US2900548A - Plasma generator - Google Patents
Plasma generator Download PDFInfo
- Publication number
- US2900548A US2900548A US589831A US58983156A US2900548A US 2900548 A US2900548 A US 2900548A US 589831 A US589831 A US 589831A US 58983156 A US58983156 A US 58983156A US 2900548 A US2900548 A US 2900548A
- Authority
- US
- United States
- Prior art keywords
- plasma
- electrodes
- discharge
- gas
- generator
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 210000002381 plasma Anatomy 0.000 description 49
- 239000012212 insulator Substances 0.000 description 18
- 239000004020 conductor Substances 0.000 description 15
- 150000002500 ions Chemical class 0.000 description 8
- 238000009413 insulation Methods 0.000 description 7
- 239000003990 capacitor Substances 0.000 description 4
- 238000010891 electric arc Methods 0.000 description 3
- 229910052751 metal Inorganic materials 0.000 description 3
- 239000002184 metal Substances 0.000 description 3
- 238000007493 shaping process Methods 0.000 description 3
- 239000007787 solid Substances 0.000 description 2
- 230000009471 action Effects 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 238000005290 field theory Methods 0.000 description 1
- 239000003574 free electron Substances 0.000 description 1
- 230000000977 initiatory effect Effects 0.000 description 1
- 239000011344 liquid material Substances 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000008439 repair process Effects 0.000 description 1
- 229910052723 transition metal Inorganic materials 0.000 description 1
- 150000003624 transition metals Chemical class 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01T—SPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
- H01T1/00—Details of spark gaps
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/24—Generating plasma
- H05H1/48—Generating plasma using an arc
Definitions
- the present invention relates to method and means for producing a plasma and in particular to the production of a shaped plasma.
- plasma is taken to define a space charge neutralized ionized gas.
- a plasma there are disposed free positively charged ions and a potential balancing number of free electrons with the physical plasma features resembling a conventional are.
- ion source art it is common to generate a plasma from which ions may be extracted and, likewise, in other arts plasmas are employed. It has been found in ion sources employing plasmas that the efiiciency as well as the 'total possible output and various other factors are in large part dependent upon the plasma itself and, in this respect, the plasma density and density gradients as well as plasma geometry are of importance. With regard to the properties with which it is desired to provide a plasma, many ion source criteria are applicable. Thus for pulsed operation it is advantageous to produce a plasma that is capable of accurate timing as to initiation and period, as well as having a readily reproducible size and configuration. As regards the means for plasma generation, it is desired for same to have a low power input for a given output, minimum size and weight, simplicity of construction, and extended period of reliable operation without such as repair or replenishment.
- the present invention provides an improved plasma generator having the above-noted qualities and in general comprises a pair of occluded gas electrodes between which an arc is struck for producing a'plasma and so oriented as to establish a magnetic field advantageously shaping the resultant plasma.
- Figure 1 is a longitudinal sectional view of a preferred embodiment of the invention together with an associated circuit for energization thereof;
- Figure 2 is a transverse sectional view taken at 22 of Fig. 1;
- Figure 3 is a schematic illustration of the establishment of a shaping magnetic field by the plasma generating current.
- the invention generally comprises a pair of metal electrodes loaded with a gas to be ionized, as by occlusion therein, and spaced by insulation. These electrodes are adapted for pulsed energization to produce an are discharge therebetween whereby the gas therein is released therefrom and ionized to form a plasma.
- the electrodes are disposed out of axial alignment so that the arc current path therebetween is inclined with respect to the current path through the electrodes for establishing a magnetic field that expands the plasma and shapes same.
- a solid insulat ing plate or disc 11 formed for example of ceramic, and having a pair of metal electrodes 12 and 13 extending transversely therethrough.
- These electrodes 12 and 13 terminate flush with the outer face 14 of the insulator 11 and extend rearward beyond the insulator for connection to a pair of spaced conductors .16 and 17 as by con" nectors 18 and 19, respectively.
- the electrodes 12 and 13 preferably fit snugly through the insulator and are loaded with a gas to be ionized. This gas loading is best ac: complished with certain metals having an affinity for gas and thus the electrodes may be formed of titaniumor another of the transition metals with gas loading being accomplished in a conventional manner.
