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United States Patent [i°]

Robbins

[li] Patent Number: 4,528,671 [45] Date of Patent: Jul. 9, 1985

[54] MULTIPLE HOST FACE-PUMPED LASER

[75] Inventor: Alexander G. Robbins, Vestal, N.Y.

[73] Assignee: General Electric Company, Burlington, Vt.

[21] Appl. No.: 602,841

[22] Filed: Apr. 23, 1984

Related U.S. Application Data

[63] Continuation-in-part of Ser. No. 317,134, Nov. 2, 1981, abandoned.

[51] Int. CV HOIS 3/14

[52] U.S. CI 372/68; 372/71;

372/66; 372/35

[58] Field of Search 372/62, 68, 71, 66,

372/67, 51, 54, 72, 35

[56] References Cited

U.S. PATENT DOCUMENTS

3.810.040 5/1974 Martin et al. 372/68

3.810.041 5/1974 Martin 372/68

4,207,541 6/1980 Karger et al 372/71

4,233,567 11/1980 Chernock 372/72

Primary Examiner—James W. Davie
Assistant Examiner—Leon Scott, Jr.
Attorney, Agent, or Firm—Bailin L. Kuch

[57] ABSTRACT

A total internal reflection, face pumped laser is provided, in a single head, with two (or more) generally parallel, spaced apart hosts for providing a higher average power output than the typical single host FPL. A pair of flash lamps, one each adjacent the outer surface of each host, acts as the "pumping" means for the laser and operates in effect to produce asymmetrical pumping of the respective hosts. In order to prevent exceeding the thermal stress limit and thermally inducing bending of the hosts, a system of asymmetrical cooling is provided whereby a greater flow of fluid coolant is provided the surfaces of the two hosts which are closer to the "pumping" flash lamps than to the inner host surfaces which are proximate one another.

9 Claims, 3 Drawing Figures

[graphic]

U.S. Patent Jul. 9,1985 Sheet 1 of2 4,528,671 1 2

[merged small][merged small][graphic]

The general form of these multi-segment rod type

MULTIPLE HOST FACE-PUMPED LASER lasers as shown in U.S. Pat. No. 3,715,682 issued to

Young have glass discs which are generally edge

RELATED APPLICATIONS pumped and therefore have some radial thermal gradi

This application is a continuation-in-part of Ser. No. 5 ents due,to "°n-uniform pumping. These radial gradi

317,134 filed Nov. 2, 1981, now abandoned. e"ts result In degradat>on of the, >>eam coherence. Opt.

cal compensation can be introduced as shown m U.S.

BACKGROUND OF THE INVENTION Pat. No. 3,675,152 issued to Young. The radial refrac

1. Field of the Invention ln tive index Sradien/ compensation means^ utilized re

This invention relates to a face pumped laser, and 10 fires ll!at therma equilibrium be reached before the

, , „ , , .,. ■ , j laser pulse has full energy and good coherence. An

more particularly, to such a laser providing in one head u *\. . . &j e>

i r. r i u * ii ■ . i r alternative optical compensation means is the multi

a plurality of laser hosts allowing a greater volume of *\ . 're _ . XT , . , .

, Y. . . „ . , path array as shown in U.S. Pat. No. 3,628,179 issued to

host material and therefore higher average power laser . . c .'

. . .., . . . . .5 , rc r Cuff et al. This compensates for transverse temperature

output while maintaining the benefits of the face J- » J * i.n *

. 4 t i • ^ in*- i . i_ • 15 gradients due to coolant flow but does not compensate

pumped, total internal reflection laser technique. *r ^ ... M t erature dient dueon.

