US2211668A - Electronic device - Google Patents
Electronic device Download PDFInfo
- Publication number
- US2211668A US2211668A US183893A US18389338A US2211668A US 2211668 A US2211668 A US 2211668A US 183893 A US183893 A US 183893A US 18389338 A US18389338 A US 18389338A US 2211668 A US2211668 A US 2211668A
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- US
- United States
- Prior art keywords
- discharge
- magnetic field
- cathode
- anode
- pressure
- 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
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Classifications
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- 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
- H05H3/00—Production or acceleration of neutral particle beams, e.g. molecular or atomic beams
- H05H3/06—Generating neutron beams
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21G—CONVERSION OF CHEMICAL ELEMENTS; RADIOACTIVE SOURCES
- G21G4/00—Radioactive sources
- G21G4/02—Neutron sources
Definitions
- neutrons can be produced during the resulting nucleus reactionrI-Iereinafter the material against which the ions are projected will be referred to as a disc of impact.
- Such devices are also useful for effecting other nucleus reactions. For instance, they may be used to produce c particles by bombardment of a lithium compound with hydrogen ions (protons), according to the reaction H +Li +2He or according to the reaction H +Li 2He In the last-mentioned case lithium is consequently bombarded with ions of heavy hydrogen (deutons).
- the object of my invention is to overcome this disadvantage, and to simplify devices of the above type.
- the device according to the invention comprises an electric discharge tube having a plu- 5 rality of interconnected portions in which the pressure is the same.
- the ions are produced in a glow discharge taking place in one portion and are accelerated in another portion, and strike finally a disc of impact, which contains a definite v(i5 compound to'produce the nucleus reaction.
- the glow-discharge electrodes are shaped as fiat'plates arranged parallel to each other; and the magnetic field is so arranged that the magnetic lines of force extend perpen- .25 dicularly to these plates.
- ignition voltage which, of course, is also an important advantage.
- an apertured an- 30 .ode may be arranged centrally between two cathodes, of which one is also apertured for the passage of the ions produced.
- the anode may be a cylinder or ring whose axis extends normally to 35 the surface of the cathodes and parallel to'the magnetic lines of force.
- the gas in which the glow-discharge is. struck and the substance bombarded by the ions produced are different.
- the glow discharge may be struck in heavy hydrogenand the ions produced may be projected against a disc of impact containing heavy hydrogen or lithium in some compound or other; for example a compound of zirconium and heavy hydrogen.
- the discharge device illustrated in the drawing comprises an envelope having a vitreous portion I, two metal rings l and I8 for instance of chrome iron, a connecting vitreous portion [9,-
- Portion which forms a glow-discharge chamber is provided with a re,-'
- a lead support 4 Sealed in pinch 3 is a lead support 4 which carries on its lower end a cathode 5 in the form of a'plate.
- Beneath cathode 5 is an anode 1 in the form of a metal plate member, for instance of constantan provided with a central aperture 8.
- Anode is supported at one side by a wire 22 sealed in the end of projection 20 and onit's opposite side by a wire 23 sealed into the end of projection 2
- Supported by wires 22 and 23 are two vitreous cap-shaped members. 6 which extend over the ends of projections 20 and 2
- a second cathode 9 in the form of a metal cylinder, for instance of iron, whose ends are partly closed to form apertures 24 and 29.
- anaccelerating electrode ll in'the form of a metal cylinder, 'for instance of iron, having partly closed ends is supported from ring l8.
- Vitreous portion 2.forms a pinchll from which is supported a dis'c'of impact I2provided with a lead I3.
- the disc I2 may contain heavy hy drogen or lithium in'some compound for example a compound of'zirconium and heavy hydrogen.
- compound is used not only a chemical compound is meant but also a'body which contains a gas absorbed'in it or adsorbed to it.
- the tube is supported by a plate l5 of suitable insulating material such as Bakelite, and a suitable insulating cement 16, such .as'pecine or similar material, is used to cover the surface of portion [9 and to hold'the tube'to plate [5.
