o~ but are cros~linkçl1 and behave as IPNs at the t~ )c~dLu.~,s of normal use.
Semi-IPNs are compositions of two or more polymers in which one or more of the polymers are cro~link~l and one or more of the polymers are linear or br~nch~i As inc1ics~tf~1 above, co-cv.. l;.. ~iLy can be achieved in multicomponent systems as well as in binary systems. For example, three or more m~tt?ri~ may be CA 02246545 l998-08-l7 used in combination to give desired optical ~lop~.lies (e.g., tr~n~mie~ion and reflectivity) and/or improved physical ~lop~.Lies. All components may be imrniscible, or two or more components may dem~ Ll~lc miscibility. A number of ternary systems exhibiting co-cc-ntin-lity are described, ~or example, in L.H.
5 Sperling, Chapter 1 "Interpcl.cLldLhlg Polymer Networks: An Overview", Interpenetratin~ Pol~ner Networks, edited by D. ~lemr~-r, L.H. Sperling, and L.A. Utracki, Advances in Chemistry Series ~239, 3-38, 1994).
~ h~r~L~teri~tic sizes of the phase structures, ranges of volume fraction over which Co-ccJ~ uiLy may be observed, and stability of the morphology may all be 0 i~ ..L e-l by additives, such as co~ ;hilizers, graft or block copolymers, or rcacLivc co",l-o-lL~nt~, such as maleic anhydride or glycidyl ...~ L ~ylate. Such effects are described, for example, for blends of poly~Lyl~.le and poly(ethyleneterephth~l~tL~) in H.Y. Tsai and K. Min, "Reactive Blends of Functinnzlli7ecl Poly~lyl~e and Polyethylene Terephth~l~te", 1995 Annual Technical Conr~cllce ofthe Societv of Plastics F.l,~;,.r~ .~i AN~C. Vol. 53, No. 2, 1858-1865.
However, for particular :jy~ ms, phase L~i~m~ may be col~Llu.;Lcd through routine L ~ ;"~ ;on and used to produce co-continuous ~y~LL,llls in accordance with the present invention.
The microscopic :iLlLtc~ul~, of co-continuous systems made in accu,-l~lce 20 with the present invention can vary significantly, depending on the method ofP~ l ion, the mi~ci~ility of the phases, the plesc"ce of additives, and other factors as are known to the art. Thus, for L~mple one or more of the phases in the co-continuous system may be fibrillar, with the fibers either randomly orientL-~l or oriented along a common axis. Other co-continl~ous systems may CL ...p. ;~e an 25 open-celled matrix of a first phase, with a second phase disposed in a co-c~ ous ,,,al~ucl within the cells of the matrix. The phases in these systems maybe co-continuous along a single axis, along two axes, or along three axes.
Optical bodies made in accoldallce with the present invention and having co-continuous phases (particularly IPNs~ will, in several inet~nres, have pl~ Lies 30 that are adv~nt~eous over the ~lo~clLies of similar optical bodies that are made with only a single continuous phase, dep~n~ling, of course, on the pl~ . Lies of the individual polymers and the method by which they are combined. Thus, for example, the co-continuous systems of the present invention allow for the chrmirsll and physical combination of structurally flieeimik7r polymers, thereby providing a convenient route by which the properties of the optical body may be modified to S meet specific needs. Fu~LL~ ore, co-continuous systems will frequently be easier to process, and may impart such ~-,u~c~Lies as weatherability, reduced fl~7mm~7bility, greater impact resistance and tensile strength, improved flexibility, and superior rh~nnic~l reCiet~7nre IPNs are particularly advantageous in certainapplications, since they typically swell (but do not dissolve) in solvents, and 0 exhibit ~u~p~cs~ed creep and flow co..l~,uGd to analogous non-IPN ~ ell.s (see, e.g., D. ~lempner and L. Berkowski, "I.lk,~ ;n~ Polymer NcLwo~
EncYclopedia of PolYmer Science and Enei.lcc~ 2nd Ed., Vol. 9, 489-492.
One skilled in the art will ~I-L,Lccialc that the principles of co-continuous systems as are known to tne art may be applied in light of the te~rhin~c set forth 5 herein to produce co-c- n~in-lous morphologies having unique optical l~opc;~ Lies.
Thus, for example, the lc,lia.~ e indices of known co-con1im~ollc morphologies may be manipulated as taught herein to produce new optical films in accol.:la,lce with the present invention. Likewise, the prinriples taught herein may be applied to known optical systems to produce co-continuous morphologies.
2~
T~ q 9 of Optical Body T_e lhicLless of the optical body is also an illl~Oll~lt 1)~11GL~L which can be manipulated to affect reflection and tr~n~miCcinn ~lu~ lies in the present invention. As the ll . ;cl~ s~ of the optical body increases, diffuse reflection also 2s increases, and tr~ncmiccion~ both specnl~r and diffilse, de-,leases. Thus, while ~e thicl~nrcc of the optical body will typically be chosen to achieve a desired degree of mPrh~nic~l strength in the finichr~l product, it can also be used to directly tocontrol reflection and tr~ncmic~inn ~lo~llies Thicl~nrs~ can also be utilized to make final adjustments in reflection and 30 tr~ncmiCcion l.ru~llies of the optical body. Thus, for example, in film applications, the device used to extrude the film can be controlled by a dow.~L~ n optical device which measures tr~n~mi~sion and reflection values in the extrudedfilm, and which varies the thickness of the film (i.e., by adjusting extrusion rates or ch~ngin~2 casting wheel speeds) so as to ".A;~ the reflection and tr~ncmi~ n values within a pre(letermined range.
s ~ Materials for Continuous/D;~ Phases Many different m~terizll~ may be used as the contim~-)Us or disperse phases in the optical bodies of the present invention, depending on the specific application to which the optical body is directed. Such materials include inorganic m~teri~l~
o such as silica-based polymers, organic m~teri~l~ such as liquid crystals, and polymeric m~teri~l~, inc~ in~ monomers, copolymers, grafted polymers, and ixLu~s or blends thereof. The exact choice of m~teri~l~ for a given application will be driven by the desired match and mi~m~t~h obtainable in the refractive indices of the continuous and disperse phases along a particular axis, as well as the 5 desired physical plop~,llies in the re~ ting product. However, the m~t~ri~l~ of the continuous phase will generally be çl~ i by being ~b~l~. ,f ;~lly L~ ellL
in the region of the s~e-;Ll Ulll desired.
A further c->n~id~-r~tion in the choice of m~teri~lc is that the resllltin~
product must contain at least two distinct phases. This may be accomplished by 20 casting the optical m~tf ri~l from two or more m~tf~ri~l~ which are immi~eible with each other. ~Itf~rn~tively~ if it is desired to make an optical m~tf-ri~l with a first and second m~tPri~l which are not immi~cihle with each other, and if the first msltf~ri~l has a higher melting point than the second m~teri~l, in some cases it may be possible to embed particles of a~,plo~ e .l i " ,~ i. ns of the first m:ltf ri~l 2s within a molten matrix of the second m~tf-ri~l at a lt~ cldLulc below the mPlting point of the first m~tf ri~l The rPs -Iting llli~ c; can then be cast into a film, with or without subsecluent orientation, to produce an optical device.
Suitable polymeric m~t~r~ s for use as the contin~ us or f~i~perse phase in the present invention may be amorphous, s~ .ni~ llin~?7 or crystalline polymeric30 m~teri5ll~, incl~fling mz~terizll~ made from monomers based on carboxylic acids such as isophthalic, azelaic, adipic, sebacic, dibenzoic, terephth~lic, 2,7-CA 02246545 l99X-08-17 WO 97t32230 PCT/US97/03130 n~phth~lene dicarboxylic, 2,6-naphth~1~ ne dicarboxylic, cycloh~ x~n~licarboxylic, and bibenzoic acids (including 4,4'-bibenzoic acid), or m~teri53i~ made from thecorresponding esters of the aforementioned acids (i.e., dimethylterephth~ te). Of these, 2,6-polyethylene n~phth~l~te (PEN) is especially ~lGr~ ,d because of its strain inflllce~T birefringence, and because of its ability to remain pL.Il~Al~P~ll]y birefringent after ~L~,;cllLLlg. PEN has a refractive index for polarized incident light of 550 nm wavelength which increases after stretching when the plane of polarization is parallel to the axis of stretch from about 1.64 to as high as about 1.9, while the refractive index decreases for light polarized perpendicular to the axis of 0 stretch. PEN exhibits a birefring~nre (in this case, the difr~ ce bG~ the index of refraction along the stretch direction and the index ~Ll~ ic~ r to the stretch direction) of 0.25 to 0.40 in the visible ~e~LLul.l. The birefringence can be h,~ dsed by increasing the molecular o~ ;on PEN may be sllkst~nti~lly heat stable from about 155~C up to about 230~C, dep~onfling upon the proce~inP
conditions utilized during the m~mlf~rtl~re of the film.
Polybutylene n~rhth~l~t~ is also a suitable m~teri~l as well as other crystalline n~phth~len~ dicarboxylic polyesters. The crystalline ~"1~1.Ll.s~l~n~dicarboxylic polyesters exhibit a di~,lcnce in refractive indices ~sori~te~l with ,.clll in-plane axes of at least 0.05 and plcrc~dbly above 0.2~.
When PEN is used as one phase in the optical m~teri~l of the present invention, the other phase is preferably polylllc~lyh~ th~rrylate (PMMA) or a syndiotactic vinyl aromatic poly-mer such as poly~Ly,c,le ~sPS). Other l.lefc"~,d polymers for use with PEN are based on terephthalic, isorhth~lic7 sebacic, azelaic or cycloh~n~rliç~rboxylic acid or the related aLt~yl esters of these m~t~ris~l~
N~phth~l~n~ dicarboxylic acid may also be employed in minor amounts to improve ~ hl?~inn b~ ;e~l the phases. The diol component may be ethylene glycol or a related diol. Preferably, the index of refraction of the selected polymer is less than about 1.65, and more preferably, less than about 1.55, although a similar result may be obtainable by using a polymer having a higher index of refraction if the satne index dif~erence is achieved.

Syndiotactic-vinyl aromatic polymers useful in the current invention include poly(styrene), poly(alkyl styrene), poly(styrene halide), poly(alkyl styrene), poly(vinyl ester benzoate), and these hydrogenated polymers and mixtures, or copolymers con~ining these ~Ll.l~;l~dl units. Examples of poly(alkyl styrenes) 5 include: poly(methyl styrene), poly(ethyl styrene), poly(propyl styrene), ~ poly(butyl styrene), poly(phenyl styrene), poly(vinyl n~phth~lPnf~), poly(vinylstyrene), and poly(acPn~rhth~iene) may be mentioned. As for the poly(styrene halides), exarnples include: poly(chlorostyrene), poly(bromostyrene), and poly(fluorostyrene). E~ lcs of poly(alkoxy styrene) inf~ln~1~P: poly(methoxy10 styrene), and poly(ethoxy styrene). Among these PX~ ,Ie~, as particularly p~r~ le styrene group polymers, are: poly~Lyl~lle, poly(p-methyl styrene), poly(m-methyl styrene), poly(p-tertiary butyl styrene), poly(p-chlv.o~Lyl~.~), poly(m-chloro styrene), poly(p-fluoro styrene), and copolymers of styrene and p-methyl styrene may be mentioned.
15 Furth~,.. llvle, as comc~ n~ ~.s of syndiotactic vinyl-aromatic group copolymers, besides mv lVll~:i of above Pxrl~in~?fl styrene group polymer, olefin ~vno~ such as ethylene, propylene, butene, hf~ rf?nf? or octene; diene monomers such as b~tAflif?nf? isoprene; polar vinyl . . .Ol-O. ~ .r - ~ such as cyclic diene mr~nomf r, methyl m~ths~ ~ yl~ , maleic acid anhydride, or acrylonitrile may be mentioned.
The syndiotactic-vinyl aromatic polymers of the present invention may be block copolymers, random copolymers, or ~ ;..g copolymers.
The vinyl aromatic polymer having high level syndiotactic structure referred to in this invention genf?r~lly inrhlfles poly~lyl~ne having syndiotacticity of higher than 75% or more, as flf trrminf?f~l by carbon-13 nuclear m~gnf tic reson~nre Pl~ir~bly, the degree of syndiotacticity is higher than 85% racemic diad, or higher than 30%, or more preferably, higher than 50%, racemic pentad.
In addition, although there are no particular restrictions regarding the molecular weight of this syndiotactic-vinyl aromatic group polymer, preferably, the weight average molecular weight is greater than 10,000 and less than 1,000,000, and more preferably, greater than 50,000 and less than 800,000.

As for said other resins, various types may be mentioned, inci~-ding, for in~t~nce7 vinyl aromatic group polymers with atactic structures, vinyl aromatic group polymers with isotactic structures, and all polymers that are miscible. For example, polyphenylene ethers show good miscibility with the previous explained s vinyl aromatic group polymers. Furthermore, the composition of these miscibleresin components is preferably between 70 to 1 weight %, or more pre~erably, 50 to 2 weight %. When composition of miscible resin component exceeds 70 weight %, degradation on the heat r~ ci~t~n.~e may occur, and is usually not desirable.
o It is not required that the selectefl polymer for a particular phase be a copolyester or copolyca bolldl~;. Vinyl polymers and copolymers made from monomers such as vinyl n~phth~1enec, styrenes, ethylene, maleic anhydride, acrylates, and methacrylates may also be employed. Con-7enc~tion polymers, otherthan polyesters and polyc~hl,olldlt;s, can also be nti1i7~rl Suitable con-lenc~tion polymers include polysulfones, poly~mi~les~ polyureth~n~, polyamic acids, and polyimides. N~rhth~1ene groups and halogens such as ~hlorine~ bromine and iodine are useful in hlc~ lg the leLdcliv~; index of the s~1~ct~i polymer to thedesired level (l.S9 to 1.69) if needed to ~ub:~1 ...1;~11y match the refractive index if PEN is the host. Acrylate groups and fluorine are particularly useful in decre~ing 20 the lcrld-;liv~ index.
Minor amounts of comonompr~ may be substituted into the n~phth~1ene dicarboxylic acid polyester so long as the large refractive index difference in the orient~tion direction(s) is not ~"~b~ lly cvl~-~lomised. A smaller index dirr~ ce (and therefore dc~lc;ased reflectivity) may be coulll~balanced by ~5 advantages in any of the following~ ov~d adhesion between the continuous and tli~per5e ph~e, lowered telllp~aLu~c of extrusion, and better match of melt viscosities.