2 Description of the Prior Art uniform p m Aof the above multiple.segment

It is well known in the art tha laser devices emit rod ( ^ ^ve in common the limitat^n tlfat the

electromagnetic radiation of wavelengths generally in ^ v thro h ^ ... When w

the infrafred and visible portions of the electromagnetic 2Q md ^ tition rates are employedi the

spectrum. The radiation emission is substantially coher- . enfi isB arti^, absorbed b theF coolant. This

ent and is characterized by a narrow wavelength band. ... ... ... and thus index of refraction

Laser devices are operable using a suitable medium or dients which cause serious D tical distortion or loss host m which a population inversion may be established of coherence in the lasin beam_ m a particular metastable energy level by proper optical 25 Present!y face d lasers are advantageously pumping . Neodymium glass ruby, helium, neon, and employed as pulsed lasers. A face pumped laser rmits carbon dioxide are media which . are commonly em- substantially uniform activitation and concomitant heatployed m lasers. By pumping or irradiating the active ing across the ,aser aperature in contract t0 the nonuni. medium with electromagnetic radiation possessing form optical properties of the side-pumped, rod-type power necessary to create the population inversion, J0 laser device u s pat No 3,631,361-Almasi et al., conditions permitting coherent emission may be ob- assigned t0 the same assignee as the present invention, tamed. The means emitting the radiation causing mver- discioses an arrangement for substantially increasing the sion is called "pumping means" while the wavelength of pulse repetition rate of face-pumped laser devices by the radiation is known as the "pumping wavelength". eliminating the distortion due to nonuniform heating.

Laser devices which emit high energy pulses are well 35 xhe losses and the distortion due to the laser output

known in the art as pulsed lasers. The emitted pulses, beam passjng through the interspersed coolant flow

though high in energy, are short in duration, lasting on remain.

the order of milliseconds to picoseconds. The face pumped iaser with total internal reflection The laser output is only a small percentage of the wnen uniformly activated has intrinsic beam wave front input energy, a large percentage of the energy ending 40 compensation for thermal gradients within the laser up as heat in the laser medium. In pulsed lasers, one or nost and no wave front distorition due to laser output more surfaces of the active medium are cooled in order beam paSsage through the coolant. These characteristo extract the excess heat. Because of the limited ther- tjcs are advantageously utilized for high average power, mal conductivity of the host material, the excess heat is high beam intensity and high repetition rate lasers. Exmore rapidly removed from near the surface than from 45 ampies of this art are U.S. Pat. No. 3,633,126 issued to the interior, causing the center of the host to be warmer Martin et al and U.S. Pat. No. 4,214,216 issued to Jones, than the surface. Repeated operation of the laser host, jr., both assigned also to the same assignee as the presprecluding a proper cooling period, causes a substantial ent invention.

thermal gradient to be established, resulting in possible A unique characteristic of the face pumped laser with

strutural failure or distortion of the output beam. Lasers 50 total internal reflection is that the laser beam is directed

employing host materials characterized by low thermal through the laser host by means of total internal reflec

conductivities are particularly limited to low pulse rep- tions from the major faces which also admit the pump

etition rates. ing radiation. Thus maintaining the optical alignment

Recent interest in high repetition rates of pulsed la- and, hence, the performance of a laser resonator that

sers has led to increased activity in this field. Since a 55 incorporates a face pumped laser host with total internal

number of materials, particularly those of the doped reflections is dependent upon maintaining the laser host

glass species, which are employed as the active laser major faces substantial flat and parallel. The potential

host have low thermal conductivity, several approaches means of disturbing the resonator alignment is to cause

have been taken to overcome this restraint on pulse flexure of the laser host by either inadequate support or

repetition rate. These approaches have in common the 60 unequal heating (or cooling) of the major faces. Flexure

segmenting of a side-pumped, rod type laser host and of the laser host curves the major face where the total

interspersing of a flowing coolant. The result of this internal reflection occurs and cause the exiting laser

procedure is that the unwanted heat is more quickly beam to be non-parallel to the entering laser beam. Thus removed through the relatively smaller dimension of all faced pumped lasers with total internal reflections the segmented laser host material and therefore the 65 require proper means of supporting and cooling the composite arrangement can be operated at higher pulse laser host to ensure that there is no flexure of the laser repetition rates without structural failure due to ther- host to cause misalignment that results in degraded

mally induced stress. performance.

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