- a magnet coil Surrounding the central portion of the'tube is a magnet coil" I! which produces in th'edischar'ge space a magnetic field whose lines of force extend substantially normally't'o the surface of cathode 5 and anode I. v
- .resistance may be insertedin the supply lead I3.
- resistance 26 is connected between" lead l3 and the high-tension source whereas the ring I8 is directly-connected to this high-tensionsource.
- the ions produced in the glow-discharge chamber pass through'apertures 24 and 29 and, after being accelerated by electrode ll,.. strike thedisc of impact l2 whereby neutronsare produced.
- a voltage of about 15 k. v. may be applied betweencathodes 5 and 9 and anode I, a voltage of about 60 k. vQmay be applied between cathode 9 and electrode II, and
- resistance 26 may have a value of about 1 megohm.
- the tube has a filling of heavy hydrogen at a pressure of about mm.
- coil 1 should produce a magnetic field having a value of about 800 gauss.
- the current may be of the order of magnitude of about 1 ma. in the main discharge and of the order of 0.1 ma. in the disc of impact I2.
- the pressure of gas filling within the tube becomes too high or too low due to the discharge, it may be readjusted in a known manner, for instance by means of palladium tubes or by means of tubes of zirconium which can absorb hydrogen as well as heavy hydrogen.
- the pressure of the gas within a tube according to the invention may be advantageously measured and supervised by means of the device described in my copending U. S. patent application Ser. No. 106,915, filed October 21, 1936, which device utilizes the fact that at a low pressure and by using a suitable magnetic field, a glow discharge can be produced and the intensity of the current of this discharge used as a measure of the pressure.
- This may, for instance, be effected by sealing to the extension 29 of the tube of Fig. 1, a separate tube in which a glow discharge is struck at a low pressure in .a suitable magnetic field.
- the magnetic field and the anode voltage of this separate tube are so selected that, for the pressure range used, the intensity of the glow discharge current is a'suitable measure of the value of the gas pressure.
- a device for effecting nucleus reactions comprising an envelope, a gaseous filling within said envelope, means within said envelope for producing a glow discharge comprising a cathode having a plate-shaped portion, a second cathode having a plate-shaped portion provided with an aperture and arranged parallel to said first por ing a glow discharge comprising a cathode having a plate-shaped portion, a second cathode having an apertured plate-shaped portion substantially parallel to said first portion, and an anode consisting of an annular member arranged with its axis normal to said cathode portions, a disc of impact withinsaid envelope,,means for accelerating the ions produced in the discharge toward the disc of impact to effect a nucleus .reaction, and means to; produce a' magnetic field whose .lines of force extend substantially normal to .said cathode portions and parallel to the axis of the anode.
Description
F. M. PENNING ELECTRONIC DEVICE Filed Jan. 7, 1938 Aug. 13, 1940.
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Arrokusy.
Patented Aug. 13, 1940 vArea ELECTRONIC DEVICE Frans Michel Penning, Eindhoven, Netherlands, assignor, by mesne assignments, to Hartford 1 National Bank andr'lfrust Company, Hartford,
Conn, as trustee Application January 7, 1938, Serial No. 183,893 In the Netherlands January 23, 1937 2 Claims.
ii) which contains, for example, heavy hydrogen,
lithium and the like, neutrons can be produced during the resulting nucleus reactionrI-Iereinafter the material against which the ions are projected will be referred to as a disc of impact.
ii Such devices are also useful for effecting other nucleus reactions. For instance, they may be used to produce c particles by bombardment of a lithium compound with hydrogen ions (protons), according to the reaction H +Li +2He or according to the reaction H +Li 2He In the last-mentioned case lithium is consequently bombarded with ions of heavy hydrogen (deutons).
To produce neutrons in the above manner, de-
vices are known in which a stream of ions of heavy hydrogen produced in a glow discharge space is passed into a second space of the device in which the pressure is lower than in the glowdischarge space. The ions are accelerated in the second space by applying a much higher potential, and-they finally strike a disc of impact containing, for instance, a compound of heavy hydrogen. Neutrons are produced due to meeting 'of heavy hydrogen with a definite constituent of this compound, for instance of heavy hydrogen or lithium, according to the nucleus re-' actions which are already known.