Region of S~e~l~ ..~
While the present invention is frequently described herein with reference to the visible region of the spectrurn, various embo-limPnt~ of the present invention can be used to operate at different wavelen~thc (and thus frequencies) of electromagnetic radiation through a~ro~l;ate scaling of the components of the optical body. Thus, as the wavelength increases, the linear size of the components of the optical body may be increased so that the ~lim~ncions of these components, 5 measured in units of wavelength, remain approximately constant.
~ Of course, one maJor effect of çh~n~in~ wavelength is that, for most m~t~ri~lc of interest, the index of refraction and the absorption coefficient change.
However, the principles of index match and micm~trh still apply at each wavelength of interest, and may be utilized in the selection of m~t~ri~1s for an0 optical device that will operate over a specific region of the ~e.;~ . Thus, for example, proper scaling of ~lim~ncions will allow operation in the infrared, near-ultraviolet, and ultra-violet regions of the spectrum. In these cases, the indices of refraction refer to the values at these wav~lenpthc of operation, and the body thicl~n~cc and size ofthe ~licper~e phase sCs~ ;"g components should also be 15 a~3~ro,~illlately scaled with wavelength Even more of the electrom~gnP,tic ~e.;L,u~ll can be used, inchl-ling very high, llitr~hiph, mi~ilvw~vc and millim~tf~r wave freql~lonri~c Polarizing and diffusing effects wil} be present with proper scaling to wavelength and the indices of refraction can be obtained from the s~uare root of the dielectric function (in~ riin~ real and im~Ein~ry parts~. Useful products 20 in these longer wavelength bands can be diffuse reflective polarizers and partial polarizers.
In some embo iim~nt~ of the present invention, the optical pl~)pcl Lies of the optical body vary across the wavelength band of interest. In these embo-1imt?ntc, m~t~ri~lc may be utilized for the continuous and/or disperse phases whose indices 25 of refraction, along one or more axes, varies from one wavelength region to another. The choice of continuous and disperse phase m~t~ri~lc, and the optical properties (i.e., diffuse and disperse reflection or specular tr~ncmicciQn) resulting from a specific choice of m~teri~lc, will depend on the wavelength band of interest.

~;kin Layers A layer of m~f~rjzll which is substantially free of a disperse phase may be coextensively disposed on one or both major surfaces of the film, ;.e., the extruded blend of the disperse phase and the continuous phase. The composition of the 5 layer, also called a skin layer, may be chosen, for example, to protect the i-lle~-ity of the disperse phase within the extruded blend, to add m~çh~nical or physical properties to the final film or to add optical functionality to the final film. Suitable m~t~ lc of choice may include the m~t~ l of the continuous phase or the m~tf~ri~l of the disperse phase. Other m~te~l c with a melt viscosity similar to the 10 extruded blend may also be useful.
A skin layer or layers may reduce the wide range of shear; ~ .IP. ~ ;ec the extruded blend might experience within the extrusion process, particularly at the die. A high shear environment may cause nnflesir~ble surface voiding and may result in a le~Lul~d surface. A broad range of shear values throughout the thic~n~se 15 of the film may also p~ the disy~ e phase from forming the desired particle size in the blend.
A skin layer or layers may also add physical: L~ Lh to the r~elllting cc)~ osilt: or reduce problems during proc~eeing, such as, for example, reducingthe tendency for the film to split during the orient~tion process. Skin layer 20 m~t~ri~le which remain amorphous may tend to make films with a higher tou~hn~ee, while skin layer m~t~ri~le which are semicrystalline may tend to makefilms with a higher tensile modulus. Other filn~ti~n~l components such as ~ntiet7~tic additives, W a~sol~ , dyes, ~ntio~ nt~, and pi~ nte, may be added to the skin layer, provided they do not sllhst~nti~lly il~te.rele; with the desired 25 optical plo~ ies of the rçslllting product.
Skin layers or co~tin~e may also be added to impart desired barrier plo~ ies to the resllltin~ film or device. Thus, for example, barrier films or co~tin~e may be added as skin layers, or as a component in skin layers, to alter the tr~nemieeive properties of the film or device t~w~u.ls liquids7 such as water or30 organic solvents, or gases, such as oxygen or carbon dioxide.

WO 97/32230 PCT/U$97/03130 Skin layers or coatings may also be added to impart or improve abrasion reei~t~nce in the rçsl-ltinP article. Thus, for example, a skin layer comprisingparticles of silica embedded in a polymer matrix may be added to an optical filmproduced in accordance with the invention to impart abr~ion re~i~t~nce to the film, s provided, of course, that such a layer does not unduly c~ ulllise the optical properties required for the application to which the film is directed.
Skin layers or coatings may also be added to impart or improve puncture and/or tear ro~i~t~n~ e in the reslllting article. Thus, for example, in embo-lim~nt~
in which the outer layer of the optical film cunlaills coPEN as the major phase, a lO skin }ayer of monolithic coPEN may be coextruded with the optical layers to impart good tear r~ t~n~e to the reslllting film. Factors to be cûnsidered in s~ cting a m~t~ri~l for a tear resistant layer include percent elongation to break, Young's modulus, tear ~ Lh, ~rlh~ei~n to interior layers, percent ~ e and absGll,a.lce in an ele.;L~ gnetic bandwidt_ of interest, optical clarity or haze, 5 lcLa~i~iv~;; indices as a function of frequency, texture and rû-lghn~ melt thermal stability, molecular weight distributiûn, melt rheology and coextrudability, miscibility and rate of inter-diffusion between m~t~ri~l~ in the skin and optical layers, vi~coel~tic l.,;,~onse, rel~tion and cryst~lli7~tion behavior under drawconditions, thermal stability at use ~ ...~ .,.,.l...._~, w~th~or~hility, ability to adhere to 20 co~ting~c and permeability to various gases and solvents. Puncture or tear resistant skin layers may be applied during the m~nllf~turing process or later coated onto or l~.~.;..~lecl to the optical film. A~lh.oring these layers to the optical film during the m~mlf~ ring process, such as by a coextrusion process, provides the advantage that the optical film is protected during the ...;1....r~ ... ;..g process. In some 25 embo~1im~n~, one or more puncture or tear resistant layers may be provided within the optical film, either alone or in combination with a pul~ c or tear lcSi~ t skin layer.
The skin layers may be applied to one or two sides of the extruded blend at some point during the extrusion process, i.e., before the extruded blend and skin 30 layer(s) exit the extrusion die. This may be accomplished using collv~;lltional coextrusion technology, wh~ich may include using a three-layer coextrusion die.

r .~min~tion of skin layer(s) to a previously formed film of an extruded blend is also possible. Total skin layer thicknesses may range from about 2% to about 50% of the total blend/skin layer thickness.
In some applications, additional layers may be coextruded or a&ered on the outside of the skin layers during m~nllfA~t-lre of the optical films. Such additional layers may also be extruded or coated onto the optical film in a separate coating operation, or may be 15~ n1~d to the optical film as a separate film, foil, or rigid or semi-rigid substrate such as polyester (PET), acrylic (PMMA), polycarbonate, metal, or glass.
o A wide range of polymers are suitable for skin layers. Of the pred~ AI.lly amorphous polymers, suitable examples include copolyesters based on one or more of ter~,~.hlh~lic acid, 2,6-n~phth~lPn~ dicarboxylic acid, isophthalic acid phth~lic acid, or their alkyl ester coul.L~ , and alkylene diols, such as ethylene glycol. Examples of semicrystalline polymers suitable for use in skin layers include 2,6-polyethylene n~phth~l~te, polyethylene t~ ~e~l.ll.~l~t~, and nylon m~tl~ri~lc, Skin layers that may be used to incre~e the tonF~hn~occ of the optical film include high elongation polyesters such as EcdelTM and PCTG 5445 (availablecommercially from F~ctn~n Ch~mics~l Co., Rochester, NY.) and polycarbonates.
Polyolefins, such as poly~ ylene and polyethylene, may also be used for this purpose, especially if they are made to adhere to the optical film with a cnmp~tihilizer.

Fu~ti- -1 layers Various fimc~tion~l layers or co~tin~C may be added to the optical films and 2s devices of the present invention to alter or improve their physical or ~h~mi~l ~lUpe~. Lies, particularly along the surface of the film or device. Such layers or co~tingc may inçhlcle, for exarnple, slip agents, low adhesion backside m~t~ri~l.c, con-lnçtive layers, ~ntict~tic co~fing~ or films, barrier layers, flame retardants, UV
stabilizers, abrasion resist~tnt m~t~riAlc, optical co~tinp~, or substrates de~i~nP~I to im~l ove the me~h~nical i~lLegfily or strength of the film or device.

, CA 02246545 l998-08-l7 The fi}ms and optical devices of the present invention may be given good slip properties by treating them with low friction coatings or slip agents, such as polymer beads coated onto the surface. ~ It~rn~tely, the morphology of the surfaces of these m~teri~lc may be modified, as through manipulation of extrusion s conditions, to impart a slippery surface to the film; methods by which surfacemorphology may be so modified are described in U.S. Serial Number 08/612,710.
In some applications, as where the optical films of the present invention are to be used as a component in adhesive tapes, it may be desirable to treat the films with low adhesion b~cl~ci7P (LAB) co~tingC or films such as those based on lo urethane, silicone or fluorocarbon ~ h~mictry. Films treated in this manner will exhibit proper release ~,Lop~ ies towards p~ S.7UI~, sensitive adhesives (PSAs),thereby enabling them to be treated with adhesive and wound into rolls. Adhesivetapes made in this m~ el can be used for dccolalivt; purposes or in any application where a diffusely reflective or tr~ncmiccive surface on the tape is 1 5 desil~lc.
The films and optical devices of the present invention may also be provided with one or more conductive layers. Such conductive layers may co~ ..se metals such as silver, gold, copper, ~1....,;""..., cl.lomiu~l., nickel, tin, and tit~nillm, metal alloys such as silver alloys, st~inl~cc steel, and inconel, and semiconductor metal 20 oxides such as doped and undoped tin oxides, zinc oxide, and indium tin oxide (ITO).
The films and optical devices of the present invention may also be provided with ~ntict~tic co~tingc or films. Such coatings or films inchl(le, for example, V205 and salts of sulfonic acid polymers, carbon or other conductive metal layers.
The optical films and devices of the present invention may also be provided with one or more barrier films or co~tin~.C that alter the l.,."~ re properties of the optical film towards certain liquids or gases. Thus, for example, the devices and films of the present invention may be provided with films or co~ting.c that inhibit the trAncmi~cion of water vapor, organic solvents, ~2~ or CO2 through the 30 film. Barrier co~ting~ will be particularly desirable in high hnmi~lity environm~ntc, CA 0224654=, l998-08-l7 where components of the film or device would be subject to distortion due to moisture permeation.
The optical films and devices of the present invention may also be treated with flame ~ ." particularly when used in environments, such as on s airplanes, that are subject to strict fire codes. Suitable flame ,~,L~dallts include ~11..,,;,,,..,, trihydrate, antimony trioxide, antimony pentoxide, and fiame retarding organophosphate co.l.~oullds.
The optical films and devices of the present invention may also be provided with abrasion-resistant or hard coatings, which will frequently be applied as a skin o layer. These include acrylic hardcoats such as Acryloid A-l 1 and Paraloid K-120N, available from Rohm & Haas, Phil~lelrhi~ PA; ~;LI-~le acrylates, such as tnose described in U.S. Pat. No. 4,249,011 and those available from Sartomer Corp., We~ h~ ., PA; and u~c;l~ e hardcoats obtained from the reaction of an ~liph~tic polyisocyanate ~e.g., Desmodur N-3300, available from Miles, Inc., Pill~l)ul~,ll, PA) ~,vith a polyester ~e.g., Tone Polyol 0305, available from Union Carbide, Houston, TX).
The optical films and devices of the present invention may further be ecl to rigid or semi-rigid :iu~ LLates~ such ~, for example, glass, metal, acrylic, polyester, and other polymer b?~ ~in~.c to provide structural rigidity,w~thPr~hility, or easier h~nflling For example, the optical films of the presentinvention may be 1~ cl to a t_in acrylic or metal b~c~in~ so that it can be st~mpe~l or otherwise formed and 11~ F~ in a desired shape. For some applications, such as when the optical film is applied to other brealcable b~ in~,c, an ~ litionzll layer c~ mri~in~ PET film or pun~;Lule-tear resistant film may be2s used.
The optical fflms and devices of the present invention may also be provided with shatter resistant films and coatings. Films and coatings suitable for this purpose are described, for P~mple, in publications EP 592284 and EP 591055, and are available commercially from 3M Company, St. Paul, MN.
Vanous optical layers, m~t~ , and devices may also be applied to, or used in col~ lcLion with, the films and devices of the present invention for specific WO 97/32230 I'CT/US97/03130 applications. These include, but are not limited to, m~Enetic or magneto-optic co~tin~s or filrns; liquid crystal panels, such as those used in display panels and privacy windows; photographic emulsions; fabrics; pri~m~tic films, such as linear Fresnel lenses; brightnees ~nh~nr~ment films; holographic films or images;
s embossable films; anti-tamper films or coatings; IR transparent film for low ~ emissivity applications; release films or release coated paper; and polarizers or mirrors.
Multiple additional layers on one or both major surfaces of the optical film are colllelnplated, and can be any combination of ~lelllcntioned coSltin~ or films.
o For example, when an a&esive is applied to the optical film, the adhesive may contain a white pigm~nt such as liL~liu l- dioxide to increase the overalI
reflectivity, or it may be optically tr~n~p~rent to allow the reflectivity of the ~ub~LlaL~ to add to the reflectivity of the optical film.
In order to improve roll formation and coll~.~Libility ofthe film, the optical 5 films ofthe present invention may also comprise a slip agent that is incc.~olaL~d into the film or added as a sc~ e co~ting- In most applic~tion~, slip agents will be added to only one side of the film, ideally the side facing the rigid ~ua~ dle in order to ~ haze.

20 Microvoiding In some embodiment~, the m~tPri~lc of the colltinllous and disperse phases may be chosen so that the int~ t e bt;Lwt;ell the two phases will be s..ffiçiently weak to result in voiding when the film is oriented. The average ~limen~ion~ of the voids may be controlled through careful manipulation of proce~ing par~m.ot~rs 2s and stretch ratios, or through selective use of col~ libilizers. The voids may be back-filled in the fini~1 product with a liquid, gas, or solid. Voiding may be used in conjunction with the aspect ratios and leLa~ re indices of the di~ e andcontinuous phases to produce desirable optical ~ llies in the resnlting film.