- a sheet insulator 21 may be disposed therebetween.
- This sheet insulation 21 preferably extends past the far ends of the conductors or at least past a point where same are bent outwardly away from each other, as shown.
- the unit may be neatly packaged for ease of handling and maximization of insulation by the provision of an enveloping insulation in the form of a cylinder 22 aflixed to the back side of the insulating disc 11 about the conductors 16 and '17 and insulating sheet 21.
- This cylinder 22 may be formed from a liquid material poured about the aforementioned elements and solidified in place -so as to, seal all of the elements into a solid block.
- Energization of the generator may be accomplished with a conventional pulsed circuit such as that shown in Fig. 1.
- the circuit includes a direct current power supply 3'1 with a resistor 32 coupling the positive terminal thereof to the anode of a gaseous discharge tube 33.
- the negative power supply terminal is connected to one of the generator conductors 16 as by a ground line, while the other generator conductor 17 is connected to the-cathode of the tube 33.
- a capacitor 34 is connected across the tube and generator from the tube anode toconductor 16, and for controlling operation of the discharge tube 33 there is provided a trigger pulse generator 36 connected to the tube control electrode. It will be appreciated that with the power supply 31 energized, the capacitor 34 will be charged thereby and, that upon receipt by the tube 33 of a trigger pulse from the pulse generator 36, the tube conducts to connect the capacitor across the plasma generator conductors 16 and 17.
- the generator is adapted for disposition in an evacuated chamber so that the discharge occurs between the electrodes in a high vacuum. Establishment of a discharge between the electrodes releases gas occluded or otherwise stored in the electrodes and as this gas leaves the electrodes it is ionized to produce an arc discharge.
- the ionized gas includes electrons and positive ions which I 3 form a space-charge neutralized discharge or plasma 37.
- substantially all of the plasma is formed of the gas released from the electrodes so that a pure plasma is produced without contamination with ions of ambient gas.
- substantially all gas released is ionized a very dense plasma is produced with only a minute quantity of gas, and further no increase in ambient pressure results from unionized gas.
- the plasma produced is shaped as shown in Fig. 1 by the action of self-generated magnetic fields and in this respect note Fig. 3.
- a discharge current flowing, for example, down electrode 13 and up electrode 12 produces magnetic lines of force about these conductors as indicated. This current also flows across the electrode gap through the plasma as a so-called arc current, so that similar lines of force are produced about the discharge, as shown.
- the magnetic field strength above the discharge is'thus stronger than below the discharge and elementary magnetic field theory shows that there is thus produced a net force F downward on the discharge.
- This force F urges the discharge downward, i.e., expands the plasma axially of the generator into a configuration such as that shown in Fig. 1.
- an advantageous plasma configuration which, for example, is desirable for ion extraction.
- the plasma has other than a straight axis, i.e., that the discharge between electrodes lies on other than a straight line.
- the amount and disposition of the discharge curvature determine the ultimate plasma configuration and variations therein are possible.
- the plasma generator of the present invention is adapted for pulsed operation with each pulse extending for a period determined by the charge on the capacitor 34 and the pulses being initiated by the triggering of the discharge tube 33 from the pulse generator 36.
- each pulse extending for a period determined by the charge on the capacitor 34 and the pulses being initiated by the triggering of the discharge tube 33 from the pulse generator 36.
- a very strong plasma is obtained with a minimum gas expenditure so that suflicient gas supply lies in the electrodes for long term pulsed operation.
- the generator is quite compact and may be made very small particularly in view of the plasma densities produced.
- a plasma generator comprising an insulator having a planar face, a pair of electrodes extending through said insulator flush with said face, a gas supply for supplying gas between said electrodes at said insulator face, and a pulsed circuit connected to said electrodes for providing a pulsed high voltage therebetween to establish an arc discharge, said discharge being curved between electrodes whereby the self-induced magnetic field thereof deforms the discharge outwardly from the insulator face.
- a plasma generator as defined in claim 1 further defined by said electrodes being inclined toward each other so as to be closest together at the planar face of said insulator.