Although such prior-art; devices give satisfactory results, they have the serious disadvantage, that it is necessary to maintain diiferent pressures in two communicating spaces, and for this purpose at least one of these spaces must be continuously connected to a vacuum pump during the operation of the device.
5 The object of my invention is to overcome this disadvantage, and to simplify devices of the above type.
The device according to the invention comprises an electric discharge tube having a plu- 5 rality of interconnected portions in which the pressure is the same. The ions are produced in a glow discharge taking place in one portion and are accelerated in another portion, and strike finally a disc of impact, which contains a definite v(i5 compound to'produce the nucleus reaction. I
influence the glow discharge by a magnetic field,
. and give this magnetic field such a configuration,
and so shape the glow-discharge electrodes and so space the same with respect to the magnetic field that the discharge current is much stronger 5 than it would be were the magnetic field not present. By so arranging the magnetic field between the cathode and the anode that the electrons emitted from the cathode must cover a much 10 longer path than that which they would cover without the magnetic field, the discharge 'current is as strong as it would be without a magnetic field with a much higher pressure of the gas. A second advantage of this arrangement 5 is thefact that it is possible to strike the glow discharge which would be impossible Without a magnetic field.
This efiect of apparent pressure increase can be realized in various manners by means of the 20 magnetic field. According to one embodiment of'the invention the glow-discharge electrodes are shaped as fiat'plates arranged parallel to each other; and the magnetic field is so arranged that the magnetic lines of force extend perpen- .25 dicularly to these plates. Thus not only an apparent pressureincrease is obtained during operation of the tube, butalso a. decrease in: ignition voltage which, of course, is also an important advantage. For example an apertured an- 30 .ode may be arranged centrally between two cathodes, of which one is also apertured for the passage of the ions produced.
In another embodiment the anode may be a cylinder or ring whose axis extends normally to 35 the surface of the cathodes and parallel to'the magnetic lines of force.
In the above cases the electrons move to and fro between the cathodes along curved paths, and generally reach the anode only after having 40 repeatedly moved back and forth. Consequently these paths are appreciably longer than the direct path from the cathode to the anode, and as a result the efiect produced is equivalent to an increase in the gas pressure. 5
In accordance with the variousapplications of a device according to the present invention, the gas in which the glow-discharge is. struck and the substance bombarded by the ions produced are different. When the device is used for producing neutrons the glow discharge may be struck in heavy hydrogenand the ions produced may be projected against a disc of impact containing heavy hydrogen or lithium in some compound or other; for example a compound of zirconium and heavy hydrogen.
' In order that the invention may be clearly understood and readily carried into effect, I shall describe the same more fully with reference to the accompanying drawing which is a sectionized view of a device according to the invention.
The discharge device illustrated in the drawing comprises an envelope having a vitreous portion I, two metal rings l and I8 for instance of chrome iron, a connecting vitreous portion [9,-
and a vitreous portion 2. Portion which forms a glow-discharge chamber, is provided with a re,-'
entrant part forming a pinch 3 and two tubular projections 20 and 2|. Sealed in pinch 3 is a lead support 4 which carries on its lower end a cathode 5 in the form of a'plate.
Beneath cathode 5 is an anode 1 in the form of a metal plate member, for instance of constantan provided with a central aperture 8. Anode is supported at one side by a wire 22 sealed in the end of projection 20 and onit's opposite side by a wire 23 sealed into the end of projection 2| and extending therethrough to serve as a lead. Supported by wires 22 and 23 are two vitreous cap-shaped members. 6 which extend over the ends of projections 20 and 2| and serve to protect wires 22 and 23"from'the discharge.
