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Publication numberUS3657600 A
Publication typeGrant
Publication dateApr 18, 1972
Filing dateMay 18, 1970
Priority dateMay 18, 1970
Publication numberUS 3657600 A, US 3657600A, US-A-3657600, US3657600 A, US3657600A
InventorsWiegand Walter J Jr
Original AssigneeUnited Aircraft Corp
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Auxiliary ionization of dc electric discharge electrode boundary sheaths
US 3657600 A
Abstract
Auxiliary ionization is provided in a DC electric discharge plasma immediately adjacent one or more electrodes, whereby the tendency for streamering or incipient arcing and non uniform attachment of the discharge to electrodes is mitigated. Separate RF electrodes, RF electrodes combined with a DC cathode, separate and combined low voltage DC auxiliary ionization are disclosed. Photon and particle beam ionization are discussed.
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Description  (OCR text may contain errors)

United States Patent Wiegand, Jr.

[54] AUXILIARY IONIZATION OF DC ELECTRIC DISCHARGE ELECTRODE BOUNDARY SHEATHS [72] lnventor: Walter J. Wiegand, ,lr., Glastonbury,

Conn.

[73] Assignee: United Aircraft Corporation, East Hartford,Conn.

[22] Filed: May 18, 1970 [21] Appl. No.: 38,033

[52] U.S.Cl ..3l7/4,3l5/330,313/l97 [51] Int. Cl. ..H0lj 61/54 [58] Field oiSearch ..3l7/3,4, 262 R;3l5/93,330; 313/189, 197

[56] References Cited UNITED STATES PATENTS 2,921,236 l/l960 Gawehn ..313/197x 1451 Apr. 18, 1972 3,275,885 9/1966 Pompfreti ..3 1 5/3 30 3,480,820 11/1969 Fehnel ..3 13/1 89 X 3,465,192 9/1969 Lafferty ..3l5/330 X 2,699,513 1/1955 Watt ..3l3/93 X Primary Examiner-L. T. Hix Attorney-Melvin Pearson Williams auxiliary ionization are disclosed. Photon and particle beam ionization are discussed.

5 Claims, 5 Drawing Figures BACKGROUND OF THE INVENTION 1. Field of Invention This invention relates to DC electric discharge plasmas, and more particularly to auxiliary ionization in the electrode sheaths therein.

2. Description of the Prior Art In the various electronic arts dealing with DC electric discharge plasmas, the creation and use of such plasmas has long been known. However, the recent advent of the high power gas laser, and particularly the nitrogen/carbon dioxide laser, has revealed certain critical adverse relationships between the useful performance of the discharge and certain of the properties thereof. For instance, in gas lasers, the function of the electric discharge plasma is to excite atoms or molecules of an energizing gas or a lasing gas to higher energy states which are useful in the production of electromagnetic radiation. This function is enhanced by a uniform plasma, having little or no streamering or incipient arcing, and having a uniform attachment of the plasma to the electrodes of the discharge. Streamering or incipient arcing is undesirable since it results in a loss of efficiency and power and in most cases it is necessary that the discharge be operated at a lower than optimum current density to avoid these effects. Another troublesome discharge phenomena is nonuniform attachment of the discharge to the electrodes, particularly in the case of large cathode and anode surface areas. These difficulties are compounded in high power gas laser systems where the gas pressure and current density are set at their upper limits in order to extract maximum power per unit volume.

Discharges of this type consist of a positive column connected through sheaths to a cathode and an anode. The positive column, a region of more or less uniform electric field, comprises a major portion of the discharge length. The cathode fall region at typical operating pressures of a nitrogen/carbon dioxide laser extends a short distance into the discharge, typically from about 0.5 cm to about 10 cm, depending inversely upon pressure; this distance being small compared to the length of the positive column. The magnitude of the electric field in the positive column is determined basically by the requirement that the electrons be distributed in energy in such a way as to make up through ionization the loss of charge particles due to volume recombination and ion neutralization on the tube walls. Furthermore, the electric field E, must, in conjunction with the local electric conductivity of the plasma, give rise to the required discharge current which, in the positive column, is carried almost exclusively by the electrons. The total voltage drop across the positive column may in some discharges represent only a small portion of the total discharge voltage. In gas lasers, it is the positive column that normally contributes most to the laser output. This is true since the positive column is usually much longer than any other region of the discharge and its properties may more easily be controlled by changes in the applied voltage. This has been verified by the fact that when the ratio of electric field to neutral particle gas density (E/N) in the positive column is adjusted by changing the voltage applied across the discharge to optimize the laser output, it is found that the E/N measured in the positive column is consistent with that calculated to be near the optimum for laser operation. The sheaths are the discharge regions at either extreme of the positive column where the boundary conditions on the ends of the column are satisfied. The electric fields in the sheath regions (which are much higher than the field along the positive column), are therefore too high to efficiently produce a laser population inversion. Basically, this indicates that the positive column is the effective laser energizing portion of the discharge and the sheath regions are necessary only to'the extent that they permit the positive column to exist.

