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• 4 Umax=0.9 kV *6 Umax=1.4 kV
■ 5 Umax=1.1 kV *7 Umax=2.7 kV
METHOD AND A DEVICE FOR ELECTRO
MICROSURGERY IN A PHYSIOLOGICAL
FIELD OF THE INVENTION 5
The invention is a method and a device that allows for the electrical emulation of the microsurgical abilities of pulsed lasers. These lasers are the basis for new laser procedures that are responsible for high speed and high precision cutting action in biological liquid environments with minimal damage to the surrounding mechanism. They work by producing cavitation bubbles. The action of these lasers and laser procedures are simulated in the current invention by using protocols that are a part of this invention. These protocols regulate the electrical current injected into the specialized device that has been devised. As a result it is possible to emulate the cavitation bubble formation cutting that has become a hallmark of various pulsed laser procedures. The invention allows the same device to be used for such an
emulation of these cavitation bubbles while also allowing for heat induced coagulation and poration of biological materials.
BACKGROUND OF THE INVENTION
Various pulsed lasers have been applied to soft tissue cutting and removal in a liquid environment. Three basically different mechanisms of light absorption have been involved in laser surgery: (1) linear absorption of light by tissue (I. Turovets, D. Palanker, Y. Kokotov, I. Hemo, A. Lewis, /. 30 Appl. Phys. 79(5): 2689-2693 (1996); D. Palanker, I. Turovets, A. Lewis, Laser-Tissue Interaction VII, Proc. SPIE 2681 (1996)); (2) linear absorption of light by the medium (P. D. Brazitikos, D. J. D'Amico, M. T. Bernal, A. W. Walsh, Ophthalmology 102 (2): 278-290 (1994); C. P. 35 Lin, D. Stern, C. A. Puliafito, Invest. Ophthalmol. Vis. Sci 31(12): 2546-2550 (1990)); or (3) non-linear absorption by tissue or medium associated with dielectric breakdown of the material (A. Vogel, S. Busch, K. Jungnickel, R. Birngruber, Lasers Surg. Med. 15: 32-43 (1994)). In spite of 40 differences in the mechanisms of laser radiation absorption in tissue, the mechanism of tissue disruption with pulsed lasers has been generally associated with an explosive expansion of overheated liquid and subsequent cavitation bubble formation. As a result, material disruption occurs in 45 the light absorption zone and in a zone of fast expansion and collapse of cavitation bubbles (I. Turovets, D. Palanker, Y. Kokotov, I. Hemo, A. Lewis, /. Appln. Phys. 79(5): 2689-2693 (1996); P. D. Brazitijos, D. J. D'Amico, M. T. Bernal, A. W. Walsh, Ophthalmology 102(2): 278-290 50 (1994); and A. Vogel, S. Busch, K. Jungnickel, R. Birngruber, Lasers Surg. Med. 15: 32-43 (1994)).
In view of the general complicated nature of laser-based devices a search was made for ways to emulate with non-laser methodologies the mechanisms that are known to 55 occur with available lasers. In the case of cavitation bubble generation it is known, as described above, that these bubbles result from local and fast heat energy deposition. Thus, it is logical to consider an overheating of a conductive medium with a short pulse of electric current in order to 60 generate an action which is similar to such pulsed laser. The invention described herein realizes such electro microsurgery in a physiological medium with a specific potential for applications in ophthalmology. Previous investigators who have considered pulsed electrical techniques and have seen 65 cavitation bubble formation (R. Vorreuther, R. Corleis, T. Klotz, P. Bernards, U. Englemann,/. Urology 153: 849-853
(1995); R. Lemery, T. K. Leung, E. Lavallee, A. Girard, M. Talajic, D. Roy, M. Montpetit, Circulation 83(1): 279-293 (1991)) considered these bubbles either as an undesired side effect or as a means for shock wave generation for hard tissue destruction. These electrosurgical devices were designed for relatively high energy pulse generation: between 25 mJ and 40 J and with relatively long pulse duration: hundreds of microseconds. Such high energy pulses resulting in a few millimeter-sized cavitation bubbles cannot be applied to microsurgical applications such as those envisioned in delicate organs such as the eye. To accomplish such delicate cavitation bubble based microsurgery, a new electrical system based on an asymmetric microelectrode that enables generation of hundreds of thousands of cavitation bubbles, is described. This can become an alternative to endo-laser equipment in such areas as vitreoretinal surgery.
The concept can also be extended to the electroporation of individual cells and assemblies of cells in which the state of the prior art is a macroscopic device with macroscopic electrodes placed in a large bath with a solution of cells (M. Joersbo and T. Brunstedt, Physiologia Plantarium 81: 256-264 (1991)). Instead of this a microelectrode for local electroporation of individual cells is used, or alternatively, an array of microelectrodes could be applied for poration of assemblies of cells.