Supported from ring I U is a second cathode 9 in the form of a metal cylinder, for instance of iron, whose ends are partly closed to form apertures 24 and 29. In a similar manner anaccelerating electrode ll in'the form ofa metal cylinder, 'for instance of iron, having partly closed ends is supported from ring l8. I
Vitreous portion 2.forms a pinchll from which is supported a dis'c'of impact I2provided with a lead I3. The disc I2 may contain heavy hy drogen or lithium in'some compound for example a compound of'zirconium and heavy hydrogen. Wherever throughout this specification the word "compound is used not only a chemical compound is meant but also a'body which contains a gas absorbed'in it or adsorbed to it.
To prevent sparking over between rings Ill and I8, between which a potential difierence of for instance 60k. v. and more may beset u'p dur-' ing operation, the tube is supported by a plate l5 of suitable insulating material such as Bakelite, and a suitable insulating cement 16, such .as'pecine or similar material, is used to cover the surface of portion [9 and to hold'the tube'to plate [5.
Surrounding the central portion of the'tube is a magnet coil" I! which produces in th'edischar'ge space a magnetic field whose lines of force extend substantially normally't'o the surface of cathode 5 and anode I. v
To reduce the detrimental effect of secondary electrons merging from the disc of impact [2; a
.resistance may be insertedin the supply lead I3.
As shown in the drawinga resistance 26 is connected between" lead l3 and the high-tension source whereas the ring I8 is directly-connected to this high-tensionsource.
Duringthe operation of the device the ions produced in the glow-discharge chamber pass through'apertures 24 and 29 and, after being accelerated by electrode ll,.. strike thedisc of impact l2 whereby neutronsare produced.
a; particular example a voltage of about 15 k. v. may be applied betweencathodes 5 and 9 and anode I, a voltage of about 60 k. vQmay be applied between cathode 9 and electrode II, and
resistance 26 may have a value of about 1 megohm. During operation the tube has a filling of heavy hydrogen at a pressure of about mm. Under such conditions coil 1 should produce a magnetic field having a value of about 800 gauss. The current may be of the order of magnitude of about 1 ma. in the main discharge and of the order of 0.1 ma. in the disc of impact I2.
If the pressure of gas filling within the tube becomes too high or too low due to the discharge, it may be readjusted in a known manner, for instance by means of palladium tubes or by means of tubes of zirconium which can absorb hydrogen as well as heavy hydrogen.
The pressure of the gas within a tube according to the invention may be advantageously measured and supervised by means of the device described in my copending U. S. patent application Ser. No. 106,915, filed October 21, 1936, which device utilizes the fact that at a low pressure and by using a suitable magnetic field, a glow discharge can be produced and the intensity of the current of this discharge used as a measure of the pressure. This may, for instance, be effected by sealing to the extension 29 of the tube of Fig. 1, a separate tube in which a glow discharge is struck at a low pressure in .a suitable magnetic field. As more fully described in the above application the magnetic field and the anode voltage of this separate tube are so selected that, for the pressure range used, the intensity of the glow discharge current is a'suitable measure of the value of the gas pressure.
While I have described my invention in connection with specific examples and applications, I do not wish to be limited thereto but desire the appended claims to be construed as broadly as permissible in view of the prior art.
What I claim is:
1 A device for effecting nucleus reactions comprising an envelope, a gaseous filling within said envelope, means within said envelope for producing a glow discharge comprising a cathode having a plate-shaped portion, a second cathode having a plate-shaped portion provided with an aperture and arranged parallel to said first por ing a glow discharge comprising a cathode having a plate-shaped portion, a second cathode having an apertured plate-shaped portion substantially parallel to said first portion, and an anode consisting of an annular member arranged with its axis normal to said cathode portions, a disc of impact withinsaid envelope,,means for accelerating the ions produced in the discharge toward the disc of impact to effect a nucleus .reaction, and means to; produce a' magnetic field whose .lines of force extend substantially normal to .said cathode portions and parallel to the axis of the anode.