- a plasma generator comprising a pair of closely spaced electrical conductors separated by insulation, an insulator across the first ends of said conductors and having 'an outer face away from same, a pair of electrodes electrically connected one'to each of said conductors adjacent said insulator and extending through said insulator into flush relationship with the outer face thereof, said electrodes being inclined toward each other adjacent the outer face of said insulator, at least one of said electrodes having a gas to be ionized occluded therein whereby electrical energization of said conductors produces a magnetically deformed arc discharge across the outer insulator face between said electrodes, and molded insulation encompassing said conductors and electrodes behind said insulator except for conductor ends adapted for electrical energization.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Plasma Technology (AREA)
- Physical Or Chemical Processes And Apparatus (AREA)
Description
Aug. 18, 1959' w. H, BOSTICK ETAL 2,900,548
- PLASMA GENERATOR Filed June 6, 1956 D.C. TRIGGER 36 POWER 34\ 0 PULSE SUPPLYO GENERATOR INVENTORS.
WINSTON H. BOST/CK VlRG/L G. MC/NTOSH ATTORNEY.
United States Patent PLASMA GENERATOR Application June 6, 1956, Serial No. 589,831
3 Claims. (Cl. 313--131) The present invention relates to method and means for producing a plasma and in particular to the production of a shaped plasma.
At the outset, it is noted that the term plasma, as herein employed, is taken to define a space charge neutralized ionized gas. Within a plasma there are disposed free positively charged ions and a potential balancing number of free electrons with the physical plasma features resembling a conventional are.
In an ion source art it is common to generate a plasma from which ions may be extracted and, likewise, in other arts plasmas are employed. It has been found in ion sources employing plasmas that the efiiciency as well as the 'total possible output and various other factors are in large part dependent upon the plasma itself and, in this respect, the plasma density and density gradients as well as plasma geometry are of importance. With regard to the properties with which it is desired to provide a plasma, many ion source criteria are applicable. Thus for pulsed operation it is advantageous to produce a plasma that is capable of accurate timing as to initiation and period, as well as having a readily reproducible size and configuration. As regards the means for plasma generation, it is desired for same to have a low power input for a given output, minimum size and weight, simplicity of construction, and extended period of reliable operation without such as repair or replenishment.
The present invention provides an improved plasma generator having the above-noted qualities and in general comprises a pair of occluded gas electrodes between which an arc is struck for producing a'plasma and so oriented as to establish a magnetic field advantageously shaping the resultant plasma.
It is an object of the present invention to provide a plasma generator producing a magnetically shaped plasma of advantageous configuration.
It is another object of the present invention to provide a plasma generator of high output and small size.
It is a further object of the present invention to provide a plasma generator producing a shaping magnetic field with the plasma generating current.
It is yet another object of the present invention to provide an improved compact occluded-gas plasma generator.
Numerous other advantages and possible objects of the present invention'will become apparent to those skilled in the art from the following description taken together with the attached drawing, wherein:
'Figure 1 is a longitudinal sectional view of a preferred embodiment of the invention together with an associated circuit for energization thereof;
Figure 2 is a transverse sectional view taken at 22 of Fig. 1; and
Figure 3 is a schematic illustration of the establishment of a shaping magnetic field by the plasma generating current.
The invention generally comprises a pair of metal electrodes loaded with a gas to be ionized, as by occlusion therein, and spaced by insulation. These electrodes are adapted for pulsed energization to produce an are discharge therebetween whereby the gas therein is released therefrom and ionized to form a plasma. The electrodes are disposed out of axial alignment so that the arc current path therebetween is inclined with respect to the current path through the electrodes for establishing a magnetic field that expands the plasma and shapes same.
' Considering now a preferred embodiment of the invention in some detail and referring to Figs. 1 and 2 of the drawings, there will be seen to be provided a solid insulat ing plate or disc 11, formed for example of ceramic, and having a pair of metal electrodes 12 and 13 extending transversely therethrough. These electrodes 12 and 13 terminate flush with the outer face 14 of the insulator 11 and extend rearward beyond the insulator for connection to a pair of spaced conductors .16 and 17 as by con" nectors 18 and 19, respectively. The electrodes 12 and 13 preferably fit snugly through the insulator and are loaded with a gas to be ionized. This gas loading is best ac: complished with certain metals having an affinity for gas and thus the electrodes may be formed of titaniumor another of the transition metals with gas loading being accomplished in a conventional manner.