In addition, by varying the nature of the characteristics of the electrical current the same device can be used for cavitation bubble cutting, electroporation or coagulation.
STATE OF PRIOR ART
Electrosurgical devices are widely used in surgery. The majority of these techniques are based on heating the tissue by an RF current and this local heat deposition causes one of the following processes: coagulation, and/or water evaporation. As a result, the only capability of such devices is to cut soft tissues by heat deposition which causes significant coagulation in the area surrounding the cut tissue. Such devices are totally useless for endolaser applications, for example in the eye. In addition to such RF techniques, DC pulsed electrical methodologies have not achieved a widespread acceptance because the absence of coagulation was considered an undesirable effect. In the past, cavitation bubbles were generated by DC pulsed methodologies. However, these techniques, which were designed for relatively high energy pulse generation (tens of milliJoules) with relatively long pulse durations (hundreds of microseconds), were only used as a means for shock wave generation for hard tissue destruction (R. Vorreuther, R. Corleis, T. Klotz, P. Bernards, U. Engelmann, /. Urology 153: 849-853 (1995)). These high energy pulses resulted in cavitation bubbles with dimensions of a few millimeters, and these have no applicability to, for example, eye microsurgery in which considerably smaller bubbles are required. Laserbased techniques indicate that the pulse energies required to produce such bubbles are in the range of a few tens of microJoules and the pulse durations required are generally in a sub-microsecond range (D. Palanker, I. Hemo, I. Turovets, H. Zauberman, A. Lewis, Invest Ophthal. Vis. Sci. 35: 3835-3840 (1994); C. P. Lin, Y. K. Weaver, R. Birngruber, J. P. Fujimoto, C. A. Puliafito, Lasers Surg. Med. 15: 44-53 (1994)). In addition to these differences in the time/energy characteristics of the available DC pulsed technologies as compared the present invention, it is required that any device for applications such as vitreoretinal surgery should be able to withstand tens of thousands of pulses. The previous high energy devices described above have a lifetime of less than
100 pulses (R. Vorreuther, R. Corleis, T. Klotz, P. Bernards, U. Engleman,/. Urology 153: 849-853 (1995) and this is by far not sufficient for the microsurgical applications that are envisioned.
In terms of cell poration, the prior art were again macroscopic devices with macroscopic electrodes placed in a large bath (M. Joersbo and J. Brunstedt, Physiologia Plantarium 81: 256-264 (1991)) with a solution of cells.
SUMMARY OF THE INVENTION
The method and device of the present invention are based on producing submicrosecond high voltage discharges in physiological media with special protocols designed for the generation of cavitation bubbles for soft tissue microsurgery in a liquid environment as is possible today with certain pulsed lasers. The device consists of a combination of three elements:
a specific microelectrode structure, specific electrical protocols to develop the required pulse characteristics to emulate pulsed laser microsurgery with cavitation bubble generation in the same device that can produce other electrical protocols for tissue coagulation and electroporation; and the above protocols determine the characteristics of the HV pulse generator that is to be used.
DESCRIPTION OF THE INVENTION
The foregoing features of the invention are illustrated in the accompanying drawings, in which:
FIG. 1A is a schematic illustration of a microelectrode in accordance with the invention, utilizing a single wire and having a tapered insulator with a flat tip;
FIG. IB is a schematic illustration of a microelectrode in accordance with the invention, utilizing a single wire and having a nontapered insulator with a flat tip;
FIG. 1C is a modification of the device of FIG. 1A, wherein the insulator has a rounded tip;
FIG. ID is a modification of the device of FIG. IB, wherein the insulator has a rounded tip;
FIG. 2 is a schematic diagram of a high voltage generator connected to the microelectrode of FIGS. 1A-1D;
FIG. 3A is a schematic illustration of a microelectrode in accordance with the invention, having multiple wires;
FIG. 3B is a schematic illustration of a partially bent, single-wire microelectrode in accordance with the invention, having a flat tip;
FIG. 3C is a schematic illustration of a single-wire side-firing microelectrode in accordance with the invention, having a flat tip;
FIG. 4A and 4B are schematic top and side views, respectively, of a microelectrode array;
FIG. 5A is a graphical illustration of the time dependence of electrode potential (U) and current passing through the exit surface of an electrode (-1) during a discharge, the electrode having a wire diameter of 25 fim;
FIG. 5B is a graphical illustration of a second discharge, following that illustrated in FIG. 5A;
FIG. 6 is a sequence of micrographs illustrating the dynamics of cavitation bubbles generated at a potential (Umax) of 2.7 kV, utilizing an electrode having a wire diameter of 20 fim and a tip diameter of 200 fim, at a magnification of lOOx, the delay between the electric pulse and the flash pulse being shown in fis in each frame
One way to form the microelectrodes, or needles, of the present invention is to seal a thin metal wire (1.5) into an insulator (1.2) with a variety of structures that can be tapered 5 (FIGS. 1A & 1C) or have other geometries (FIGS. IB & ID). The wire (1.5) has a diameter at its exit from insulator
(1.2) in the range of 1-100 microns. This insulator (1.2) and wire (1.5) creates an internal (main) electrode (1.1). A second electrode (1.3) is provided to mechanically protect
10 the main electrode. This may be formed by coating the surrounding insulator (1.2) with a metallic coating (1.3) (see FIG. 1A). The resulting external electrode can play the role of a protective metal cover for the main inner electrode (1.1). The geometry of this microelectrode and its connection to
15 the output terminals (2.1) and (2.2) of the HV pulse generator (2.3) are schematically shown in FIG. 2.