, FRANS MICHEL PENNTNG.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NL491766X | 1937-01-23 |
Publications (1)
Publication Number | Publication Date |
---|---|
US2211668A true US2211668A (en) | 1940-08-13 |
Family
ID=19786693
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US183893A Expired - Lifetime US2211668A (en) | 1937-01-23 | 1938-01-07 | Electronic device |
Country Status (4)
Country | Link |
---|---|
US (1) | US2211668A (en) |
FR (1) | FR832356A (en) |
GB (1) | GB491766A (en) |
NL (1) | NL50089C (en) |
Cited By (38)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2735019A (en) * | 1952-07-02 | 1956-02-14 | Particle accelerator | |
US2786143A (en) * | 1955-08-16 | 1957-03-19 | Ruby Lawrence | Source unit for producing ionized gas |
US2906903A (en) * | 1954-04-07 | 1959-09-29 | Elizabeth R Graves | Low voltage 14 mev. neutron source |
US2914677A (en) * | 1954-03-08 | 1959-11-24 | Schlumberger Well Surv Corp | Well logging apparatus |
US2926271A (en) * | 1953-07-20 | 1960-02-23 | Tracerlab Inc | Apparatus for producing neutrons |
US2933611A (en) * | 1960-04-19 | Neutron source | ||
US2951945A (en) * | 1954-05-26 | 1960-09-06 | Schlumberger Well Surv Corp | Renewable target |
US2957096A (en) * | 1954-06-10 | 1960-10-18 | Nels K Bernander | Neutron source |
US2964634A (en) * | 1960-12-13 | Apparatus for producing neutrons | ||
US2964665A (en) * | 1955-12-01 | 1960-12-13 | Tracerlab Inc | Pressure control system |
US2967245A (en) * | 1954-03-08 | 1961-01-03 | Schlumberger Well Surv Corp | Neutron source for well logging apparatus |
US2973444A (en) * | 1952-04-09 | 1961-02-28 | Schlumberger Well Surv Corp | Neutron source for well logging apparatus |
US2983820A (en) * | 1954-03-08 | 1961-05-09 | Schlumberger Well Surv Corp | Well logging apparatus |
US2983834A (en) * | 1955-05-09 | 1961-05-09 | Armour Res Found | Neutron discharge tube |
US2988671A (en) * | 1958-06-30 | 1961-06-13 | Schlumberger Well Surv Corp | Particle accelerating system |
US2991367A (en) * | 1949-07-30 | 1961-07-04 | Well Surveys Inc | Neutron source |
US3014132A (en) * | 1959-01-02 | 1961-12-19 | High Voltage Engineering Corp | Loss current diminisher for compact neutron source |
US3020408A (en) * | 1955-11-14 | 1962-02-06 | Philip W Martin | Nuclear analytical apparatus |
US3047720A (en) * | 1956-12-07 | 1962-07-31 | Jersey Prod Res Co | Helium 3 scintillation neutron detector |
US3071690A (en) * | 1949-07-30 | 1963-01-01 | Well Surveys Inc | Well logging radiation sources |
US3082326A (en) * | 1954-03-08 | 1963-03-19 | Schlumberger Well Surv Corp | Neutron generating apparatus |
US3104322A (en) * | 1958-02-10 | 1963-09-17 | High Voltage Engineering Corp | Compact neutron source |
US3112401A (en) * | 1957-09-27 | 1963-11-26 | Philips Corp | Shielding to confine magnetic field to ion source area of a neutron generator |
US3215836A (en) * | 1952-04-09 | 1965-11-02 | Schlumberger Well Surv Corp | Apparatus and methods relating to production of neutron radiation |
US3283193A (en) * | 1962-05-14 | 1966-11-01 | Ellison Company | Ion source having electrodes of catalytic material |
DE1248180B (en) * | 1954-05-28 | 1967-08-24 | Well Surveys Inc | Neutron source for a geophysical borehole survey device |
US3359422A (en) * | 1954-10-28 | 1967-12-19 | Gen Electric | Arc discharge atomic particle source for the production of neutrons |