More Than Two Phases The optical bodies made in accordance with the present invention may also consist of more than two phases. I~us, for example, an optical m~t~ l made in accordance with the present invention can consist of two different disperse phases s within the continuous phase. The second disperse phase could be randomly or non-randomly dispersed throughout the continuous phase, and can be randomly aligned or aligned along a common axis.
Optical bodies made in accordance with the present invention may also consist of more than one continuous phase. Thus, in some embo~imentc, the 0 optical body may include, in addition to a first continuous phase and a disperse phase, a second phase which is co-co~ luous in at least one ~7in~PnciQIl with the first continuous phase. In one particular emboriimPnt the second continuous phase is a porous, sponge-like material which is coe~LGl~ivG- with the first continuous phase (i.e., the first contin~ us phase extends through a nGL~ k of çh~nnelc or ls spaces PYtPn-ling through the second continllous phase, much as water extendsthrough a network of c l~nnPls in a wet sponge). In a related embodiment, the second continuous phase is in the form of a flPnAritic :jLL U~;lUI~_ which is coextensive in at least one ~limPnci~n with the first continuous phase.

20 Mu}tilayer Cc h~
If desired, one or more sheets of a co~tinllous/~ p~rse phase film made in accor~lce with the present invention may be used in combination with, or as a c~ o~el,L in, a multilayered film (i.e., to i~-~;lGase reflectivity). Suitable multilayered films include those of the type described in WO 95/17303 (Oll~lçrkirk 25 et al.). In such a construction, the individual sheets may be l~"~in~ or otherwise adhered together or may be spaced apart. If the optical thicknPc~çs of the phases within the sheets are sllbst~nti~lly equal (that is, if the two sheets present asllhst~nti~lly equal and large number of scalh~Gl~ to incident light along a given axis)7 the composite will reflect, at somewhat greater efficiency, ~bs~ 11y the 30 same band width and spectr~l range of reflectivity (i.e., "band") as the individual sheets. If the optical thicl~ne~es of phases within the sheets are not :iub~ lly equal, the composite will reflect across a broader band width than the individual phases. A composite combining mirror sheets with polarizer sheets is useful for increasing total reflectance while still polarizing tr~nsmitte(l light. ~Itern~tively, a ~ single sheet may be asymmetrically and biaxially oriented to produce a film having 5 selective reflective and polarizing p~ . Lies.
FIG. 5 illustrates one example of this embodiment of the present invention.
There, the optical body consists of a multilayer film 20 in which the layers altern~te between layers of PEN 22 and layers of co-PEN 24. Each PEN layer inrll-fles a disperse phase of syndiotactic polystyrene (sPS) within a matrix of PEN.
0 This type of col~shuc~ion is desirable in that it promotes lower off-angle color.
Furtherrnore, since the layering or inclusion of scaLL~ averages out light leakage, control over layer thickness is less critical, allowing the film to be more tolerable of variations in processing p~r~meters Any of the m~t~ri~l~ previously noted may be used as any of the layers in 5 this embo~lim~nt or as the continuous or disperse phase within a particular layer.
However, PEN and co-PEN are particularly desirable as the major components of ren~ layers, since these m~tPri~l~ promote good laminar adhesion.
Also, a number of variations are possible in the arrangement of the layers.
Thus, for PY~mple7 the layers can be made to follow a ~ aling sequence through 20 part or all of the ~LIu~L~ . One example of this is a co~ku~Lion having the layer pattern ... ABCABC ..., wherein A, B, and C are distinct m~tP ~lc or distinct blends or nli~Lu~es of the same or dirr~ l m~tPri~lc, and wh~leill one or more of A, B, or C contains at least one disperse phase and at least one continuous phase.
The slcin layers are preferably the same or chemically similar m~ n~
Antirefl- - Layers The films and other optical devices made in accol~ulce with the invention may also include one or more anti-reflective layers or coatings, such as, for example, conventional vacuum coated dielectric metal oxide or metal/metal oxide - 30 optical films, silica sol gel co~tin~ and coated or coextruded antireflective layers such as those derived from low index fluoropolymers such as THV, an extrudable fiuoropolymer available from 3M Company (St. Paul, MN). Such layers or co~ting~, which may or may not be polarization sensitive, serve to increase tr~n~m;~sion and to reduce reflective glare, and may be imparted to the films and optical devices of the present invention through ~pplo~lLate surface trç~tment such s as coating or sputter etching. A particular example of an antireflective coating is described in more detail in Examples 132-133.
In some embotlim~ntc of the present invention, it is desired to m~imi7~ the tr..n~n~ ion and/or minimi7t~ the specular reflection for certain polarizations of light. In these embodiments, the optical body may comprise two or more layers in0 which at least one layer comrri~çs an anti-reflection system in close contact with a layer providing the continuous and sll .p~. .t; phases. Such an anti-reflection system acts to reduce the specular reflection of the inri~1ent light and to increase the amount of incident light that enters the portion of the body co. l ~ i . .g the Co~ ou~s and ~ p~qr~se layers. Such a function can be accomplished by a variety 5 of means well known in the art. FY~.mples are quarter wave anti-reflection layers, two or more layer anti-reflective stack, graded index layers, and graded densitylayers. Such anti-reflection functions can also be used on the l...~ light side of the body to increase ~ le(l light if desired.

20 Anti-Fog Layers The films and other optical devices made in accu..l~lce with the invention may be provided with a film or coating which imparts anti-fogging ~up~,.lies. Insome cases, an anti-reflection layer as described above will serve the dual purpose of hll~al ~h~, both anti-reflection and anti-fogging l,rop~,. lies to the film or device.
Various anti-fogging agents are known to the art which are suitable for use with the present invention. Typically, however, these materials will substances, such as fatty acid esters, which impart hydrophobic ~lu~c~lies to the film surface and which promote the formation of a continuous, less opaque film of water.
Coatings which reduce the tendency for surfaces to "fog" have been reported by several inventors. For example, U.S. Patent No. 3,212,909 to Leigh discloses the use of ammonium soap, such as alkyl ,.mmonillm carboxylates in ~mixtnre with a surface active agent which is a sulfated or sulfonated fatty matterial, to produce a anti-fogging composition. U.S. Patent No. 3,075,228 to Elias discloses the use of salts of sulfated alkyl aryloxypolyalkoxy alcohol, as well as alkylbenzene sulfonates, to produce an anti-fogging article useful in cleaning 5 and hll~Lhlg anti-fogging plO~ Lies to various sllrf~ec U.S. Patent No.

3,819,522 to Zmoda, discloses the use of sllrf~rit~nt combinations comprising derivatives of decyne diol as well as snrf~ t~nt lllixlu~es which include ethoxylated alkyl sulfates in an anti-fogging window cleaner sllrf~c~t~nt mixture. Japanese Patent Kokai No. Hei 6[1994]41,335 discloses a clouding and drip pl~V~ .ILi~
10 composition compricin~ colloidal ~hlmin~ colloidal silica and an anionic ,--. r~ n~-~ U.S. Patent No. 4,478,909 (T~ni$~n~hi et al) ~licclos~c a cured anti-fogging coating film which comrrie~c polyvinyl alcohol, a finely divided silica,and an organic silicon compound, the carbon/silicon weight ratio a~l~dle~ y ebing lL~ to the film's reported anti-fogging ~rop~lLies. Various ~I.. r~
1S include fluorine-c~...l~;..;..g sl~ t~ntc~ may be used to improve the surfacesmoothness of the co~ting Other anti-fog co~tin~c incol~oldLi~g ~- ~- r~ are described in U.S. Patents 2,803,552; 3,022,178; and 3,897,356. World Patent No.
PCT 96/18,691 (Scholtz et al) discloses means by which Co~ i may impart both anti-fog and anti-reflective plOp~ll~es.
UV Protective Layers The films and optical devices of the present invention may be plole~ d from W radiation t-h-rough the use of W stabilized films or co~tingC Suitable W
st~hili7Pfl films and co~tin~c include those which incol~o.a~ bel~oll;azoles or zs hindered amine light stabilizers ~HALS) such as Tinuvin~M 292, both of which are available comrnercially from Ciba Geigy Corp., Hawthorne, NY. Other suitable W stabilized films and co~ting.c include those which contain benzoph~n~-nes or diphenyl acrylates, available coll..ll~.cially from BASF Corp., PdL~i~ly, NJ.
Such films or coatings will be particularly hnpol L~l when the optical films and30 devices ofthe present invention are used in outdoor applications or in ll....;..~;..s where the source emits signirlc~ll light in the UV region of the spectrum.

Surface Tr. - ' _ ts The films and other optical devices made in accordance with the present invention may be subjected to various tr~tm~nts which modify the surfaces of s these mAt~ri~iC, or any portion thereof, as by rendering them more conducive to subsequent treAtment~ such as co~ting dying, m~tAIli7ing, or lAmin~tinn. This may be accomplished through treAtm~nt with primers, such as PVDC, PMMA, epoxies, and aziridines, or through physical priming 1,~ ; such as corona, flame, plasma, flash lamp, sputter-etrhin~, e-bearn treAtrnent~, or amo~hi,il.g the surface l o layer to remove crystallinity, such as with a hot can.

LUIJ,, ~ - -Various lubricants may be used during the proc~C~ing (e.g., extrusion) of the films of the present invention. Suitable lubricants for use in the present s invention include calcium sterate, zinc sterate, copper sterate, cobalt sterate, molyl,dellulll neoAoc~nc-Ate, and l~ ..i..." (III) acetylacetonate.

~ ~ ~ .
Antioxidants useful in the present invention include 4,4'-thiobis-(6-t-butyl-m-cresol), 2,2'-methylenebis-(4-methyl-6-t-butyl-butylphenol), octadecyl-3,5-di-t-butyl-4-hydroxylly~1lo~ ?, bis-(2,4-di-t-butylphenyl) pentat~ L;l rliphn~hitP, IrganoxTM 1093 (1979)(((3~5-bis(1~1-dimethylethyl)-4-hy~ y~h~llyl)methyl)-dioctadecyl ester ph~sphonic acid), IrganoxTM 1098 (N,N'-1,6-h~.~Anl~iylbis~3,5-bis(l,l dimethyl) 4 ~lydL~oxy-~pn7pn~r~ l"~"~
N~uga~LLdTM 445 (aryl amine), IrganoxTM L 57 (alkylated diphenylamine), IrganoxTM
L 115 (sulfur contAinin~ bi~hf~nol), IrganoxTM LO 6 (alkylated phenyl-delta-napthylamine), Ethanox 398 (flourophnc.l~hnni~t:), and 2,2'-ethylidenebis(4,6-di-t-butylphenyl)fluol~)ho~
A group of antioxidants that are especially ~.c~ ,d are sterically hindered phenols, in~hl-lin~ butylated hydroxytoluene (BHT~, Vitarnin E (di-alpha-toco~helol~, IrganoxTM 1425WL(calciurn bis-(O-ethyl(3,5-di-t-butyl-4-hydroxyl.el~yl))phosphon~t~), IrganoxTM 1010 (tetrakis(methylene(3,5,di-t-butyl-4-hydroxyhydrocinn~m~te))n~eth~ne), IrganoxTM 1076 (octadecyl 3,5-di-tert-butyl-4-hydroxyhydroeinn~m~tP), EthanoxTM 702 (hindered bis phenolic), Etanox 330 - (high molecular weight hindered phenolic), and EthanoxTM 703 (hindered phenolic 5 amine).

Dyes, Pigments, Inks, and T.-.~t~ Layers The films and optical devices of the present invention may be treated with inks, dyes, or pjgrnl~t te to alter their a~ e~ e or to cu~lu~ t; them for specific 10 applications. Thus, for ex~mrle, the films may be treated with inks or other printed indicia such as those used to display product i~l~ntifi~tion~ adverti~
w~rning.c, decoration, or other h-fu~ n- Various techniques can be used to print on the film, such as scLe~ g, 1C;L~ S~S~ offset, flexographic printing, stipple printinp, laser pr inting, and so ffirth, and various types of ink can be used, ~5 including one and two co~oll~nt inks, oxidatively drying and W-drying inks, dissolved inks, rliep~ree~l inks, and 100% ink systems.
The a~e .. .~ e of the optical film may also be altered by coloring the film, such as by lS -lliili11;1~ a dyed film to the optical film, applying a pigmentçcl coating to the surface of the optical film, or including a pi m~nt in one or more of them~t~ri~le (e.g., the continuous or disperse phase) used to make the optical film.
Both visible and near IR dyes and I)i mentc are co.ll~;lllE lated in the presentinvention, and inr.hlcle, for c:x~llplc, optical hti~ i such as dyes that absorb in the W and nuci~sce in the visible region of the colom~e~;Ll ~ll. Other z~rldition~
layers that may be added to alter the appe~r~n~e of the optical film include, for example, opacifying (black) layers, ~I;rrlle;,~g layers, holographic images or holographic .l; rr, .c~. ~, and metal layers. Each of these may be applied directly to one or both sllrf~es of the optical film, or may be a col.l~ullent of a second film or foil construction that is ~ cl to the optical film. ~lt~rn~tely, some cc,ll~ollents such as opacifying or ~liffi~eing agents, or colored pi~mente, may be - 30 inclll~1e~1 in an adhesive layer which is used to l~."i~ the optical film to another sllrf~-~e.

~ .

The films and devices of the present invention may also be provided with metal co~tingS. Thus, for example, à metallic layer may be applied directly to the optical film by pyrolysis, powder coating, vapor deposition, cathode 5~ g, ion plating, and the like. Metal foils or rigid metal plates may also be 1~min~te :1 to the s optical film, or separate polymeric films or glass or plastic sheets may be first met~lli7~cl using the aforementioned techniques and then 1~min~fe~l to the optical films and devices of the present invention.
Dichroic dyes are a particularly useful additive for many of the applications to which the films and optical devices of the present invention are directed, due to lo their ability to absorb light of a particular po1~n7~tion when they are molecularly aligned within the m~t~ri~1 When used in a film or other m~t.ori~l which pre~ln1.1;11A.1l1y scatters only one polarization of light, the dichroic dye causes the mslt~risl1 to absorb one pnk-ri7~tion of light more than another. Suitable dichroic dyes for use in the present invention include Congo Red (sodium diphenyl-bis-a-5 na~lylamine sulfonate), methylene blue, stilbene dye (Color Index (CI) = 620),and 1,1'-diethyl-2,2'-cyanine ~h1Ori~1e (CI = 374 (orange) or CI = 518 (blue)). ~he .o~ ies of these dyes, and m~tho-i~ of m~king them, are described in E.H. Land, Colloid Ch~ (1946). These dyes have noticeable dicl~r~ .l in polyvinyl alcohol and a lesser dichroism in cellulose. A slight dichlvi~.ll is observed with 20 Congo Red in PEN.

Other suitable dyes include the following materials:
(1) R~R

whereRis ;~ 3 o OH

(3 O NH2 o ~4) ~N--CH~) The p--ap~,~ Lies of these dyes, and methods of making them, are discussed in the Kirk Othmer Encyclopedia of Ch~ l Technology, Vol. 8, pp. 652-661 (4th Ed.
5 1993), and in the references cited therein.
When a dichroic dye is used in the optical bodies of the present invention, it - - may be incoll,olaLt;d into either the continllo~ or disperse phase. However, it is ~.~r~ .,d that the dichroic dye is incorporated into the disperse phase.