As shown in FIG. 2, the main electrode is placed in a conducting medium (2.4). The high voltage (HV) generator
(2.3) produces electrical submicrosecond duration dis20 charges through a gas layer in the conducting liquidcontaining environment which produces cavitation bubbles with characteristics which emulate the action of pulsed lasers in a liquid medium. The bubbles are of sub-millimeter sizes. Such cavitation bubbles provide a mechanism for soft
25 tissue microsurgery in a physiological medium, such as in the eye.
The microelectrode may be fabricated by pulling a glass microcapillary tube having a metal wire inside the tube. The tube is heated and pulled to produce the tapered shape of
30 FIG. 1A, with the glass forming the insulator (1.2). Alternatively, the microelectrode can be fabricated using microlithography. The device may be used as a single device or multiple microelectrodes may be mounted in an array, as illustrated in FIGS. 4A and 4B, for use in microcutting or
35 microperforation of materials, such as aggregates of cells. The outer dimensions of the microelectrode (1.4) can be chosen according to the requirements of the application. For example, for microsurgical applications they could be similar to that of laser tips applied in endolaser microsurgery.
40 The diameter of the insulator around the exit of the main electrode (1.1) should be large enough to have mechanical strength while preventing the puncture of soft tissue. On the other hand, it should be small enough to enable it to reach the tissue to be cut at various angles. These requirements
45 determine the range of the diameter of electrode (1.1) to be: 0.05-0.4 mm. It is useful to have rounded edges of the insulator (FIG. 1C, 1.6) in order to keep the electrode wire (1.5) in close proximity to the treated tissue when the tip is held at different angles relative to the tissue surface. The
50 diameter of insulator (1.2) inside the second electrode (1.3) should be as large as possible to decrease the capacitance of the electrodes in the conductive liquid environment, and could be equal to the inner diameter of the external electrode (1.3). In certain cases (1.2) could be smaller than (1.3) in
55 order to provide a gap (1.9) between electrode 1.3 and insulator (1.2) (FIG. 1A) to allow suction during the treatment. Such suction allows lifting of treated tissues and the evacuation of gas bubbles and tissue debris that results from tissue cutting by the generated bubbles.
60 The outer diameter of the second (external) electrode (1.4) should be 0.9-1 mm, as this is standard equipment for instruments used in certain microsurgical procedures used in vitreoretinal surgery.
The total length (1.7) of the microelectrode (FIG. 1A) is
65 38-40 mm to allow for access to all the areas inside the eye ball for such vitreoretinal surgery. Other microsurgical procedures may require other dimensions.
The same structure could be used with, for example, a set of multiple wires as the inner electrode (see FIG. 3A, 1.8) or the tip can be partially bent in order to fire the cavitation bubble at an angle (FIG. 3B) or can have a geometry that can produce a cavitation bubble at right angles to the axis of the 5 electrode (FIG. 3C). All the electrode configurations shown in FIGS. 3A-3C can also have electrode and insulator geometries with the structures that are seen in FIGS. 1A-1D. Electrical Protocols to Emulate Pulse Laser Induced Cavitation Bubbles 10
To achieve the high cutting efficiency of the pulsed laser treatments that are currently being developed, cavitation bubbles should be created fast enough for generation of high pressures and high boundary velocity and acceleration. These requirements determine the minimal peak power of the pulse. On the other hand, the cutting action should be local enough for prevention of extensive damage in the surroundings of a lesion. This requirement limits the total energy imposed on the bubble formation. Based on the 20 experience of laser-induced cavitation (D. Palanker, I. Hemo, I. Turovets, H. Zauberman, A. Lewis, Invest Ophthal. Vis. Sci 35: 3835-3840 (1994); C. P. Lin, Y. K. Weaver, R. Birngruber, J. G. Fujimoto, C. A. Puliafito, Lasers Surg. Med. 15: 44-53 (1994)), the diameter of the cavitation 25 bubble required for precise and effective cutting of vitreoretinal tissue should be in a range of 0.4-0.5 mm, that corresponds to the bubble energies in a range of 3 to 6 pd. The High Voltage Pulse Generator 30
The foregoing protocols determine the characteristics of the high voltage pulse generator. The electrode diameter 1.5 has to be capable of generating single pulses and pulse trains with a pulse duration varying in a range of 30 ns-3 pis, and the generator must be capable of varying the voltage ampli- 35 tude in the range of 100 V-10 kV. The peak current during the pulse can reach a few Amperes.