US4529571A (en) * | 1982-10-27 | 1985-07-16 | The United States Of America As Represented By The United States Department Of Energy | Single-ring magnetic cusp low gas pressure ion source |
US4996017A (en) * | 1982-03-01 | 1991-02-26 | Halliburton Logging Services Inc. | Neutron generator tube |
US5215703A (en) * | 1990-08-31 | 1993-06-01 | U.S. Philips Corporation | High-flux neutron generator tube |
US20070237281A1 (en) * | 2005-08-30 | 2007-10-11 | Scientific Drilling International | Neutron generator tube having reduced internal voltage gradients and longer lifetime |
US20080232532A1 (en) * | 2005-04-29 | 2008-09-25 | Larsen Lewis G | Apparatus and Method for Generation of Ultra Low Momentum Neutrons |
US20120063558A1 (en) * | 2009-11-16 | 2012-03-15 | Jani Reijonen | Floating Intermediate Electrode Configuration for Downhole Nuclear Radiation Generator |
US9756714B2 (en) | 2013-12-31 | 2017-09-05 | Halliburton Energy Services, Inc. | Nano-emitter ion source neutron generator |
US9835760B2 (en) | 2013-12-31 | 2017-12-05 | Halliburton Energy Services, Inc. | Tritium-tritium neutron generator and logging method |
WO2018195436A1 (en) | 2017-04-20 | 2018-10-25 | Philip Teague | Near-field sensitivity of formation and cement porosity measurements with radial resolution in a borehole |
US10408968B2 (en) | 2013-12-31 | 2019-09-10 | Halliburton Energy Services, Inc. | Field emission ion source neutron generator |
US11558037B2 (en) | 2020-12-10 | 2023-01-17 | Gary Hanington | High efficiency high voltage pulse generator |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2576600A (en) * | 1945-07-03 | 1951-11-27 | Alfred O Hanson | Device for generating neutrons |
US2816242A (en) * | 1953-05-19 | 1957-12-10 | Schlumberger Well Surv Corp | Neutron sources |
US2905826A (en) * | 1953-09-30 | 1959-09-22 | Socony Mobil Oil Co Inc | Measurement of gamma ray energy due to inelastic neutron scattering |
-
0
- NL NL50089D patent/NL50089C/xx active
-
1938
- 1938-01-07 US US183893A patent/US2211668A/en not_active Expired - Lifetime
- 1938-01-20 GB GB1948/38A patent/GB491766A/en not_active Expired
- 1938-01-21 FR FR832356D patent/FR832356A/en not_active Expired
Cited By (39)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2933611A (en) * | 1960-04-19 | Neutron source | ||
US2964634A (en) * | 1960-12-13 | Apparatus for producing neutrons | ||
US2991367A (en) * | 1949-07-30 | 1961-07-04 | Well Surveys Inc | Neutron source |
US3071690A (en) * | 1949-07-30 | 1963-01-01 | Well Surveys Inc | Well logging radiation sources |
US3215836A (en) * | 1952-04-09 | 1965-11-02 | Schlumberger Well Surv Corp | Apparatus and methods relating to production of neutron radiation |
US2973444A (en) * | 1952-04-09 | 1961-02-28 | Schlumberger Well Surv Corp | Neutron source for well logging apparatus |
US2735019A (en) * | 1952-07-02 | 1956-02-14 | Particle accelerator | |
US2926271A (en) * | 1953-07-20 | 1960-02-23 | Tracerlab Inc | Apparatus for producing neutrons |
US2983820A (en) * | 1954-03-08 | 1961-05-09 | Schlumberger Well Surv Corp | Well logging apparatus |
US3082326A (en) * | 1954-03-08 | 1963-03-19 | Schlumberger Well Surv Corp | Neutron generating apparatus |
US2967245A (en) * | 1954-03-08 | 1961-01-03 | Schlumberger Well Surv Corp | Neutron source for well logging apparatus |
US2914677A (en) * | 1954-03-08 | 1959-11-24 | Schlumberger Well Surv Corp | Well logging apparatus |
US2906903A (en) * | 1954-04-07 | 1959-09-29 | Elizabeth R Graves | Low voltage 14 mev. neutron source |