Dychroic dyes in combination with certain polymer systems exhibit the ability to polarize light to varying degrees. Polyvinyl alcohol and certain dichroic dyes may be used to make films with the ability to polarize light. Other polymers, such as polyethylene terephth~l~t~ or poly~mi~les, such as nylon-6, do not exhibit 5 as strong an ability to polarize light when combined with a dichroic dye. The polyvinyl alcohol and dichroic dye combination is said to have a higher dichroism ratio than, for example, the same dye in other film forming polymer systems. A
higher dichroism ratio in~ t~s a higher ability to polarize light.
Molecular ~li nm~nt of a dichroic dye within an optical body made in lo accordance with the present invention is preferably accomplished by ~,LL~,Lcl~ g the optical body after the dye has been inco~ -dled into it. However, other methods may also be used to achieve molecular ~lignment Thus, in one method, the dichroic dye is cryst~11i7e-1, as L~ U~11 sublim~ticm or by cryst~11i7~fi-)n from solution, into a series of el~ng~t~o~l notches that are cut, etched, or otherwise formed IS in the surface of a film or other optical body, either before or after the optical body has been ol;elllt;d. The treated surface may then be coated with one or more surface layers, may bé incc,l~uld~;d into a polymer matrix or used in a multilayer structure, or may be utilized as a cc~lllpollc.lL of another optical body. The notches may be created in accord~ce with a pred~l- . ..,i..~l pattern or ~ gr~n, and with a 20 pre~1~t~rmin~1 amount of ~r~cing between the notches, so as to achieve desirable optical p-up~.Lies.
In a related embc-lim~nt the dichroic dye may be disposed within one or more hollow fibers or other c~ n~lllit~, either before or after the hollow fibers or con-i11it~ are disposed within the optical body. The hollow fibers or co~ may 25 be constructed out of a m~t~ri~1 that is the same or ~ .lL from the surrounding m~t~ri~1 of the optical body.
In yet another embodiment, the dichroic dye is disposed along the layer intt-rf~- e of a multilayer col~,Ll .~clion, as by sublimation onto the surface of a layer before it is inc~ Led into the multilayer construction. In still other 30 embot1im~nt~, the dichroic dye is used to at least partially backfill the voids in a microvoided f lm made in accoLdance with the present invention.

Adhesives Adhesives may be used to l~min~te the optical films and devices of the present invention to another film, s~ e.? or substrate. Such adhesives include 5 both optically clear and diffuse adhesives, as well as ~le~u-~; sensit;ve and non-pressure sensitive adhesives. Pressure sensitive adhesives are normally tacky atroom telllpe~aLule and can be a&ered to a surface by application of, at most, light finger ~.es~, while non~ s:~e sensitive adhesives include solvent, heat, or radiation activated adhesive systems. Examp}es of adhesives useful in the present o invention include those based on general compositions of polyacrylate; polyvinyl ether; diene-c~ rubbers such as natural rubber, polyisoprene, and polyisobutylene; po}ychloroprene; butyl rubber; bnt~ en~-acrylonitrile polymers;thermoplastic c!~ ; block copolymers such as styrene-isoprene and styrene-isoprene-styrene block copolymers, ethylene-propylene-diene polymers, and 15 styrene-bllt~rli~ne polymers; polyalphaolefins; amorphous polyolefins; silicone;
ethylene-co..~ gJ copolymers such as ethylene vinyl acetate, ethylacrylate, and ethylmeth~crylate, poly~e~ f ~; polyamides; polyt;~Lt;~, epoxies;
polyvh~yl~y~olidone and vinylpyrrolidone copolymers; and mi~Lul.,s of the above.liti~ lly, the adhesives can contain additives such as tackifiers, pl~etici7~re~ fillers, ~ntioxi~l~ntc~ stabilizers, pi~m~nte, ~liffilein~ paTticles, ~;uLaLiv~s, and solvents. When a Iz~.,,i,,~l;,.~ a&esive is used to adhere an optical film of the present invention to another sllrf~ce, the adhesive composition and thicl~nPc.e are preferably s~ ct~o~ so as not to i~L.,~ with the optical ~ lies of the optical film. For ç-*~mple7 when l~ ;,.g ~ liti~)n~l layers to an optical polaTizer or mirror wherein a high degree of tr~nemis~ion is desired, the 1~ ;"p;
adhesive should be optically clear in the wavelength region that the polarizer or mirror is ~leci~nto-l to be I l,~ lL in.

Other Additives In ~ liti~n to the films, coatings, and additives noted above, the optical m~tt-ri~le of the present invention may also compriee other m~t~ri~le or additives as ~s-CA 02246545 l998-08-l7 are known to the art. Such m5~tt~ri:~1.c include binders, co~tingC~ fillers, compatibilizers, surfactants, antimicrobial agents7 foaming agents, reinforcers, heat st~hili7~rs, impact modifiers, plasticizers, viscosity modifiers, and other such m~t~ ic, Gelleral Applications of rr~ t Invention The optical bodies of the present invention are particu}arly useful as diffuse pol~ri7Pnc However, optical bodies may also be made in accordance with the invention which operate as reflective polarizers or diffuse mirrors. In these 0 applications, the col~L,~;Lion of the optical mzltf~ri:~l iS similar to that in the diffuser applications described above. However, these reflectorc will g~n~r~lly have a much larger di~ .ellce in the index of refraction along at least one axis. This index di~ llCe iS typically at least about 0.1, more preferably about 0.15, and most preferably about 0.2.
Reflective polarizers have a l~r~a~;live index difr~.e.lce along one axis, and ~Ul~ lly ...~ e~ indices along another. Reflective filrns, on the other hand, differ in lc~ld~;Liv~ index along at least two in-film plane orthogonal axes.
However, the reflective ~ p~.Lies ofthese embo-1imPntc need not be ~tt~in~
solely by reliance on refractive index micm~t~h~s Thus, for example, the 20 thic.knPcc of the films could be adjusted to attain a desired degree of reflection. In some cases, adj . .~ . .1 of the thicknPqs of the film may cause the film to go from being a fr~ncmiccive diffuser to a diffuse reflector.
The reflective polarizer of the present invention has many difl~
applications, and is particularly useful in liquid crystal display panels. In addition, 25 the polarizer can be constructed out of PEN or similar m~ten~lc which are good ultraviolet filters and which absorb ultraviolet light efficiently up to the edge of the visible ~c~ ll~. The reflective polarizer can also be used as a thin infrared sheet polarizer.

~6--F~,..~.,l~ ..tions The optical films and devices of the present invention are suitable for use in fenestrations, such as skylights or privacy windows, where diffuse tr~n~mi~eion of light is desirable and transparency or clarity of the fenestration is either s l~nn~cçe~ry or undesirable. Irl such applications, the optical films of the present invention may be used in conjunction with, or as components in, conventional glazing m~t~n~l~ such as plastic or glass. Glazing m~teri~le ~ ~ed in this manner can be made to be polarization specific, so that the fenestration is ~-eeenti:llly l~d~ ~e.ll to a first pol~ri7~tion of light but subst~nti~lly reflects a 0 second polarization of light, thereby elimin~ting or reflu~ing glare. The physical plU~G~ Lies of the optical films can also be modified as taught herein so that the glazing m~t~ri~l~ will reflect light of one or both pol~ri7~ti~ ns within a certain region of the s~e-;LI u~-l (e.g., the W region), while f . ,...~ g light of one or both polarizations in another region (e.g., the visible region).
The optical films of the present invention may also be used to provide decorative r~ .le ,LlaLions which 1~ .; l light of specific wavelengths. Such r~ ,f~l;ons may be used, for c ;..,,ple, to impart a specific color or colors to a room (e.g., blue or gold), or may be used to accent the decor thereof, as through the use of wavelength specific lighting panels.
The optical films ofthe present invention may be hlcol~oldLGd into glazing m~ri~l~ in various ...~..I....i as are known to the art, as through coating or extrusion. Thus, in one embodiment, the optical films are adhered to all, or a portion, of the outside surface of a glazing m~t~r~ either by l~min~tion or withthe use of an optical adhesive. In another embodiment, the optical films of the 25 present invention are sandwiched b~,~weGll two panes of glass or plastic, and the r~clllting composite is incol~oldLGd into a fenestration. Of course, the optical film may be given any additional layers or coatings (e.g., W absorbing layers, antifogging layers, or antireflective layers) as are described herein to render it more suitable for the specific application to which it is directed.

~7-Light Fixtures The optical films of the present invention may be used in various light fixture applications, especially those in which polarized emitted light is p~r~ .red.
A typical light fixture contains a light source and various other elem~ntC whichs may include a reflective element (typically placed behind the light source), apol~ri7ing elem~nt (typically positioned at the output of the light fixture), and a diffusing element that obscures the light source from direct viewing. These el~mentc may be arranged in various confignratinnc within a housing as dictated by a~sthPtic and/or functional considerations.
The light sources most suitable for use with the optic~l films of the present invention are diffuse light sources which ernit light having a high degree of scatter or r~n~omi7~tinn with respect to both polarization and direction. Such diffuse sources preferably include a light emittin~ region and a light reflecting, sc~ g, and/or depol~ri7ing region. Depending upon the particular application to which the 5 light fixture is directed, the diffuse source may be a nuo-e3cclll lamp, an in~nll~scent lamp, a solid-state source or electrol~ cc- ~~1 (EL) light source, or a metal halide lamp. The source may also be a rando.lPi~g, depol~ri7ing surface used in combination with a point light source, a distant light source, or even solar illl...,;l, 3l;on, the later being L~ e~l to the diffuse polarizer by free space 20 propagation, a lens system, a light pipe, a polarization ~lcse~ ~/illg light guide, or by other means as are known to the art In a n~lol~,scclll lamp, such as a hot or cold cathode lamp of the type used in a typical backlit LCD, the light ~ ...il~;..g region and the light refl.?cting, Sf'.;.~t~ ~ ;llg and depol~ri7ing regions are combined into the phncphnrs, which serve all of these 25 fi~nctions. In the case where a highly collim~t~l beam of light is desired, the reflective polarizing element can be optically configured to image the rejected polarization back onto the light ~",;~ region, which will typically be a fil~ment or arc. The light Pmitting region may serve both as the light source and the depol~ri7ing region. ~ltprn~tely~ the light source may comprise a light ~mittin g 30 region and a se~iudlc ran~lomi7ing reflector.

~8-As described previously, the optical films of the present invention may be either a diffuse reflecting polarizing film (DRPF), in which light of one plane of polarization is L~ eA and light of the other plane of polari_ation is diffusely reflected, or it may be a diffuse reflecting mirror film ~DRMF) in which both 5 planes of polarization are diffusely reflected from the film. As such, the optical film of the present invention may be used in a light fixture as the reflective element and/or the polarizing element. Since the film is diffusely reflective and optically tr~n.~hlcPnt a s~ diffusing element is not nPcess~ry and the present optical film can fimction as both the ~ cing çlement and the polarizing element.
Optical films of the present invention may be used in co~ lional ll...,i.~i.;. ;es that use louvers both to direct the light as well as to obscure the light source from direct view. If films of the present invention are l~n~in~tPA or otherwise juxtaposed to col~ llionally llliLlc,lcid louvers, then one pol~n7~tion of light could be diffusely reflected, wh~ .cas the second pol~ri7~tinn of light could be directed (e.g., nearly vertically3 to .,.;~ glare throughout the ill~ rA area.
One could envision the use of at least two pieces of optical film of the present invention, where one is rotatable with respect to the other, used in lighting fixtures so that the intensity and/or degree of polarized light could be controlled or tuned for the specific needs of the imm~ te ellvilol.lllent.
For those applications where polarized light is not required, such as in the typical i 1-- . . i . .~;.es used for office li~htin~, the light fixture generally consists of a housing c~,..l71;..;l-g a light source, such as a fluorescent bulb, a reflecting elem~nt behind the light source, and a dirrusillg eleTn~nt The source may be any of the light sources noted above (e.g., a fluorescc;nl lamp). The reflecting element may be any 25 reflective s~ e, including, for example, a painted white reflector, a m~t~lli7~r1 film such as Silverlux TM brand reflective film (available coll....~.cially from 3M
Colll~al~, St. Paul, MN), a reflective metal surface such as polished al. .i, . . .ll l., ,, or a reflective multilayered, birefringent mirror film such as that described in WO95/17303 and WO 96/19374 and inevl~ulaled herein by reference. In one 30 embodiment, the DRMF of the present film as herein described may be used as the reflective elernent in a non-polarized light fixture. The DRM~ may additionally be CA 02246',45 1998-08-17 mPtsllii7t?d either by vapor coating or k7minsl~ing a reflective metal to the back side of the DRMF to improve total reflecthity.
Many applications require polarized light to function plup~,ly. Examples of such an applications include optical displays, such as liquid crystal displays 5 (LCDs), which are widely used for lap-top CO~ u~,.S, hand-held calculators, digital watches, automobile dashboard displays and the like, and polarized luminaires and task 1ighting which make use of polarized light to increase cO~ a.,l and reduce glare. For applications where polarized light is desired, the light fixture generally consists of a housing co..ts ;..i.,~ a light source and a polarizing element 0 and may additionally include a reflecting element and/or a .li lr~ element. The light source may be any of the light sources dP~ribe~ above (e.g., a fluorescentlarnp), but is ~l~,dbly a diffuse light source which emits light having a high degree of scatter or r,7nriomi7f7tion with respect to both pok7ri7fltiQn and direction.
The reflecting eiemPnt if present, may be any of the reflective msltPris7l c described above, or may also be the BRMF of the present invention. The polarizing element may include any polarizer, including abso.l,ing dichroic, thin film dielectric or cholesteric polsn i7Prs, but is ~f~,lably the mu tilayer bire~in~-P-nt reflective pol~rizer described in WO 95/17303 and WO 96/19347.
Absorptive polarizers typically use dichroic dyes which tr,7n~mit light of one pol~r77fltinn orientsltion more ,l-ollgly than the o thogonal poi~ri7sltion orientsltion When an absol~tive polarizer is used in a display or polslri7pcl light fixture, for example, the absorbed light does not contribute to the illl7mins tion, and thus to the overall brightnPss, ofthe LCD or h~ s);.e. The use of such polarizers in li~hting applications is described in 7J.S. Pat. Nos. 3,124,639 (Kahn), 3,772,128 2s (Kahn), and 4,796,160 (Kahn), and ~ U.S. Pat. Nos. 5,184,881 (Karpen) and 5,359,498 (KaIpen). Vacuum deposited, thin film dielectric pola~zers are not absorbing, as are dichroic polslri7Prs7 but do suffer other disadvantages, such as poor angular response and poor spectrs l trsln~mi~ion for non--lesi~nPd wavelength~ In addition, they are co~ ionally coated onto stable substrates, such as buLtc optical glass or polymer substrates, and this may render them too buLky and heavy for use in li~hfing applic~tion~ requiring light weight and small -so-profile. For some li~hting applications, these polarizers may be combined with asuitable light source and the DRMF of the present invention to provide a polarized light fixture.
The prer~,.,ed reflective polarizers specularly transmit light of a desired 5 polarization and reflect light of another polarization. Light produced by a diffuse source is randomly polarized and therefore has polarization components (a) and (b) present. This light is incident on the reflective polarizing element. The reflective polAri7in~ element is adapted to transmit light having a first polAri7Ation component (polarization component (a) in this example), and reflect light having10 the orthogonal pol~ri7Ati~m col~ ollent ((b) in this e~A~nl le). Consequently, light of polarization co~ olle.l~ (a) is ~ -..iLlecl by the reflective poiAri7in~ element, while light of polari_ation co~ o~lent (b) is reflected back into the light fixture where it is randomized. Some of the initially rejected light is thus converted into the desired polAri7AtiQn and is specularly l.,...x...;lled through the reflective 15 polAri7ing element. This process co..I;.. ~ e, and the repeated reflections and xubse~lu~ rAn~iomi7Ation of light of the undesired polAri7Atif)n increases the amount of light of the desired polarization that is emitted from the diffuse pol~ri7f-~1 light fixture. The result is a very efficient system for producing light of a desired polAri7Ation- The repeated reflections and randomizations effected by the 20 comhinAtinn of the diffuse source and the reflective polarizing element form an efficient mecl7s...;~. for COllV~ g light from state (b) to state (a). The system is efficient in the sense that light which would other~-vise have been absorbed, and therefore unavailable, is instead collvt;lled to the desired polAri7~tiQn. A light fixture using such a polAri7in~ el~ment thus makes much more efficient use of the 2s light emitted from the source, since light of the rejected polAri7Ati~n is reflecte(l back into the source and randomized. As a result, the total amount of light emitted from the fixture in the desired polarization is increased. The use of a multilayer bil~rlillgent reflective polAri7ing film (RPF) in li~htin~ applications is described in applicants commonly AeeiFne-1 U.S. Patent Application Serial Numbers 08/418,009 and 08/479,319, also incol~ol~Led herein by reference. These applications describe the use of the multilayer RPF in liph*n~ applications, especially in LCD displays :