The boundary conditions near the anode are considerably simpler than the cathode fall conditions.

At the anode end of form,

the positive column, an ion current is directed toward the cathode. This ion current is required to make up for the ion current flowing into the cathode sheath at the far end of the positive column. Normally, it is assumed that there are no sources or sinks of current in the positive column, but only enough ionization to make up for ion diffusion to walls and volume recombination losses. An electron accelerating sheath forms at the anode through which the electron current passes.

This sheath typically has a voltage drop of approximately the ionization potential of the gas in order that a small ion current source exists through direct electron ionization processes.

The processes taking place near the cathode are considerably more complex than those at the anode. Between the cathode and the positive column there is the cathode fall region which is a high electric field region attached to the cathode followed by a negative glow region nearer to the positive column. The boundary conditions at the cathode end of the positive column must be matched to the electron emission properties of the cathode. In hot cathode discharges and in spray or Malter discharges, copious electron emission takes place at the cathode and only a very small cathode fall exists. Unfortunately, materials problems and/or chemical processes occur on these types of cathodes in some applications, such as nitrogen/carbon dioxide lasers and perhaps other gas lasers such that the small cathode fall associated with a hot cathode cannot be exploited to full advantage. Moreover, these cathodes can be subject to the streamering and nonuniformity problems that the present invention is designed to circumvent.

in cold cathode discharges, used for instance in the current laser art, a large cathode fall usually exists. The high electric field is required to accelerate electrons emitted from the cathode into the cathode fall region where some of the electrons cause ionization and give rise to a region of fairly high ionization rate. ions from this region are accelerated back through the cathode fall potential, gaining energy, and upon striking the cathode, gives rise to secondary electron emission. These secondary electrons are then accelerated into the cathode fall region, completing the circular process. The shape of the potential profile across the cathode fall, the electron and ion currents and energy distributions, the secondary emission process and losses in this region, must all be inter- I nally, mutually consistent.

It is important to note that the cathode fall of a cold cathode discharge must satisfy a number of individual requirements in order to accommodate the boundary conditions of the discharge and the cathode processes. This, of course, has far reaching consequences since it is thought that it is because the discharge is unable to solve the boundary conditions imposed at the electrode that it is forced into a condition of streamering at the cathode. In particular, it appears that, at the currents and pressures encountered in high power lasers, the secondary electron emission process is not adequate to give rise to that ionization rate required in the cathode fall to maintain equilibrium. The only way that the cathode can give rise to the electron current consistent with the external DC power supply and the discharge boundary conditions is to constrict into an arc at the cathode and thereby meet the electron emission requirements through thermionic emission.

SUMMARY OF THE INVENTION The object of the present invention is to provide improved DC electric discharge plasmas.

According to the present invention, auxiliary ionization of the plasma is provided in a region near at least one of the discharge forming electrodes. According further to the present invention, auxiliary ionization may be provided at both electrodes of a DC electric discharge plasma.

According to the ionization in oneform, radio frequencyionization is employed; the ionizatinon may be applied by separate electrodes or may be provided across a segmented DC electrode. in accordance with the invention in another low voltage DC ionization may be utilized, it being applied either by separate electrodes or across a segmented high voltage DC electrode. In accordance still further with the invention, other sources of auxiliary ionization may be employed.

' The present invention improves the boundary conditions of BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a simplified, schematicized diagram of one embodiment of the present invention employing separate primary and auxiliary DC ionization electrodes;

FIG. 2 is a simplified, schematicized diagram of an embodiment of the invention applying low voltage DC auxiliary ionization to a segmented primary high voltage DC cathode;

FIG. 3 is a simplified, schematicized diagram of an embodiment of the invention employing separate auxiliary RF and primary DC electrodes;

FIG. 4 is a simplified, schematicized diagram of an embodiment of the present invention employing the application of RF auxiliary ionization to a segmented high voltage DC cathode; and

FIG. 5 is a simplified, schematicized perspective of an embodiment of the invention applying RF auxiliary ionization between segmented RF electrodes and a DC cathode.