US2951945A (en) * | 1954-05-26 | 1960-09-06 | Schlumberger Well Surv Corp | Renewable target |
DE1248180B (en) * | 1954-05-28 | 1967-08-24 | Well Surveys Inc | Neutron source for a geophysical borehole survey device |
US2957096A (en) * | 1954-06-10 | 1960-10-18 | Nels K Bernander | Neutron source |
US3359422A (en) * | 1954-10-28 | 1967-12-19 | Gen Electric | Arc discharge atomic particle source for the production of neutrons |
US2983834A (en) * | 1955-05-09 | 1961-05-09 | Armour Res Found | Neutron discharge tube |
US2786143A (en) * | 1955-08-16 | 1957-03-19 | Ruby Lawrence | Source unit for producing ionized gas |
US3020408A (en) * | 1955-11-14 | 1962-02-06 | Philip W Martin | Nuclear analytical apparatus |
US2964665A (en) * | 1955-12-01 | 1960-12-13 | Tracerlab Inc | Pressure control system |
US3047720A (en) * | 1956-12-07 | 1962-07-31 | Jersey Prod Res Co | Helium 3 scintillation neutron detector |
US3112401A (en) * | 1957-09-27 | 1963-11-26 | Philips Corp | Shielding to confine magnetic field to ion source area of a neutron generator |
US3104322A (en) * | 1958-02-10 | 1963-09-17 | High Voltage Engineering Corp | Compact neutron source |
US2988671A (en) * | 1958-06-30 | 1961-06-13 | Schlumberger Well Surv Corp | Particle accelerating system |
US3014132A (en) * | 1959-01-02 | 1961-12-19 | High Voltage Engineering Corp | Loss current diminisher for compact neutron source |
US3283193A (en) * | 1962-05-14 | 1966-11-01 | Ellison Company | Ion source having electrodes of catalytic material |
US4996017A (en) * | 1982-03-01 | 1991-02-26 | Halliburton Logging Services Inc. | Neutron generator tube |
US4529571A (en) * | 1982-10-27 | 1985-07-16 | The United States Of America As Represented By The United States Department Of Energy | Single-ring magnetic cusp low gas pressure ion source |
US5215703A (en) * | 1990-08-31 | 1993-06-01 | U.S. Philips Corporation | High-flux neutron generator tube |
US20080232532A1 (en) * | 2005-04-29 | 2008-09-25 | Larsen Lewis G | Apparatus and Method for Generation of Ultra Low Momentum Neutrons |
US20070237281A1 (en) * | 2005-08-30 | 2007-10-11 | Scientific Drilling International | Neutron generator tube having reduced internal voltage gradients and longer lifetime |
US20120063558A1 (en) * | 2009-11-16 | 2012-03-15 | Jani Reijonen | Floating Intermediate Electrode Configuration for Downhole Nuclear Radiation Generator |
US9793084B2 (en) * | 2009-11-16 | 2017-10-17 | Schlumberger Technology Corporation | Floating intermediate electrode configuration for downhole nuclear radiation generator |
US9756714B2 (en) | 2013-12-31 | 2017-09-05 | Halliburton Energy Services, Inc. | Nano-emitter ion source neutron generator |
US9835760B2 (en) | 2013-12-31 | 2017-12-05 | Halliburton Energy Services, Inc. | Tritium-tritium neutron generator and logging method |
US10408968B2 (en) | 2013-12-31 | 2019-09-10 | Halliburton Energy Services, Inc. | Field emission ion source neutron generator |
WO2018195436A1 (en) | 2017-04-20 | 2018-10-25 | Philip Teague | Near-field sensitivity of formation and cement porosity measurements with radial resolution in a borehole |
US11558037B2 (en) | 2020-12-10 | 2023-01-17 | Gary Hanington | High efficiency high voltage pulse generator |
Also Published As
Publication number | Publication date |
---|---|
FR832356A (en) | 1938-09-26 |
NL50089C (en) | |
GB491766A (en) | 1938-09-08 |
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