Inasmuch as a relatively large potential is to be impressed between the electrodes 12 and 13 in order to establish an arc therebetween, it is necessary to provide adequate insulation between the electrode conductors and to this end a sheet insulator 21 may be disposed therebetween. This sheet insulation 21 preferably extends past the far ends of the conductors or at least past a point where same are bent outwardly away from each other, as shown. The unit may be neatly packaged for ease of handling and maximization of insulation by the provision of an enveloping insulation in the form of a cylinder 22 aflixed to the back side of the insulating disc 11 about the conductors 16 and '17 and insulating sheet 21. This cylinder 22 may be formed from a liquid material poured about the aforementioned elements and solidified in place -so as to, seal all of the elements into a solid block.
, Energization of the generator may be accomplished with a conventional pulsed circuit such as that shown in Fig. 1. The circuit includes a direct current power supply 3'1 with a resistor 32 coupling the positive terminal thereof to the anode of a gaseous discharge tube 33. The negative power supply terminal is connected to one of the generator conductors 16 as by a ground line, while the other generator conductor 17 is connected to the-cathode of the tube 33. A capacitor 34 is connected across the tube and generator from the tube anode toconductor 16, and for controlling operation of the discharge tube 33 there is provided a trigger pulse generator 36 connected to the tube control electrode. It will be appreciated that with the power supply 31 energized, the capacitor 34 will be charged thereby and, that upon receipt by the tube 33 of a trigger pulse from the pulse generator 36, the tube conducts to connect the capacitor across the plasma generator conductors 16 and 17.
With regard to operation of the plasma generator, the application of a high voltage pulse across the conductors 16 and 17, as above noted, produces a large potential difference between the electrodes 12 and 13 at the insulator face 14. This potential is of suflicient magnitude to establish a discharge between the electrodes 12 and 13 across the face 14 of the insulator 11. Note at this point that the generator is adapted for disposition in an evacuated chamber so that the discharge occurs between the electrodes in a high vacuum. Establishment of a discharge between the electrodes releases gas occluded or otherwise stored in the electrodes and as this gas leaves the electrodes it is ionized to produce an arc discharge. The ionized gas includes electrons and positive ions which I 3 form a space-charge neutralized discharge or plasma 37. As the discharge occurs in a high vacuum substantially all of the plasma is formed of the gas released from the electrodes so that a pure plasma is produced without contamination with ions of ambient gas. As substantially all gas released is ionized a very dense plasma is produced with only a minute quantity of gas, and further no increase in ambient pressure results from unionized gas.
The plasma produced is shaped as shown in Fig. 1 by the action of self-generated magnetic fields and in this respect note Fig. 3. A discharge current flowing, for example, down electrode 13 and up electrode 12 produces magnetic lines of force about these conductors as indicated. This current also flows across the electrode gap through the plasma as a so-called arc current, so that similar lines of force are produced about the discharge, as shown. It will be noted that as the current flow bends in the discharge area from a downward direction in elec trode 13 to an upward direction in electrode 12, the lines of force are closer together above the discharge than below. The magnetic field strength above the discharge is'thus stronger than below the discharge and elementary magnetic field theory shows that there is thus produced a net force F downward on the discharge. This force F urges the discharge downward, i.e., expands the plasma axially of the generator into a configuration such as that shown in Fig. 1. There is thus produced an advantageous plasma configuration which, for example, is desirable for ion extraction.
In order to produce an unbalanced self-induced magnetic field for deforming the plasma it is necessary that the plasma has other than a straight axis, i.e., that the discharge between electrodes lies on other than a straight line. The amount and disposition of the discharge curvature determine the ultimate plasma configuration and variations therein are possible. In the illustrated embodiment there is shown a portion of an insulator interposed between the electrodes to prevent the discharge from pass ing directly therebetween so that the original discharge is curved. With the original discharge curved in space, it Will induce an unbalanced magnetic field to deform the resultant plasma as set forth above. It will be appreciated that various geometries are possible to provide a desired plasma configuration.