and polarized luminaires. The reflective po1~ri7ing element of these applications light of a desired polarization and specularlY reflects light of another polarization back into the diffuse source where it is randomized. When a multilayer RPF is used in this way, a separ~te diffuser film is typically used in 1llmin~;res or s task 1i~hting applications so that the light source is not directly visible. Areflective element is preferably also included in these polarized light fixtures, and the reflective element may comprise the BRMF of the present invention or any othe~r suitable reflective surface that either ranrl~ mi7~e the light reflected from the RPF or reflects the rçflecte~ light back into a diffusing source where it can be0 randomized and partially cc,~ .Lt:d into the correct polarization to be ~ /e-l by the pl~1ari7ing element.
The DRPF of the present invention functions similar to the multilayer RPF
to increase the arnount of light of the desired polari7~tion that is emitted by the polari7ed light fixture, however, the initially rejected light of the wrong s polarization is diffusely rçflecte(l back into the light fixture where it may be randomi_ed, partially converted to light of the correct po1~ri7~tinn~ and specularly ", il le~ through the po1~ri7ing element. The diffuse reflective polari_ing film(DRPF) ofthe present invention is tr~n~ Pnt so that a se~ .,.le difrus~. is not needed. When combined with the light source to make a diffuse reflecting 20 polarized light fixture, a reflecting elemPnt is preferably also incl~ e~1 to direct the reflected light back to the source and/or aid in the randomi7~tion and partial conversion of the r~flecte~l light into light of the correct pol~ri7~tion to be e~l by the po1~ri7ing element. The reflecting C1~.2~ may be any suitable reflective m~teris~l as described above, and in particular may be the DRMF of the 25 present invention. As such, the DRMF of the present invention may be used in one embodiment as the reflecting e1ement and the DRPF of the present invention may be used as the pf)1~ri~ing elPment and/or the ~1iffi-~ing element.
In the light fix~ s described herein, the light source may be coupled with the po1~ri~ing elenn~nt and reflecting e1ement in a variety of config--r~tion~ Some 30 of the configurations will be described with respect to using the diffuse reflecting po1~ri7ing film (DRPF) of the present invention as ~e polariing element and the CA 02246545 l998-08-l7 diffuse reflectinP mirror film (DRMF) of the present invention as the reflectingelement, but it should be recognized that various combinations of DRPF with other m~t~ri~lc as the reflectin~ element and DRMF with other m~tl-ri~lc as the polarizing element are envisioned. In one configuration, the DRPF may be 5 wrapped around such that it completely encloses the diffuse source. A sepal~L~- reflector may be used in addition to the light source and DRPF. The reflector may be a diffuse reflective film (DRMF) which r~n~ mi7~s the light of polarization (b) that is reflected from the DRPF, or it may be a specular reflector which redirects light to the light emitting region of a diffuse r~n~lomi7ing light source. The D~MF
10 may be oriented around one side ofthe light source and may be l~min~cl or otherwise ~tt~chefl to the light source. In this configuration, the DRPF may also be ed or otherwise :~tt~ch~cl so that it partially enrloses the other side of the light source.
The embodiments of the present polarized light source using the DRPF
5 have several adv~ es. The reflection and r~n~omi7~tion process achieved with the light source and DRPF gives a polarized light fixture that is very efficient The bro~lb~n~1 reflectivity provided by the DRPF means that efflci~ncy is achieved over a broad spectral range. In ~ liti~n, the DRPF provides high off-angle re~ectivity of the rejected polarization. These redL-u~;s make the DRPF/diffuse 20 source combination useful over a broader range of the optical s~e ~ and over a broader range of angles than the embo-lim~nt~ h~c~ OlaLi~g bulk optic co 1ll~ lellL~. In addition, the DRPF is lightweight, thin and flexible, which makes it good for applications requiring low bulk and light weight. The DRPF also conforms well to the larnp surface and could be inco1~o1d~d into the lamp 2s m~nllf~--tllre. Furthermore, since the DRPF is a diffuse reflector, its opaque ~c~allce obviates the need for a s~ diffuser film that is typically used in polarized luminaires and task li~hting fixtures to obscure the light source fromdirect viewing.
In yet another application, optical films of the present invention may be 30 used to gener7~te polarized light used in smoke detection systems or in the analysis of the polarization of light scattered from smoke particles, including those smoke .

WO 97/32230 PCT/U$97/03130 detection systems which attempt to define the nature or origin of the combustion as taught by U.S. S,576,697 ~N~chim~ et al.).

Light Extractors s The optical films of the present invention may be used as light extractors in various optical devices, including light guides such as the Large Core Optical Fiber (LCOF) ill11~tr~t~1 in FIG. 8. The LCOF 50 uses very efficient total intern~1 reflection (TIR) to guide light ~ es from an illllmin~r or light source 52. However, when the optical films of the present invention are applied as an e~tt~rn~1 r~ kling 54, they upset the light guiding at the fiber-to-air int~ e7 thereby ejecting light out into the ~ o~ tingc This feature may be used advantageously in various remote source 1ighting applic~tionc~ such as arc1~ifPctl1r~1 high1ighting decoldliv~; 1ighting, mP.lic~ htin~, ~ign~ge, visual g~ n~e (e.g., on landing strips or in aisles for airplanes or ~ledlles), display (e.g., m~ t l 5 displays, especially those in which ~ ce "ive heating is a problem) and exhibit 1i~htinf~ roadway liphtin~, automotive 1ighting, down1ighting~ task 1ight;ng, accent 1i~hting and ambient 1i~htinp In some a~ 1ic;~ n~, the films ofthe present invention may be applied as a c1~A~ing at mn1tir1e locations along the length of the fiber, thereby i11l....i..i.1;.,~ m111tiple locations from a single light source.
20 Fu~ . . .ore, since these systems are commonly equipped with W and IR filters, the 1ightin~ produced by suc_ systems will not (1e r~Clp W sel~iLiv~; m~t~ri~1c, nor will the light guides heat up with use.
The films of the present invention can atso be made to extract only a single pot~ri7~tion of light, thereby cled~ g a po1~li7~tion-specific source. With proper 25 cnnfi~nr~tion of the light fiber system, sllhst~nti~lly all of the light injected into the fiber will eventually make its way through the ~xtr~ctor in the desired pol~ri7~tiQn.
pol~ri7~tion-specific sources can be made, for Px~mrle, by using an optical film of the present invention which is a strong diffuse ~c~U.,~ for light of a first polarization, but is a non-sc~ttering, specular m~t~ri~1 which ", ~ a total 30 int~rn:~1 reflection (TIR) c~ lin~-to-surface int~ ce for light of a second po1~ri7~tion ~uch a system is described in Example 134.

Suitable light guides for use in the present invention include both side emitting and end emitting fibers. The light guides themselves may be glass or plastic and may be of varying diameters, depending on such factors as the required efficiency at collecting light, required flexibility, and whether the light guides are s to be used alone or in bundles. The light guides may also be fiber optic lightguides or prism light guides, with the later being more suitable for large scaleapplications, and the former being more suitable for smaller scale applications where cost per lumen is less ill~polL~lL.
Commercially available light guides that are suitable for use in the present 0 invention include those made from films of low Tg acrylic polymers, such as the optical lighting film available commercially from 3M under the trad~n~me Scotch Optical T.i~hting Film (SOLF). Such film, which acts like a mirror towards lightstriking it at certain angles, is a ~ .lL plastic film which has a prismaticsurface (tvpically microreplicated) on one side and a smooth surface on the other.
15 The film is commonly used in conjunction with a tubing or b~rl~ing of a L~ L or opaque plastic or metal. Other suitable light guides include the linear illl..n;..;1l;on fiber optics available c~ mm~rcially from LulllellyL~ under the tr~ n~m~ Fib~escenLTb'', and the end-emitting fibers available commercially fromFib~ under the ~ n~m~? FiberSpotsTM.
Various light sources may be used in COllj u~ ion with the light guides made in acco.~ ce with the present invention, depending on the application to which the light guide is directed. Such sources are described, for example, in T jghtin~ Futures. Vol. 1, No. 3 (1995), apublication ofthe T.ightin~ Research Center, P~n~ or PolyLI;c~ ic Tn~tih-te, Troy, N.Y. Typically, a low voltage 20-2s 75 watt MR16 lamp used in conj ul. ;lion with a fiber optic system will be suitable for applications such as m~lsellm, display and accent lighfing, while a 70-250 watt metal halide lamp, used in COllj u~ ion with a fiber optic or prism light guide system, is suitable for appli~ti- n~ such as ~ ,h;~ l or outdoor ligh~ing applications. For applications requiring 250 watts or greater, metal halide or high 30 ~l~,S~ulC sodium lamps may be used in cuju,-~ Lion with prism light guide systems.
Other suitable light sources include 60 watt xenon metal halide lamps, cornmercially available from General Electric Company, Danbury, Connecticut, which are particularly useful for automotive applications, and sulfur lamps, commercially available from Fusion T.ighting, Rockville, MD, which have been used s~l~cçccfully on an c~e~ l basis in prism light guide sy~Ls~ s. Compact 5 and tubular fluol~;,cclll lamps may also be used where a larger diffuse light source is needed. Sunlight may also be used with fiber optic or prism light guide systems, and in conju~ ion with mirrors or lenses, as part of a s~lnlight harvesting system.
In some b~ lighf display devices, such as those used in avionics applications where high levels of ambient light impinge on the front surface of the 10 device, high; . . ~ i l ;çs rar1i~ting from the display are required to provide sllfficiPnt contrast to the display. Collse4u~ Lly, excessive heating of the b~r~light assembly in such ~y:ilt;llls can occur unless means are provided to dissipate the unwanted heat. A variety of means are used in the art to el; . . .; . .~ the heat, such as the use of cold mirrors and filters and other means.
In most new aircraft, ambient sllnlight potentially reduces cc.. l~ l to the flat panel displays used, and spatial lc L~ clllents for the ~n.c.omhle of displays are critical desgin ~dlll~,t~ . Th_.crof~, in one form of the present invention, light is Lla~ d to the display(s) via fiber optics from a remotely located, but intense, source, where the latter can be cooled efficiently and the undesired heat not affect 20 the operation of the display device. Since these displays typically work on the basis of pol~ri7~cl light prop~ting through a liquid crystal display, the optical films of the present invention may be used in such systems as light ~=~ cLo- ~ of sllhst~nti~l Iy one pol~ri7~tinn The second polarization would cc,. .1 i . .. ~5 to reflect inside the optical fiber until its polarization is coll~.Lcd to the first polarization 25 and can be emitted fiom the light ~ ol at the places where the light is needed.