In addition to pulse generation aimed at cavitation bubble generation and tissue cutting, electrical pulses with lower 40 voltage and, possibly, longer pulse duration could be applied with the above electrodes for electroporation of individual cells or for cell layers. Furthermore, the electrical power supply can also be amended so that this invention can also have the added capability of a coagulation. 45 Extension of the Invention to Parallel Devices
Similar electrode geometries and pulse protocols can be envisioned to produce a parallel array of electrodes for the generation of a parallel array of cavitation bubbles and/or heating for producing bioelectromechanical field effects on multiple biological cells at one time (see FIG. 4). Applications of the Device
Numerous applications of the invented device are possible in the field of soft tissue microsurgery based on the cutting 55 action of the generated cavitation bubbles. One of the most promising for the single electrode is vitreoretinal membrane removal, because the accepted mechanical peeling and cutting of such membranes is often associated with retinal damage. Furthermore, the present device can be used in all microsurgical procedures in physiological media (or other conducting liquids), including microsurgery of the internal organs.
In addition, with the modified electrical characteristics the 65 device could also be used for bioelectromechanical effects of individual cells and cell layers, and coagulation of tissue.
Furthermore, the bent, cantilevered tips that produced in this invention can be of considerable value in other areas of science and technology. For example, such cantilevered electrodes can be produced such that the cantilever is very flexible (Force constants of a few N/m) and the tip is very small (0.05 pi). With such an extension of the present methodology, together with the pulsed protocols that have been developed, and that have been described herein, controlled alteration of surfaces can be effected that will allow fine lithographic patterning of such surfaces. Experiments
Analysis of the Modes of the Electrical Discharge of the Device
The pulse protocols that have been invented and are described herein were developed as a result of detailed experimentation that allowed close emulation of the effects of pulsed laser cavitation bubble generation.
Specific examples of these experiments are described in this section. For example, for an electrode with a wire diameter (1.5) of 25 pirn the pulse profiles of the electrode potential (U) and the current passing through the exit surface of the electrode (I) are presented in FIG. 5. At Uma=c=0.3 kV (FIG. 5A, curves 1) the voltage and current simultaneously decrease with a time constant of about 0.6 pis. As the potential increases, the nature of the discharge changes: The current drops much faster after about 0.2 pis, resulting in slowing down the voltage reduction (FIG. 5A, curves 2). At Um(n.=0.7 kv (FIG. 5A, curves 3), the current falls to zero (switched off) when the potential is still at half of the maximum. This switching off of the current results from gas generation on the surface of the electrode that disconnects the liquid from the metal surface.
As the electric field in the gas layer becomes high enough, an electron avalanche is generated in this layer, that then propagates inside the liquid. This results in the second pulse of current generated after the first one (see FIG. 5B), and with increase of the voltage the delay between these two pulses decrease. At Uma=c higher than 1.4 kV (FIG. 5B, curve 6), these two pulses completely overlap and at Vmax 2.7 kV (FIG. 5B, curve 7), they became indistinguishable. The discharge at the voltage range of 1.4-2.7 kV was accompanied by an emission of reddish light and a sound wave generation. At Umax=2.6 kV, the dimensions of the lighted spot was about 7 fim. The best emulation of the laser cutting was achieved with a range of high voltage that is 2-2.7 kV. Cavitation Bubble Dynamics
The sequence of micrographs of cavitation generated at the electrode with a 20 fim wire at Uma=c=2.7 kV is shown in FIG. 6. The delay time between the electric pulse and the flash of the dye laser is shown (in pis) in the corner of each frame. The spark generated in the vicinity of the electrode is clearly seen as a white spot in front of the wire. The average velocity of the bubble boundary during the first 1 pis of the growth phase (frames 1,2) was about 90 m/s. The primary cavitation bubble grew in about 25 pis (frames 2,3) reaching the maximal diameter of about 0.5 mm. During the collapse, the bubble had a mushroom-like shape (frame 4) that was eventually transformed to a ring and a stem connecting its center with the center of the tip (frame 5). The secondary bubbles were generated from both the ring and the stem (frames 6,7). These bubbles were ejected away from the tip at different velocities (about 5 and 17 m/s, respectively) and