The plasma generator of the present invention is adapted for pulsed operation with each pulse extending for a period determined by the charge on the capacitor 34 and the pulses being initiated by the triggering of the discharge tube 33 from the pulse generator 36. As sub stantially all of the gas released from the electrodes 12 and 13 is ionized during each discharge, a very strong plasma is obtained with a minimum gas expenditure so that suflicient gas supply lies in the electrodes for long term pulsed operation. Additionally the generator is quite compact and may be made very small particularly in view of the plasma densities produced.
While the invention has been disclosed with respect to a single preferred embodiment, it will be apparent to those skilled in the art that numerous variations and modifications may be made within the spirit and scope of the invention and thus it is not intended to limit the invention except as defined in the following claims.
What is claimed is:
1. A plasma generator comprising an insulator having a planar face, a pair of electrodes extending through said insulator flush with said face, a gas supply for supplying gas between said electrodes at said insulator face, and a pulsed circuit connected to said electrodes for providing a pulsed high voltage therebetween to establish an arc discharge, said discharge being curved between electrodes whereby the self-induced magnetic field thereof deforms the discharge outwardly from the insulator face.
2. A plasma generator as defined in claim 1 further defined by said electrodes being inclined toward each other so as to be closest together at the planar face of said insulator.
3. A plasma generator comprising a pair of closely spaced electrical conductors separated by insulation, an insulator across the first ends of said conductors and having 'an outer face away from same, a pair of electrodes electrically connected one'to each of said conductors adjacent said insulator and extending through said insulator into flush relationship with the outer face thereof, said electrodes being inclined toward each other adjacent the outer face of said insulator, at least one of said electrodes having a gas to be ionized occluded therein whereby electrical energization of said conductors produces a magnetically deformed arc discharge across the outer insulator face between said electrodes, and molded insulation encompassing said conductors and electrodes behind said insulator except for conductor ends adapted for electrical energization.
References (Iited in the file of this patent UNITED STATES PATENTS Watters June 24, 1958-
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US589831A US2900548A (en) | 1956-06-06 | 1956-06-06 | Plasma generator |
| GB17156/57A GB821744A (en) | 1956-06-06 | 1957-05-30 | Plasma generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US589831A US2900548A (en) | 1956-06-06 | 1956-06-06 | Plasma generator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US2900548A true US2900548A (en) | 1959-08-18 |
Family
ID=24359731
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US589831A Expired - Lifetime US2900548A (en) | 1956-06-06 | 1956-06-06 | Plasma generator |
Country Status (2)
| Country | Link |
|---|---|
| US (1) | US2900548A (en) |
| GB (1) | GB821744A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3335311A (en) * | 1965-02-01 | 1967-08-08 | Gen Electric | Glow discharge device having parallel permanent magnetic rod electrodes |
| US3389289A (en) * | 1964-09-07 | 1968-06-18 | Bensussan Andre Marc | Plasma gun having a hydrogen storing reservoir |
| FR2648001A1 (en) * | 1989-05-31 | 1990-12-07 | Breda Jean Pierre | Direct current supply for plasma electrodes and process for regenerating a plasma |
| US5458754A (en) * | 1991-04-22 | 1995-10-17 | Multi-Arc Scientific Coatings | Plasma enhancement apparatus and method for physical vapor deposition |
Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2168206A (en) * | 1938-02-11 | 1939-08-01 | Jr Arthur C Hastings | Spark plug |
| US2481887A (en) * | 1947-07-23 | 1949-09-13 | Smitsvonk Nv | Spark gap and lamp |