Overview of FY5'~-~
The following F~mples illustrate the pro~ ctiQr~ of various optical m~tPri~lc in accoldance with the present invention, as well as the spectral 30 pl. l-ellies of these m~tPri~lc Unless otherwise in-lic~ted, percent composition refers to percent composition by weight. The polyethylene n~phth~l~t~ resin used CA 022465i5 1998-08-17 was produced for these samples using ethylene glycol and dimethyl-2,6-n~phth~lenf ~lic~rboxylate~ available from Amoco Corp., Chicago, IL. These reagents were polymerized to various intriILsic viscosities (IV) using conventional polyester resin polymeri7~ti-~n techniques. Syndiotactic poly~LylGlle (sPS) may be s produced in accordance with the method disclosed in U. S. Patent 4,680,353 (T.chih~r~q et al). The examples inc1u<1f~s various polymer pairs, various fractions of continuous and disperse phases and other additives or process c,h~ng~s as discussed below.
SLleLcl~illg or orif ntinE~ of the s~mp1es was provided using either 0 conventional orient~tion equirmfAnt used for making polyester film or a laboratory batch orienter. The labolatc"~ batch ol;~l.L. used was ~leei~nf~(l to use a small piece of cast mAtf~ri~l (7.5cm by 7.5cm) cut from the extruded cast web and held by a square array of 24 ~5l ;p~ (6 on each side). The orientation 1~ i of the sample was controlled a hot air blower and the film sample was oriented through a mf ~h~nic~l system that increased the ~ tAn~e b~ en the ~ in one or both directions at a controlled rate. SAmples stretched in both directions could be orif ntfAcl sequentially or ~imn1t~n~ously. For s~mrles that were oriented in the CCI~ ;llf~fl mode (C), all g~ Cl~ hold the web and the ~ move only in one ~liml~n~ion Whereas, in the L~l~consLI~i~ed mode ~U), the ~ that hold the film at a fixed ~1;~ ion perpendicular to the direction of stretch are not eng~ged and the film is allowed to relax or neckdown in that .1; " ~ iOn Polarized diffuse frAn~mie~ion and reflection were l"easu,~d using a Perkin Elrner r.~mh-l~ 19 ultraviolet/visiblelnear infrared spe~ hoL~"~ ~l equipped with a Perkin Elmer r s~bsph~re S900-1000 A 50 millimfAtfAr ;..1~ g sphere 2~ accessory and a Glan-Thollll,soll cube polarizer. Parallel and crossed tr~n~mi~ion and reflection values were measured with the e-vector of the polari~d light parallel or perpf n~lic~ r, respectively, to the stretch direction of the film. All scans were continuous and were conrlllcte~l with a scan rate of 480 nAnO~ I If t' ~ ~i per minute and a slit width of 2 nanometers. Reflection was ~e-ru-llled in the "V-reflection"
30 mode. Tr~n~mi~ion and reflect~n~e values are averages of all wavclf n~ s from 400 to 700 n~n~mf tf-r~

TrAn~mi~.eion electron micrographs were taken of fini.chP~l filrn, cross-sectioned in a plan perpendicular to the ~llacl~ine direction to ~letPrminp the nature of the dispersed phase. The outer layers of three-layer constructions were removed from oriented film7 leaving only the blend layer for embedding. Samples were s embedded in 3M ScotchcastTM S Electrical Resin which was cured at room le~ dL~t;. The embedded samples were microtomed using a diamond knife, on a Reichert UltracutTM S microtome at room temperature, into thin sections of ~lo~imately 90nm thirl~nP~, using a cutting rate of 0.2 mill;...r.tf.. s per second.
The thin sections were floated onto ~li.ctillP~l, deionized water and collected for 0 t~n.~mi.c~ n electron microscopic evaluation on a 200 mesh copper grid le;l~fo~ced with a carbon~rol.slvol ~ub~L.dLe. Photomicrographs were taken using a JEOL
200CX TrAn~mi~eion Electron Microscope.
Sc~ electron microscopic evaluations were ~t;lrolllled on cast webs prior to film c,~;c~ Lion to ~ P the nature of the disperse phase. Pieces of15 web were ~ d to expose a plane ~ l;r,~ r to the .,~Ach;..~ direction while i.... ~. ~ed in liquid nitrogen. ~Ample~ were then 1. ;.. I-~d and mounted on ~II,ilstubs prior to sputter coating with gold p~ m. Photomicrographs were taken using a Hitachi S530 Sc~nnin~ Electron Microscope.

In Example 1, an optical film was made in accordance with the invention by extruding a blend of 75% polyethylene ,.;~p~ t~ (PEN) as the continuous or major phase and 25% of polyl,~lhyl~ rylate (PMMA) as the ~ per.ce or minor phase into a cast film or sheet about 380 microns thick using conventional 2s extrusion and casting techniques. The PEN had an intrin~ic viscosity (IV~ of 0.52 (measured in 60% phenol, 40% dichlorol~c.~el~). The PMMA was obtained from ICI Americas, Inc., Wilmin~tol-, DE, under the product ~le~i~n~tion CP82. The extruder used was a 3.15 cm (1.24") Brabender with a 1 tube 6(~ ~lm Tegra filter.
The die was a 30.4 cm (12") EDI UltraflexTM 40.
About 24 hours after the film was extruded, the cast film was oriented in the width or transverse direction (TD~ on a polyester film tent~rinf~ device. The -s8-chillg was accompli~hed at about 9.1 meters per minute (30 ft/min) with an output width of about 140 cm (55 inches) and a stretching ~ ;lalulG of about 1 60~C (320~F). The total reflectivity of the stretched sample was measured withan integrating sphere at~chmpnt on a Lambda 19 spectrophotometer with the s sample beam polarized with a Glan-Thompson cube polarizer. The sample had a 75% parallel reflectivity (i.e., reflectivity was measured with the stretch direction of the film parallel to the e-vector of the polarized light), and 52% crossed reflectivity (i.e., reflectivity was measured with the e-vector of the polarized light perpendicular to the stretch direction).

In Example 2, an optical film was made and evaluated in a manner similar to F.x~mple 1 except using a blend of 75% PEN, 25% syndiotactic poly~yl~,ne (sPS), 0.2% of a poly~lyl~,.le glycidyl mPth~rrylate col~ Libilizer, and 0.25% each of IrganoxTM 1010 and UltranoxTM 626. The synthesis of polystyrene glycidyl c~rlate is described in Polymer Processes, "Chemical Technology of Plastics, Resins, Rubbers, Adhesives and Fibers", Vol. 10, Chap. 3, pp. 69-109 (1956)(Ed.
by Calvin E. Srhil-lkn~cht).
The PEN had an in~in~ic viscosity of 0.52 measured in 60% phenol, 40%
20 dichlorobel.~Glle. The sPS was obt-ained from Dow Chemical Co. and had a weight average molecular weight of about 200,000, ~e~i~nZltcc~ ~ul~se~ e~l~ly as sPS-200-0.
The parallel reflectivity- on the ~lletclled film sample was ~let~.. ,--;--e(l to be 73.3%, and the crossed reflectivity was tiPt~ - ."i,.Ptl to be 35%.

In Example 3, an optical film was made and evaluated in a manner similar to Example 2 except the compatibilizer level was raised to 0.6%. The res-l1ting parallel reflectivity was (let~nninP~l to be 81% and the crossed reflectivity was ~tPrminP~1 to be 35.6%.
~ 30 _59_ In Exarnple 4, an three layer optical film was made in accordance with the present invention ntili7in~ conventional three layer coextrusion techniques. Thefilm had a core layer and a skin layer on each side of the core layer. The core layer consisted of a blend of 75% PEN and 25% sPS 200-4 (the ~ n~tion sPS-200-4 refers to a copolyrner of syndiotactic-poly~lyl~ lle c- nt~inin~ 4 mole % of para-methyl styrene), and each skin layer consisted of 100% PEN having an intrinsic viscosity of 0.56 mea~u~ed in 60% phenol, 40% dichlorob~n7~nf The rçs-lltin~ three-layer cast film had a core }ayer thickness of about 415 0 microns, and each skin layer was about 110 microns thick for a total thickness of about 63~ microns. A labo,dlv.y batch stretcher was used to stretch the res~-hin~
three-layer cast filrn about 6 to 1 in the m~rhint? direction (MD) at a te~ alu~e of about 129~C. Rec~ the edges ofthe filrn sample parallel to the stretch directionwere not gripped by the lab ~ tchc., the sample was u~lco~ l in the L~ ,e direction CI D) and the sample necked-down in the TD about 50% as a result of the stretch procedure.
Optical y~r~l~la lce was evaluated in a lll~lllC- similar to Example 1. The para}lel reflectivity was A~t~ 1 to be 80.1%, and the crossed reflectivity was 7 to be 15%. These results f~ le that the film l ."roLms as a low absorbing, energy C~ mg system.

In Fx~mp!~s 5-29, a series of optical fflms were produced and evaluated in a manner similar to Exarnple 4, except the sPS fi ~r.ti~)n in the core layer and the IV
of the PEN resin used were varied as shown in Table 1. The IV of the PEN resin in the core layer and that in the skin layers was the same for a given sample. The total thickness of the cast sheet was about 625 microns with about two-thirds ofthis total in the core layer and the balance in the skin layers which were approximately equal in thickn~$~ Various blends of PEN and sPS in the core layerwere produced, as indicated in Table 1. The films were stretched to a stretch ratio of about 6:1 in either the m~hine direction (MD) or in the transverse direction (TD) at various lC~lllpt;ldLUl'eS as in-lir~te~l in Table 1. Some of the samples were co~ Lldi led (C) in the direction perpendicular to the stretch direction to prevent the sample from ner~ing down during stretchin~ The sarnples labeled "U" in Table 1 were unconstrained and perrnit~e~l to neckdown in the unconstrained ~iimencion.
5 Certain optical ~rop~ ies of the stretched sarnples, including percent LL~ ion, reflection, and absorption, were measured along axes both parallel and crossed or perpçn-lic~ r to the direction of stretch. The results are snmm~ri7~1 in TABLE 1.
Heat setting, as indicated for Fx~mples 24-27, was accom~ hed by m~ml~lly c~ g the two edges ofthe stretched sample which were lo perpendicular to the direction of stretch by clamping to an dp~l~,pl;ately sized rigid frame and placing the clamped sample in an oven at the inL~ic~tPd tcln~aL~LL~ for 1 minute. The two sides of the sarnple parallel to the direction of stretch were ullcn- -~ or not cl~mpeci and allowed to neckdown. The hp~t~etting of FY~mple 29 was similar except all four of the edges of the stretched sample were5 c.J..~Ir.~ fl (C) or cl~mre~l Example 28 was not heat set.

-. _~
~d ~ o oo ~ ~ ~ oo 1~ ~ O ~ ~ O 1~

c~ O ~ oo ~ 00 ~ ~ O ~ ~--u~ ~
- x c oooooooooo~~~

L~ ;> 'n '~ ~ ~ ~ ~ ~ ~ ¢ 't ¢ ~ ~t ~ o o o o o o o o o o o o o ~.c C,) ~ ) V C~) ~ ;~ ~ ~ 3 =

.s o Q
~ ~ ~ a ~ ~ ~ a ~ ;Q~ ~Q~
U~-fi ~

~, x C~S o o o o~i ~ ~ ~ ~ ~o ~s a~ ~ o o u~ ~o ~-- ~ ~ e~ Oo .~ ~ ~ ~) 3 ~

V~ ~ o o ~ 'f- ~ o o ~ ~~ t~-~ t~ , t~
G o o o o o o o o o o o o o tf~ t~ ' t~ t~ ~t t~ t~-t V'~ t~-~ t~'~
C~ ~ O O O O O O O o O O O O O
--' t ~ ,_ o E--x ~ ~~ ~ ~ ~ ~ ~ ~ ~ ~
~ z All of the above samples were observed tO contain varying snapes of tne disperse phase depending on the location of the disperse phase within the body of the film sample. The disperse phase inclusions located nearer the surfaces of the samples were observed to be of an elongated shape rather than more nearly 5 spherical. The inclusiorls which are more nearly centered between the surfaces of the samples may be more nearly spherical. This is true even for the sarnples with the skin layers, but the m~gnit~lde of the effect is reduced with the skin layers. The addition of the skin layers improves the processing of the films by reducing thetendency for splitting during the stretching operation.
Without ~,vishing to be bound by theory, the elongation of the inclusions .-(disperse phase) in the core layer of the cast film is thought to be the result of shear on the blend as it is transported through the die. This elongation feature may be altered by varying physical dimensions of the die, extrusion te.l~p~.dlllres, flow rate of the extrudate, as well as chemical aspects of the continuous and disperse phase materials which would alter their relative melt viscosities. Certain applications or uses may benefit from providing some elongation to the disperse phase during extrusion. For those applications which are subsequently stretched in the n~ hin~
direction, starting with a disperse phase elongated during extrusion may allow ahigher aspect ratio to be reached in the resulting disperse phase.
Another notable feature is the fact that a noticeable improvement in performance is observed when the same sample is stretched unconstrained. Thus, ~ 3 in Example~the % tr~ncmiccion was 79.5% and 20.3% in the parallel and perpendicular directions, lea~e~,lively. By co~ l, the tr~ncmicsion in Example l~was only 75.8% and 28.7% in the parallel and perpendicular directions, 25 ~ ecli~ely. There is a thickness i~. -ease relative to cons~ained ~LL~ lching when samples are stretched unconstrained, but since both tr~n~mi~sion and extinction improve, the index match is probably being improved.
An alternative way to provide refractive index control is to modify the chemistry of the materials. For example, a copolymer of 30 wt % of 30 interpolymerized units derived from terephthalic acid and 70 wt % of units derived from 2,6-n~phth~lic acid has a refractive index 0.02 units lower than a 100% PEN

~MEND~D SH~~

~ CA 02246545 1998-08-17 polymer. Other monomers or ratios may have siigh~ly di~ferent Ies~s. This typ~
of change may be used to more closely match the refractive indices in one axis while only causing a slight reduction in the acis which desires a large difference.
In other words, the benefits attained by more closely matching the index values in 5 one axis more than compensate for the reduction in an orthogonal axis in which a large difference is desired. Secondly, a chemical change may be desirable to alter the te1,lpeldture range in which stretching occurs. A copolymer of sPS and varying ratios of para methyl styrene monomer will alter the optimurn stretch-te.llp~ .aL.lle range. A combination of these techni~ues may be t rC~ A. ~r to most effectively lo optimize the total system for ploce~ing and res111tin~ refractive index mzt~h.~s and di~.ences. Thus, an improved control of the final ~c..ro~ ce may be ztttztinecl J by opti.,.i~;n~ the process and çh ~rni~y in terms of stretching conditions and further adjusting the chemistry of the materials to maximize the difrtl~i~ce in refractive index in at least one axis and minimi7ing the difference at least one orthogonal axis.
These samples displayed better optical perf~a~cge if oriented in the MD
rather than TD direction (compare Examples ~ Without wishing to be bound by theory, it is believed that different geometry inclusions are developed with an MD orientation than with a TD orientation and that these inclusions have higher aspect ratios, making non-ideal end effects less important. The non-ideal end effects refers to the complex geometry/index of refraction relationship at the tip of each end of the elongated particles. The interior or non-end of the particles are thought to have a ul~r~ geometry and leL~ e index which is thought to be desirable. Thus, the higher the ~e.~ e.lt~ge of the elongated particle that is uniform, the better the optical ~.rO~ .ce The extinction ratio of these materials is the ratio of the tr~ncmi~sion for polarizations perpendicular to the stretch direction to that parallel to the stretch direction. For the examples cited in Table l, the extinction ratio ranges between about 2 and about 5, although extinction ratios up to 7 have been observed in optical bodies made in accordance with the present invention without any attemptto optimize the extinction ratio. It is expected that even higher extinction ratios A~El\/o~D SH~

. = = = =

WO 97/3~230 PCT/US97/03 130 (e.g., greater than 10~) can be achieved by adjusting film thickness, inclusion volume fraction, particle size, and t_e degree of index match and miqmAtGh, or through the use of iodine or other dyes.

s EXAMPLES 30-100 In Examples 30-100, samples of the invention were made using various mAtt~riA1c as listed in Table 2. PEN 42, PEN 47, PEN 53, PEN 56, and PEN 60 refer to polyethylene n~phth~1Ate having an intrinsic viscosity (IV) of 0.42, 0.47, 0.53, 0.56, and 0.60"~ e.;Livc;ly, measured in 60% phenol, 40% dichlorobt;l~elle.
0 The particular sPS-200-4 used was obtained from Dow Ch~--miç~l Co. Ecdel~M9967 and EastarTM are copolyesters which are available commercially from FAetmAn Ch~mir~1 Co., Rochester, NY. Surlyn~ 1706 is an ionomer resin available from E.I. du Pont de Nemours & Co., Wi7min~on, DE. The m~tRris-lq listed as Additive I or 2 include poly~y.~ lle glycidyl meth~rylate. The 1S deqi~n~tionc GMAPS2, GMAPS5, and GMAPS8 refer to glycidyl m~lhAl lylate having 2, 5, and 8% by weight, l~s~e~iLively, of glycidyl methacrylate in the total copolymer. ETPB refers to the cro~qlinkin~ agent eLhy1f~ h~ ~.yl~hosrhoninm bromide. PMMA V044 refers to a polymethylmt;Lhacl ylate available commercially from Atohaas North America, Inc.
The optical film e~n~p1eq were produced in a m nner similar to Example 4 except for the ~ e.lces noted in Table 2 and ~licc-1qqe-:f below. The continuousphase and its ratio of the tot~ is reported as major phase. The ~iiqp~rsR phase and its ratio of the total is reported as minor phase. The value reported for blend thickness r~ s_nLs the appr~)xim~te? thicknRcq of the core layer in microns. The2s thickness of the slcin layers varied when the core layer thickn~ss varied, but was kept to a con~L~L ratio, i.e., the skin layers were ~I)r~xi~..aLely equal and the total of the two skin layers was about one-third of the total thicknecq The size of the fliqp~rse phase was ~leterrnin~od for some s~ ,1cc by either sç~nning electron microscope (SEM) or ~ . . . iq~ n electron microscope (TEM). Those examples 30 which were subsequently stretched using the laboratory batch orienter are shown by an "X" in the column labeled Batch Stretched.