DESCRIPTION OF THE PREFERRED EMBODIMENT Referring now to FIG. 1, the primary object of the present invention, which is to improve DC electric discharge boundary conditions by applying auxiliary ionization to the area immediately adjacent one or more of the electrodes 12 and of the DC discharge, is accomplished in an electric discharge apparatus by means of a pair of auxiliary low voltage DC electrodes 14 which are disposed adjacent the main DC cathode 16. The electrodes 12, 14 are connected across a low voltage DC power supply 18 so as to provide an electric field and produce ionization l9 therebetween. The cathode 16 and an anode 20 are connected across a high voltage, primary DC power supply 22 so as to create the useful electric discharge plasma in the region 24, the enhancement of which is the purpose of the present invention. In the embodiment of FIG. 1 the low voltage auxiliary ionization potential may be referred to the high voltage primary potential, such as by connecting the electrode 14 to the electrode 16 as at the junction 26. This connection may be considered ground potential in the system. On the other hand, the junction 26 may be eliminated if desired in certain embodiments, in which case the auxiliary ionization 19, although apparently floating, is referred to the cathode 16 through conduction within the plasma.

The discharge apparatus 10 is shown in dotted fashion to point out the fact that the present invention may be utilized in a wide variety of different types of discharge apparatus. For instance, the apparatus may be a closed system containing an ionizable gas; on the other hand, the discharge apparatus 10 may comprise an area within a conduit through which suitable gases may flow. For typical configurations, reference may be made to patented and published art relating to industrial, laser and other types of electric discharge plasma apparatus.

In the embodiment of FIG. 2, the discharge apparatus 10a includes a segmented cathode 16a, 16b and the low voltage, auxiliary ionization DC power supply 18 is connected across two segments 16a, 16b, rather than having the separate electrode shown in FIG. 1. In this embodiment, the junction 26 Because of the auxiliary ionization 19 between the segments 16a, 16b, the segment 16b will be at substantially the same potential as the segment 16a. Thus each of the two segments can act as cathodes with respect to the anode 20 in the formulation of the primary ionization in the region 24. In this embodiment, the boundary conditions discussed hereinbefore are satisfied between the cathode segments.

Referring now to FIG. 3, the auxiliary ionization 19 may be provided by means of RF excitation, rather than by the low voltage DC excitation illustrated in FIGS. 1 and 2. Therein, the auxiliary electrodes 12, 14 are connected to an RF power supply 28 through DC isolation capacitors 30, and the cathode 16 is connected through an RF choke coil 32 to the high voltage DC power supply 22. The capacitors 30 and the choke 32 provide mutual isolation between the RF and the DC.

In FIG. 4, the RF auxiliary ionization is applied by the capacitors 30 to segments 16a and 16bof a segmented cathode, the RF choke 32a being connected between the segments 16a, 16b, and the center tap thereof connected to the high voltage DC power supply 22. This provides DC power to both segments 16a, 16b while maintaining RF isolation so that the auxiliary ionization 19 may be established between them, while both segments participate with the anode 20 in the formulation of the primary electric discharge plasma in the region 24.

In another embodiment of the invention as illustrated in FIG. 5, electric discharge apparatus 10b includes a perforated cathode 16c having a plurality of finger electrodes 36 extending therethrough and slightly into the region 24 where the primary electric discharge plasma is to be established. The RF power supply 28 is connected between the finger electrodes 36 and the perforated cathode 16c. The DC power supply is connected between the cathode 16c and the anode 20 so as to provide the DC field necessary for the creation of the primary electric discharge plasma. In the embodiment of FIG. 5, the auxiliary ionization l9 exists between each finger electrode 36 and the perforated cathode 16c. However, this does provide the desired uniformity.

Each of the embodiments of FIGS. l-5 described herein employs auxiliary ionization only at the cathode. In most cases, application of auxiliary ionization to the cathode is sufficient to provide the enhanced operation of the DC electric discharge plasma which is desired. However, in the event that the particular parameters of a given utilization of the present invention so warrant, auxiliary ionization may also be provided at the anode so as to enhance the boundary conditions in the anode sheath as described hereinbefore. In most cases, a judgement must be made as to the improvement desired for the cost required; the improvement provided by auxiliary ionization at the boundary of the plasma with the cathode will usually be sufficient. so that provision of further improvement at the anode boundary will not be worth the cost thereof. The embodiments herein are schematic in nature, and not necessarily illustrative of the specific hardware utilized in performing the present invention. For instance, another method of applying RF preionization between an auxiliary RF electrode and a DC cathode is to employ a well known RF helical resonator electrode; in such case, the RF power 28 is applied across the helix; and the chamber is connected to the DC power supply 22 and serves as the main electric discharge cathode 16.

Although not disclosed herein, auxiliary ionization 19 may be provided by sources other than electric fields across electrodes. For instance, a source of intense photon flux may be oriented to inject flux adjacent to either or both of the main electrodes of the DC electric discharge. In the case where the present invention is employed in a gas laser, the photon flux should preferably be of a wavelength which does not interfere with laser operation. Similarly, a high energy particle beam source, such as the type employed in electron beam drilling and welding, may be utilized to provide auxiliary ionization. These are not disclosed herein because such complex discloprovides a reference between the two power supplies 18, 22. sure does not add to the state of the art in view of the variety of the configurations which may be employed and the well known nature of such devices in the art.