| US2596865A (en) * | 1950-07-03 | 1952-05-13 | Allis Chalmers Mfg Co | Arc chute utilizing staggered u-shaped conductive members |
| US2677771A (en) * | 1953-03-05 | 1954-05-04 | Atomic Energy Commission | Ion source |
| US2743370A (en) * | 1952-11-26 | 1956-04-24 | Bendix Aviat Corp | Mass spectrometer |
| US2754422A (en) * | 1952-07-30 | 1956-07-10 | Edward J Lofgren | Source of highly stripped ions |
| US2840742A (en) * | 1954-07-07 | 1958-06-24 | Gen Electric | Spark projection ignition device |
-
1956
- 1956-06-06 US US589831A patent/US2900548A/en not_active Expired - Lifetime
-
1957
- 1957-05-30 GB GB17156/57A patent/GB821744A/en not_active Expired
Patent Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2168206A (en) * | 1938-02-11 | 1939-08-01 | Jr Arthur C Hastings | Spark plug |
| US2481887A (en) * | 1947-07-23 | 1949-09-13 | Smitsvonk Nv | Spark gap and lamp |
| US2596865A (en) * | 1950-07-03 | 1952-05-13 | Allis Chalmers Mfg Co | Arc chute utilizing staggered u-shaped conductive members |
| US2754422A (en) * | 1952-07-30 | 1956-07-10 | Edward J Lofgren | Source of highly stripped ions |
| US2743370A (en) * | 1952-11-26 | 1956-04-24 | Bendix Aviat Corp | Mass spectrometer |
| US2677771A (en) * | 1953-03-05 | 1954-05-04 | Atomic Energy Commission | Ion source |
| US2840742A (en) * | 1954-07-07 | 1958-06-24 | Gen Electric | Spark projection ignition device |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3389289A (en) * | 1964-09-07 | 1968-06-18 | Bensussan Andre Marc | Plasma gun having a hydrogen storing reservoir |
| US3335311A (en) * | 1965-02-01 | 1967-08-08 | Gen Electric | Glow discharge device having parallel permanent magnetic rod electrodes |
| FR2648001A1 (en) * | 1989-05-31 | 1990-12-07 | Breda Jean Pierre | Direct current supply for plasma electrodes and process for regenerating a plasma |
| US5458754A (en) * | 1991-04-22 | 1995-10-17 | Multi-Arc Scientific Coatings | Plasma enhancement apparatus and method for physical vapor deposition |
| US6139964A (en) * | 1991-04-22 | 2000-10-31 | Multi-Arc Inc. | Plasma enhancement apparatus and method for physical vapor deposition |
Also Published As
| Publication number | Publication date |
|---|---|
| GB821744A (en) | 1959-10-14 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5502354A (en) | Direct current energized pulse generator utilizing autogenous cyclical pulsed abnormal glow discharges | |
| JPS6132508B2 (en) | ||
| Harrison | Investigation of the perveances and beam profiles of an aperture disk emission system | |
| Liu et al. | Experimental investigation on the velocity of cathode spots in a vacuum arc with high di/dt | |
| US2883580A (en) | Pulsed ion source | |
| US2447377A (en) | Device for regulating electrical discharge | |
| Anders et al. | High ion charge states in a high‐current, short‐pulse, vacuum arc ion source | |
| US2900548A (en) | Plasma generator | |
| GB1476293A (en) | Continuous ionization injector for low pressure gas dis charge device | |
| GB1101293A (en) | High output duoplasmatron-type ion source | |
| Tsai et al. | Plasma studies on a duoPIGatron ion source | |
| JPH0512727B2 (en) | ||
| US3453474A (en) | Plasma arc electrodes | |
| US2953718A (en) | Apparatus and method for generating high temperatures | |
| US4135093A (en) | Use of predissociation to enhance the atomic hydrogen ion fraction in ion sources | |
| US2939048A (en) | Apparatus for creating extremely high temperatures | |
| US3143680A (en) | Ion accelerators | |
| JPH07169425A (en) | Ion source | |
| RU2045103C1 (en) | Duoplasmatron | |
| Tanaka et al. | Effect of magnetic field on the characteristics of a hollow cathode ion source | |
| Petr et al. | Erosion of spark gap electrodes | |
| JPS6054200A (en) | High voltage generator by electric explosion | |
| US2595716A (en) | Gaseous discharge device | |
| Gavrilov et al. | Characteristics of an ion source with a plasma cathode and a multipole magnetic system for confining fast electrons | |
| Perkins et al. | Ion source electrode biasing technique for microsecond beam pulse rise times |