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CA 02246545 l998-08-l7 The presence of the various compatibilizers was found to reduce the size of the included or disperse phase.

s EXAMPLE 101 In Example 101, an optical film was made in a manner similar to Example 4 except the rçsnlting core thickness was about 420 microns thick, and each skinlayer was about 105 microns thick. The PEN had a 0.56 IV. The cast film was ~rientf?~f as in Example 1, except the te~ lalulc of stretch was 165~C and there10 was a 15 day delay between casting and stretching. The tr~ncmi~c;< n was 87.1%
and 39.7% for parallel and perpendicularly polarized light, lc ,~e~;livt;ly.

In Examples 102 - 121, optical f~rns were made as in Example 101, except 5 that . ,. ;~ nf ;r n conditions were varied and/or the sPS-200-0 was replzl- e I with either copolymers of sPS co~n ;.~ either 4 or 8 mole % of para-methyl styrene orwith an atactic-form of styrene, Styron 663 (available from Dow Chf micsll C~ dlly, Midland, Michigan) as listed in Table 3. Evaluations of lr~ncmic~jon p~ Lies are also reported. Tr~ncmiccion values are averaged over all 20 wavelengths bclw~ 450-700 nm.

Ex. % PS PENTe~ dLu~,Rail Perpendicular Parallel sPS IV of Draw Setting Tl,.~ ion Tr~n.cmi~cion (~C) (cm) (%) (%) 101 25200-0 0.56 165 152 g7.1 39.7 102 35200-0 0.56 165 152 87.8 44.4 103 15200-4 0.56 165 152 86.1 43.5 104 25200-4 0.56 165 152 86.5 43.6 105 35200-4 0.56 165 ~52 88.2 50.7 106 15200-8 0.56 165 152 89.3 40.7 Ex. % PS PENT~ )e~dL~c~Rail Perpendicular Parallel sPS IVof Draw Setting Tr~n~mi~ion Tr~ncmicci~
(~C) (cm) (%) (%) 107 25 200-8 0.56 165 152 88.5 42.8 108 35 200-8 0.56 165 152 88.6 43.3 109 lS Styron0.56 165 152 89.3 45.7 110 25 Styron0.56 165 152 87.8 41.6 111 35 Styron0.56 165 152 88.8 48.2 112 lS Styron0.48 165 152 88.5 62.8 113 25 Styron0.48 165 152 87.1 59.6 114 35 Styron0.48 165 152 86.8 59.6 1 ~S 15 200-0 0.48 165 152 88.0 58.3 116 25 200-0 0.48 165 152 88.0 58.7 117 35 200-0 0.48 165 152 88.5 60.6 118 lS 200-4 0.48 165 152 89.0 57.4 119 35 200-4 0.48 165 152 87.3 64.0 120 35 200-0 0.56 171 127 86.5 65.1 121 35 200-0 0.56 171 152 88.1 61.5 These examples in~lir.ate that the particles of the included phase are elnngat~l more in the m~hine direction in high IV PEN than in low IV PEN. This is con~i~t~nt with the ol)s~.~Lion that, in low IV PEN, ~ ~hi-lg occurs to a 5 greater extent near the surface of ~e film than at points interior to the film, with the result that fibrillar structures are formed near the surface and sphrric ~l sL~u~ s are formed towards the center.

Some of these Examples suggest that the orientation L~ c.d~es and degree of orientation are important variables in achieving the desired effect.
Examples 109 to 114 suggest that quiescent cryst~lli7~tion need not be the only reason for the lack of tr~ncmi~cinn of a preferred polarization of light.
s EXAMPLES l 22~ l 24 In Example 122, a multilayer optical film was made in accordance with the invention by means of a 209 layer feedblock. The feedblock was fed with two mAt~riAlc (1) PEN at 38.6 kg per hour (intrinsic viscosity of 0.48), and (2) a blend lo of 95% coPEN and 5% by weight of sPS homopolymer (200,000 molecular weight). The coPEN was a copolymer based on 70 mole % nAphth~l~n~
di~ b~ ylate and 30 mole % di~ yl isorhthAIAtç po}y..~ d with ethylene glycol to an intrinsic viscosity of 0.59. The coPEN/sPS blend was fed into the feedblock at a rate of 34. l kg per hour.
1S The coPEN blend mAt~riAI was on the outside of the t;~-LI .~d~Lt;, and the layer composition of the resllltin~ stack of layers Alt~rnAtPA b~;LV~ ,n the t~,vo mAteriAlc The thi~l~n~$~$e$ of ~he layers was d~ciPn~cl to result in a one-quA~ter wavelength stack with a linear grAfJiçnt of thict . ~~ ~ses, and having a 1.3 ratio from the Ih;.,.,~ iL to the thi~k~ct layer. Then, a thicker skin layer of coPEN (made in accol.l~.ce with the method ~lçscribed above to make the coPEN/sPS blend, exceptthe molar ratios were 70tlS/l5 ~,~pl.ll,AI~ne dica,l,oxylate /dimethyl tc.~ AIAt~/dh~leLhyl iSu~hll~Al~t~) devoid of sPS was added to each side of the 209 layer con1~osiLe. The total skin layer was added at a rate of 29.5 kg per hour, with about one-half of this 4u~liLy on each side or surface of the stack.
The r~c-lltin~ skin layer clad multilayer composite was extruded through a mnltirlier to achieve a multilayer composite of 42 l layers. The reslllting multilayer composite was then clad with another skin layer of the 70/1 5/l 5 coPEN
on each surface at a total rate of 29.5 kg per hour with about one-half of this 4u~lliLy on each side. Since this second skin layer may not be s~dlely (letectAhle from the ~rieting skin layer (as the mAt~riAl is the same), for the purposes of this ~liecu~cion, the resulting extra thick skin layer will be counted as only one layer.
The rç~nlting 421 layer composite was again extruded through a 1.40 ratio asymrnetric multiplier to achieve a 841 layer film w-hich was then cast into a sheet 5 by extruding through a die and qllenchmg into a sheet about 30 mils thick. Theresulting cast sheet was then oriented in the width direction using a conventional film making tentt~rin~ device. The sheet was stretched at a te~ .dLu.P of about 3Q0~~ (149~C) to a stretch ratio of about G: 1 and at a stretch rate of about 20% per second. The resnlting stretched film was about 5 mils thick.
In Example 123, a multilayer optical film was made as in Example 122, except that the amount of sPS in the coPEN/sPS blend was 20% instead of 5%.
In Example 124, a multilayer optical film was made as in F.x~mI~le 122, except that no sPS was added to the film.
The results reported in Table 4 include a lllea~u~e of the optical gain of the 5 filrn. The optical gain of a film is the ratio of light 1~ 1 through an LCD
panel from a b~cL Ii~ht with the film inserted b.,~wcx:ll the two to the light ;uf~l without the film in place. The ~ignifirzm~e of optical gain in the contextof optical films is described in WO 95/17692 in relation to Figure 2 of that lcr~lcl.ce. A higher gain value is generally desirable. The ~an~mi~ion values 20 include values obtained when the light source was polarized parallel to the stretch direction (TR) and light polarized L)el~,n~licular to tne stretch direction (Tl). Off-angle-color (OAC) was ~ ed using an Oriel ~e-;LIv~ olon~.,t~ as the root mean square deviation of p-polarized lr,ll ,~" . i~ion at 50 degree inci~l?nt light of wavelength bt;Lwt:e~ 400 and 700 nm.
2s Ex.mole % sPSGainTl(%) T~ (%)OAC (%) 122 5 1.5 83 2 1.5 12320 1.45 81 1.5 1.2 124 0 1.6 87 5 3.5 WO 97/32230 rCT/US97/03130 The value of o~f-angle-coior (OAC) demonstrates the advantage of using a multilayer construction within the context of the present invention. In particular, such a construction can be used to substantially reduce OAC with only a modest reduction in gain. This tradeoff may have advantages in some applications. The s values of Tll for the examples of the invention may be lower than expected because light scattered by the sPS dispersed phase may not be received by the detector.

A three layer film was made in accordance with Example 4. The core layer o concicter1 of 70% coPEN ~whose intrinsic viscosity was 0.55 measured in 60%
phenol, 40% dichlorobel.~Glle), 30% sPS 200-7, plus an ~ tio~l 2% Dylark 332-80 (available from NOVA Ch~mic~l). Each skin con~i~tPcl of 100% coPET having an intrinsic viscosity of 0.65 lllea~ ,d in methylene chloride.
The coPEN was a copolymer based on 62 mole % naphth~len~
dicarboxylate and 38 mole % dimethyl ~;phlhAi~te The coPET was a copolymer based on 80 mole % dimethyl carboxylate and 20 mole % dimethyl isophth:~kltt~
The cast film was orient~cl in a manner cn~ with F.x~mple 1. The ~llel~hillg was ~compli~he~i at 5.8 meters per minute (19 feet per minute) with an output width of 147 cm (58 inches). The stretch le~l~p~dLLlle was 124~C. The heat set t~ dlule was 163~C. The perpendicular l~ n was 85.3%, and the parallel tr~n~mi~ion was 21.7%.

The following ex~mplec illustrate the production of a co-continuous morphology in an optical system of the present invention.
In Examples 126 through 130, a series of optical films were produced and evaluated in a manner similar to Fx~mple 125, except the sPS fraction in the core layer and the stretch tel--p~.d~u~e were varied as shown in Table 5.

CA 02246545 l998-08-l7 Example Fraction Dispersed Stretch Trans. Trans.
NumbersPS or Co- Temperature (Perp.) (Para.) continuous (~C) 125 0.30 D 124 85.3 21.7 126 0.35 D 135 86.3 21.1 127 0.40 D 129 86.4 21.9 128 0.44 -- 124 85.8 25.9 129 0.53 C 129 86.6 33.6 130 0.81 D 135 88.1 69 The parallel and perpendicular tr~n~mi~ion values for Examples 125 to 130 show good optical p~lr~.. ~11t~e The high value for perpendicular tr~n~mi~cion for F~z~mple 130 I~ "~ ion sllgge~tc an effective match in the refractive indices in both phases for polarized light aligned in the direction perpenAi~ r to the stretch direction.
SC~ clc~,~oll micrographs were taken of fid~ e sllrf~ s of cast web for Examples 126 and 127. As in F.~mrle 125, there was clear evidence of lo spherical or elliptical particles .~ eA in an otherwise contmuous matrix.
T~ ;on electron micrographs were taken for Examples 129 and 130; these are shown in Figs. 6a and 6b, l~,~pe~ ly. Fig. 6a illll~tr~t~e the morphology ofco-continll~ us phases. Inspection of the micrograph shows inclusions of both the coPEN and the sPS phases, as well as regions where each appears to be the Cl~ US phase. By collLId~l, Fig. 6b shows coPEN dispersed into an sPS matrix.

A three layer film was made in accordance with Example 4. The core layer con~i~teA. of 85% coPEN whose i.~ ;c viscosity was 0.51 measured in a solu~ion of 60% phenol and 40% dichlolobell~elle, and 15% 250k-7, plus an Aitio~ 2% DylarkTM 332-80. Each skin consisted of 100% coPEN.
The coPEN used as part of the core was a copolymer based on 70 mole %
n~phth~l~nr dicarboxylate and 30 mole % dimethyl terephth~l~te The coPEN

used in the skin layers was a copolymer based on 70 mole % ~rhth~lene dicarboxylate and 30 mole % dimethyl iso~hth~l~t~
The cast film was oriented in a manner consistent with Example 1. The ,Lcllillg was accomplished at 5.3 meters per minute (17.4 feet per minute~ with an output width of 124.5 cm (49 inches). The stretch ~ ldLUlC: was 118~C. The ~ heat set t~ ;.dL lre was 141 ~C. The perpendicular tr~n~mi esion was 81.9%, and the parallel trAn~mi~eion was 32.7%. The perpendicular tr~nemiesion spectrum is ~l~sellled in Figure 7.

A film with an antireflection layer was ~l~aled by first adding 10 grams of RemetTM SP-30 (Remet Coporation, Chadwicks, NY) with 1 gram TritoxTM X-10û
(Rohm and Haas, Phil~-lçlrhi~, PA) into 89 grams of <leic~ni7~rl water. The solution was coated onto a piece of film from Example 131 utili7in~ a *3 wire 5 wound rod to yield a dry coating thic~kn~ce of a~l)ro~ alely 200 nanol.,te~. The perpendicular tr~n~emi~eion was 83.8%, and the parallel trAnemie~ion was 33.3%.