Thus, although the invention has been shown and described with respect to preferred embodiments thereof, it should be understood by those skilled in the art that the foregoing and various other changes and omissions in the form and detail thereof may be made therein without departing from the spirit and the scope of the invention.

Iclaim:

Having thus described typical embodiments of my invention, that which I claim as new and desire to secure by Letters Patent of the United States is:

1. An apparatus for producing direct current electric discharge plasma including:

electrode means comprising a pair of electrodes;

means providing a high voltage direct current electric field across said electrode means; and

an ionizable gaseous medium disposed between said electrode means within which the electric discharge plasma is established;

wherein the improvement comprises:

meaNs establishing continuous auxiliary ionization immediately adjacent one of said electrodes which comprises a plurality of segments, the auxiliary ionization being established between said segments to provide better attachment of the plasma to said one of the electrodes and to reduce incipient arcing in the plasma between said pair of electrodes.

2. In direct current electric discharge apparatus including a pair of electrodes for producing a plasma which comprises a positive column of uniform electric field and a sheath region at either end thereof, the method of minimizing streamering and incipient arcing in the plasma and providing a more uniform attachment of the plasma to the electrodes including the steps of:

discharging a high voltage direct current across an ionizable gas which is located between the electrodes to produce a cold cathode type discharge having a large cathode fall potential; and

providing a continuous source of auxiliary ionization to the sheath region to reduce the cathode fall potential.

3. The invention according to claim 9 wherein a low voltage DC power source is connected across said segments of the electrode means.

4. The invention according to claim 1 wherein an RF coupling means connects an RF power source across said segments of the electrode means, and RF isolation means is included in said high voltage DC electric field providing means for connecting said segments of the electrode means to said high voltage DC electric field providing means.

5. The invention according to claim 4 wherein the electrode means is perforated and wherein a plurality of finger electrodes is disposed within the perforations of the electrode means.

mg? v UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTEON Patent No. 3,657,600 Dated April 18, 1972 Inventor(s) WALTER J. WIEGAND, JR.

It is certified that:v error apoeers in the above-identified patent and that said Letters Patent are hereby corrected as shown below:

Column 5, Claim 1, line 10 the Word "meaNs" should read means Column 6, Claim'3, line 1 number '9" should read 1 Signed and sealed this 22nd day of August 1972.

(SEAL) Attest:

EDWARD M.FLETCHER, JR. ROBERT GOTTSCHALK Attesting Officer- Commissioner of Patents gg UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTEON Patent No. 3,657,600 Dated April 18, 1972 Inventor(s) WALTER J. WIEGAND, JR.

It is certified thateerror appears in the above-identified patent and that said Letters Patent are hereby corrected as shown below:

Column 5, Claim 1, line 10 the word "meaNs" should read Column 6, Claim 3, line 1 V number "9" should read 1 Signed and sealed this 22nd day of August 1972.

(SEAL) Attest:

EDWARD M.FLETGHER, JR. 1 ROBERT GOTTSCHALK Attesting Officer Commissioner of Patents

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Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3842284 *Dec 15, 1972Oct 15, 1974Us Air ForceRadioactive preionization method and apparatus for pulsed gas lasers
US3848202 *May 23, 1972Nov 12, 1974Secr Defence BritTransverse excitation system for gas laser using three electrodes
US3886479 *Nov 23, 1971May 27, 1975Nat Res DevElectrode systems for gas discharge devices particularly gas lasers
US3887882 *Aug 1, 1972Jun 3, 1975United Aircraft CorpElectric discharge laser with electromagnetic radiation induced conductivity enhancement of the gain medium
US4024465 *Jul 1, 1975May 17, 1977Westinghouse Electric CorporationGeneration of corona for laser excitation
US4077017 *Apr 4, 1977Feb 28, 1978The United States Government As Represented By The U. S. Department Of EnergyUltraviolet radiation induced discharge laser
US4611148 *Feb 6, 1984Sep 9, 1986Hitachi, Ltd.Low-pressure mercury vapor discharge lamp
US4697121 *Sep 8, 1986Sep 29, 1987Hitachi, Ltd.Low-pressure mercury vapor discharge lamp
US7577177 *Jan 12, 2005Aug 18, 2009Videojet Technologies Inc.Multi-path laser system
EP0560742A1 *Mar 10, 1993Sep 15, 1993PROEL TECNOLOGIE S.p.A.Plasma generator and associated ionization method
Classifications
U.S. Classification361/230, 315/330, 313/600
International ClassificationH05H1/24, H01J17/02, H01J17/30
Cooperative ClassificationH05H1/24, H01J17/30
European ClassificationH05H1/24, H01J17/30