F.xAmple 131 was repe~t~?~l, except that both sides of the film were coated with an antireflection layer. The perpendicular tr~n~mieeion was 86.2%, and the parallel LL~ --ic~;on was 33.8%.
The perp~n-lic~ r L~ e~ n spectra for Examples 131-133 are ~.cse--lt;d in Fig. 7. One can see from Fig. 7 that the overall slope of the perpendicular trAnemieeion as a function of wavelength is lower for F.x~mpleq 132-133 relative to E~ample 131, particlllarly for the range of wavelength from 450 nm to 700 nm.
One skilled in the art will a~pl~,idl~ that a filrn exhibiting a flat trAnemie~it n curve as a function of the wavelength of light will . . .; . . i . . . i ~ any ch~n~es in color to a rçel~ltAnt display device into which the reflective polarizer might be inco-~o.al~:d.

CA 02246545 l998-08-l7 These examples illll~tr~tes the use of the films of the present invention as high efficiency light extractors for light guiding structures.
In Fx~mple 134, an optical film was made in accordance with the present invention by extruding a composition con~i~t;n~ of 30% sPS in a matrix of 70/30/0 coPEN. The extruded film was oriented in the m~hinP direction to a stretch ratioof 2.5:1.
In Example 135, a second film was made from the same composition as o Example 134 and using a similar procedure. However, instead of ~)rientin~ the film in the ...~.h;..ç direction, the film was oriented lmi~ lly in the direction L~ v~ to the,, ,~ i "e direction using a tenter stretch of 4.8 :1.
The films of Examples 134 and 135 were m~c1~ ic~1ly f~ten~ as çl~ ing to s~,~ optical fibers, using a silica grease to elimin~te the fiber-air int~?rf~ce.
15 The ~;x~..,~;...~ .,1~l set-up is clPpicted sch~-rn~tic~lly in FIG. 8. The fibers were then co~ l to a 60 watt xenon metal halide short arc lamp obtained from (~ner~l Electric Co.ll~.y, Danbury, CT. The optical fibers had a thi~knPc~ of 1.2 cm andcoll~isLed of a low Tg acrylic polymer.
When the lamp was tumed on, the two samples became illnmin~t~l and 20 produced diffusely sc~Lt~ ~d light. When the two film ~mpl~s were viewed through a polari_ing film at an ori~nt~t;cn perpendicular to one plane of pol~ri7~tion, both samples a~e~ued subst~nti~lly rl~rk~n~l However, when the pol~ri7ing film was rotated 90~ in the same plane, both samples a~pcaL~ed diffusely bright, in-1ic~ting that the tr~n~mi~inn of light Lhlvu~ll the films was pol~ri7~tion 2s specific.
The effect of capping the ends of the fibers was also invesfig~tell When the ends were reflectively capped so that a portion of the light escaping from the ends of the fibers was reflPctecl back into the fibers, the hll~nsily of light produced by the films increased. This is con~i~t~nt with the creation of a light cavity in 30 which light of the non-extracted polarization undergoes further reflPction~ within the optical fiber until it is converted, by degrees, into the extracted polarization.

CA 02246545 l99X-08-17 WO 97/32230 PCT/US97/~)3130 With the light within the fiber being unable to exit the fiber except through the extractor, the extraction eff~ciency increased. In addition, polarization conversion of the light interacting with the fiber/air interface caused a greater portion of light to be extracted from the fiber in the desired polarization.

The following ç~c~mple illustrates the increase in gain achievable at non-normal incident angles with the optical fi~ms of the present invention.
A three layer film was made in accordance with Example 4. The core layer con~i~tec~ of 70% PEN whose in~tnn~ic viscosity was 0.48 (measured in 60%
phenol, 40% dichlorobenzene) and 30% sPS 200-8. Each skin consisted of 100%
coPEN and co.~ eci about 17% of the total thickness of the cast film.
The coPEN was a copolymer of 70 mole % ~phth~l~n~ dicarboxylate and 30 mole % dimethyl isophth~l~t~ The viscosity of the coPEN was not measured.
The cast film was oriented in a l~ lllC~ co~ x~ with Exarnple 1. The stretching was accompli~hP~l at 5.5 meters per minute (18 feet per minute) with an output width of 141 cm (55.5 inches). The stretch lt~ Glalu~c was 154~C. The heat set ~en~c~alul~ was 164~C. The rçsnlt~nt film was 128 micrometers thick.
A Sharp C12P b?c~light was placed against the one face of a standard 20 dichroic polarizer. The illL~ ily of the light r?~ ting from the b~r~light/polarizer assembly was measured using a Photo lcsealcll PR650 Spectra Colorimeter. The b~ct~light/polarizer assembly is oriented relative to the detector of the PR650 prior to the start of the mea~ulc;-llelll such that the plane c~ .; . Ig the arc swept by the detector arm also cOllLhills the axis of high tr~n~mi~sjon for the polarizer. The 2s ~le~;Lvl arm is swept plus and minus 60 degrees about a direction perpendicular to the b~r~ ht/polarizer assembly. A second hlL~ iLy mea~ul~ lclll was made with piece of film 23 cm s~uare placed between the b~ ht and the polarizer such that the perpendicular ~ axis of the film was coin~ nt with the high on direction of the polarizer. The ratio of the two i rl l P~ ies for each 30 angular position with the optical film in place to that without is reported as the Relative Gain.

The data for Example 136 is shown in Figure 9A. The average relative gain at the angles plus and minus 60 degrees from the normal was 1.45. This data demon~ tGs that the relative gain for the film of Fx~mple 136 increases at non-normal incic~çnt angles, particularly for angles from 30~ to 60~ away from normal 5 incidence.

The following example ill~ Ps the decrease in gain at non-normal incident angles for a typical commercially available optical film.
A piece of microreplicated hri~htn~e5 ~-nh~nr,rmrnt film from Sekisui W518 (Osaka, Japan) was measured using the Eldim 120D as rlt-srrihe~7 in Fx~mple 136. The ratio of the i~ ;es for each angular position with the Sekisui W5 18 film in place to that wit_out the Sekisui film is shown as Figure 9B.
The average relative gain at the angles plus and minus 60 degrees from the normal 15 was 0.65, in-lir,~tin~ that the gain for the film peaks at normal inc~ ?nce and ~lerlin.os for all angles away from normal inc~ nr-e As demo.~ cl by Example 136 and CO~..P~ ;VG Example l, films can be made in acco~ ce with the present invention in which the relative gain hl~i~Gases at non-norrnal in~ nt angles, particularly for angles from 30~ to 60~away from normal inrirlrnre By co~ ;l, the relative gain for col,.m~ ially available optical filrns typically peaks at normal incicllonre and dçrlin~s for all angles away from normal inciclPnre This feature of the films of the present invention make them particularly advantageous for use in applications such as hrightn~es enh~ncçn~nt films for large displays, where one will likely view the display across a wide range of angles.

The following examples further illustrate the increase in gain at non-normal angles of incidence achieved with the films of the present invention.
A series of examples were made in a manner similar to Example 136, except that nn~t.ori~l and process changes were made as inAi~t~fl In some of the -8~

WO 97132230 PCTrUS97/03130 exarnples, IrganoxTM 1425 antioxidant (available from Ciba Geigy) and/or DylarkrM
332-80 (available ~om NOVA Ch~?mic~i~) were added. The average relative gain for the angles plus and minus 60 degrees from the normal as well as the relativegain at nonnal incidence (0 degrees) are reported in Table 6.
s ~ TABLE 6 Ex. sPS % % Stretch HeatRelativeRelative IrganoxDylark Temp. Set Gain Gain 1425 Temp. (0~) ~+/- 60~) 137 30%, 0 0 160 164 1.18 1.40 138 30%, 0 0 154 199 1.21 1.48 139 30%, 0.5 2 154 199 1.20 1.46 140 30%, 0 2 154 199 1.18 1.47 141 15%, 0.5 0 154 199 1.15 1.48 142 15%, 0.5 0 154 199 1.21 1.47 143 30%, 0 0 154 199 1.16 1.47 144 30%, 0.5 0 154 199 1.29 1.47 145 30%, 0.5 0 154 199 1.06 1.35 146 30%, 0.5 2 154 199 1.13 1.43 147 30%, 0.5 2 154 164 1.21 1.47 148 30%, 0 2 154 164 1.17 1.47 149 15%, 0.5 0 154 164 1.21 1.47 150 30%, 0 0 154 164 1.23 1.38 The ~l~ce~ description of the present invention is merely illustrative, 10 and is not int~nrle~l to be limitin~. Therefore, the scope of the present invention should be construed solely by reference to the appended claims.

-8s-

Claims (41)

What is claimed is:

1. An optical device comprising a light guide and a light extractor as an optical body (10), said light extractor comprising:
a polymeric first phase (12); and a second phase (14), disposed within said first phase, which is discontinuous along at least two of any three mutually perpendicular axes;
wherein said first and second phases have indices of refraction which differ along a first axis by more than about 0.05, and which differ along a second axis orthogonal to said first axis by less than about 0.05.

2. The device of claim 1, wherein said first phase (12) has a birefringence of at least about 0.1.

3. The device of claim 1, wherein said first phase (12) has a birefringence of at least about 0.15.

4. The device of claim 1, wherein said first phase (12) has a birefringence of at least about 0.2.

5. The device of claim 1, wherein said second phase (14) has a birefringence of less than about 0.02.

6. The device of claim 1, wherein said second phase (14) has a birefringence of lees than about 0.01.

7. The device of claim 1, wherein said second phase (14) has an index of refraction which differs from said first phase by more than about 0.1 along saidfirst axis.

8. The device of claim 1, wherein said second phase has an index of refraction which differs from said first phase by more than about 0.15 along said first axis.

9. The device of claim 1, wherein said second phase has an index of refraction which differs from said first phase by more than about 0.2 along saidfirst axis.

10. The device of claim 1, wherein said second phase has an index of refraction which differs from said first phase by less than about 0.03 along said second axis.

11. The device of claim 1, wherein said second phase has an index of refraction which differs from said first phase by less than about 0.01 along said second axis.

12. The device of claim 1, wherein at least about 5% of light of a first polarization is diffusely extracted by said extractor.

13. The device of claim 1, wherein at least about 50% of light of a first polarization of light is diffusely extracted by said extractor.

14. The device of claim 1, wherein at least about 70% of light of a first polarization is diffusely extracted by said extractor.

15. The device of claim 1, wherein said first phase comprises a thermoplastic resin.

16. The device of claim 15, wherein said first phase comprises a polymer derived from naphthalene dicarboxylic acid.

17. The device of claim 16, wherein said polymer is a copolymer of at least one diol and a monomer selected from the group consisting of naphthalene dicarboxylic acid, isophthalic acid, dimethyl isophthalic acid, terephthalic acid, and dimethyl terephthalic acid

18. The device of claim 1, wherein said second phase is a syndiotactic vinyl aromatic polymer derived from a vinyl aromatic monomer.

19. The device of claim 16, wherein said second phase comprises interpolymerized units of syndiotactic polystyrene.

20. The device of claim 1, wherein said first phase comprises a polymer derived from naphthalene dicarboxylic acid and said second phase comprises syndiotactic polystyrene.

21. The device of claim 1, wherein said extractor is stretched to a sufficient stretch ratio, and at a sufficient temperature, so that it extracts predominantly only one polarization of light.

22. The device of claim 1, wherein said second phase comprises a plurality of elongated masses whose major axes are substantially aligned along acommon axis.

23. The device of claim 1, wherein said second phase is present in an amount of less than about 5% by volume relative to said first phase.

24. The device of claim 1, wherein said disperse phase is discontinuous along any three mutually perpendicular axes

25. The device of claim 1, wherein the extracted electromagnetic radiation is distributed anisotropically about the axis of specular transmission.

26. The device of claim 1, wherein said extractor is stretched in at least one direction, wherein at least about 40% of light of a first polarization is diffusely transmitted through said optical body, and wherein said diffusely transmitted rays are distributed primarily along or near the surface of a cone whose surface contains the spectrally transmitted direction and whose axis is centered on the stretch direction.

27. The device of claim 1, wherein said second phase comprises elongated inclusions whose axes of elongation are aligned in a common direction,wherein said extractor is stretched in at least one direction, and wherein the diffusely transmitted portion of at least one polarization of electromagnetic radiation is distributed primarily along or near the surface of a cone whose axis is centered on the axis of elongation direction and whose surface contains the diffusely transmitted direction.

28. An official device comprising a light guide and a light extractor said light extractor film wherein at least one layer in said film comprises:
a continuous phase;
a disperse phase disposed throughout said continuous phase, said disperse phase having an index of refraction which differs from the index of refraction of said continuous phase by greater than about 0.05 along a first axis; and a dichroic dye.

29. The device of claim 28, wherein the disperse phase has an index of refraction that differs from the index of refraction of said continuous phase by less than about 0.05 along a second axis orthogonal to said first axis.

30. The device of claim 28, wherein said dichroic dye is disposed within said disperse phase.

31. An optical device comprising a light guide and a light extractor L.P 86 > comprising:
a first phase having a birefringence of at least about 0.05; and a second phase, disposed within said first phase;
wherein the absolute value of the difference in index of refraction of said first and second phases is .DELTA.n1 along a first axis and .DELTA.n2 along a second axis orthogonal to said first axis, wherein the absolute value of the difference between, .DELTA.n1 and .DELTA.n2 is at least about 0.05, and wherein the diffuse reflectivity of said first and second phases taken together along at least one axis for at least one polarization of electromagnetic radiation is at least about 30%.

32. The device of claim 31, wherein the absolute value of the difference between .DELTA.n1 and .DELTA.n2 is at least about 0.1.

33. The device of claim 31, wherein said first phase has a larger birefringence than said second phase.

34. The device of claim 33, wherein the birefringence of said first phase is at least 0.02 greater than the birefringence of said second phase.

35. The device of claim 33, wherein the birefringence of said first phase is at least 0.05 greater than the birefringence of said second phase.

36. The device of claim 31, said optical body having a plurality of layers wherein at least one of said plurality of layers comprises:
said first phase; and said second phase which is discontinuous along at least two of any three mutually orthogonal axes;

37. The device, of claim 1 comprising:
a light source;
said light guide; and said light extractor disposed on said light guide

38. The optical device of claim 37, wherein said light extractor comprises a uniaxially oriented optical film.

39. The optical device of claim 37, wherein said first phase (12) comprises a polyester and said second phase (14) comprises syndiotactic polystyrene.

40. A method for using a diffuse reflective polarizer, as an extractor, comprising the steps:
providing a first resin, whose degree of birefringence can be altered by application of a force field, as through dimensional orientation or an applied electric field, such that the resulting resin material has, for at least two orthogonal directions, an index of refraction difference of more than about 0.05;
providing a second resin, dispersed within the first resin; and applying said force field to the composite of both resins such that the indices of the two resins are approximately matched to within less than about 0.05 in one of two directions, and the index difference between first and second resins in the other of two directions is greater than about 0.05.

41. A method of claim 40 wherein the second resin is dispersed in the first resin after imposition of the force field and subsequent alteration of the birefringence of the first resin.