US3435211A - Gaseous glow discharge tube with cathode means surrounding anode means - Google Patents

Gaseous glow discharge tube with cathode means surrounding anode means Download PDF

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US3435211A
US3435211A US518595A US3435211DA US3435211A US 3435211 A US3435211 A US 3435211A US 518595 A US518595 A US 518595A US 3435211D A US3435211D A US 3435211DA US 3435211 A US3435211 A US 3435211A
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cathode
glow discharge
anode
sample
discharge tube
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US518595A
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Sheldon D Softky
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SRI International Inc
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Stanford Research Institute
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J35/00X-ray tubes
    • H01J35/02Details
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/22Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material
    • G01N23/223Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material by irradiating the sample with X-rays or gamma-rays and by measuring X-ray fluorescence
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2223/00Investigating materials by wave or particle radiation
    • G01N2223/07Investigating materials by wave or particle radiation secondary emission
    • G01N2223/076X-ray fluorescence

Definitions

  • This invention relates to apparatus used for the analysis of materials wherein X-ray fluorescence is induced by the incidence of an electron beam on the material being analyzed, and more particularly to improvements therein.
  • the presently employed techniques for achieviug X-ray fluorescence of a material which is being studied is to derive the bombarding electron beams from an electron gun in a cathode ray tube, which usually gives up to 50 kev. electrons.
  • a thin exit window is employed at one end of this tube for enabling the beams to exit into the air.
  • the equipment usually requires power supply regulators and other apparatus necessary to operate the electron gun.
  • An object of this invention is to provide a Simpler source for generating electrons for bombarding materials to achieve X-ray fiuorescence of such materials.
  • Another object of this invention is the provision of a novel and useful arrangement for securng bombarding electrons for X-ray fiuorescent analysis.
  • Still another object of the present invention is the provision of a relatively inexpensive system for generating electrons for bombarding a specimen to achieve X-ray fluorescence thereof.
  • the sample to be analyzed on the anode of a cold cathode gaseous glow discharge arrangement.
  • the sample may be coated with a metallic conducting layer (much thinner than the electron energy range) in order to prevent charge accumulation on the sample surface.
  • the bombardment by energetic electrons from the gas discharge will excite X-ray fluorescence of the constituents of the sample, providing that the high Voltage across the discharge is made greater than the binding energies of either K, L, or M electron shells of the sample constituents.
  • the spectrum of fluorescent X-rays thus excited may be examined by allowing a portion of these X-rays to pass a thin window adjacent to the discharge :into an X-ray spectrometer for analyzing the spectrum.
  • walls 10 enclose an evacuated space in which a suitable gas for supporting a glow discharge is employed.
  • the gas may be argon, neon, or xenon,
  • a cathode structure 12 which, by way of illustrat-ion, has the form of a cylinder with an outward flaring end 12A.
  • the cathode 12 is supported on an insulating ring 14.
  • a second shiel-ding cylinder 16 made of insulating materials.
  • a specimen 20 which is to be analyzed is placed on the disc portion of the anode.
  • An X-ray eollimator 24 is placed adjacent the thin window. X-rays from the specimen can pass through the thin window and the -collimator to strike the analyzing crystal of the X-ray spectrometer, which is placed at the Bragg angle to reflect these X-rays into the detector 28.
  • the cathode 12 is connected to ground and to a source of exciting potential 30, and the anode is also connected to this source of potential. Connections are made through insulated openings in the walls 10. While a cold cathode discharge may be established in the gas within the envelope 10 by connecting the anode and cathode to a source of high current, high Voltage DC, it is preferred to use a source of radio frequency energy to induce the glow discharge. With DC glow discharge excitation, it is necessary to coat the surface of a sample which is an insulator with a thin couductve film to eliminate any ⁇ charge collection. The thickness of this film should be insufficient to prevent electron penetration. This is not necessary with RF excitation.
  • the electrons liberated by the glow discharge established between the anode and the cathode bombard the sample 20 ⁇ where'by X-ray iluorescence of the constituents of the sample are excited, providing that the high voltage existing across the discharge is somewhat greater than the binding energies of either K, L, or M electron shells in the sample constituents.
  • a spectrum of fluorescent X-rays thus excited is examined when the X-rays pass through the thin window which is positioned adjacent to the discharge into the X-ray spectrometer comprising the collimator, crystal, and detector.
  • the size of the electron current attainable to bombard a sample can easily be several thousand times as large as the bombarding current which is easily obtained from an electron gun. Such an increase in the intensity of X-rays thus excite-d can provide a higher resolution of the spectrum and greater sensitivity to measuring small amounts of contamination in samples.
  • an insulator may be analyzed without the need for a charge draining metallic coating.
  • the X-rays are observed which are produced 'during the half cycle when the sample is bombarded by the electrons.
  • the sample will be ion bombarded and thus its surface layer may be sputtered away allowing a fresh layer, previously deep in the sample, to be analyzed, and ultimatel'y yielding an analysis-versus-depth for the sample.
  • Apparatus for causing X-ray fiuorescence of the surface of a sample comprising walls defining an enclosed chamber, an inert gas within said cham ber, means for supporting said sample within said chamber, electrode means for establishing a gaseous glow discharge within said chamber adjacent said sample for bombardng said sample With electrons produced by said gaseous glow discharge, and thin window means in the wall of said chamber for passing X-rays produced by said electron bombardment of said sample out from said chamber.
  • said means for establishing a gaseous glow discharge comprises an anode, a cathode spaced from said anode, said specimen being placed upon said anode, and means for applying a potential to said anode and cathode for establishing said glow discharge.
  • Apparatus for bombarding the surface of a specimer with electrons to produce X-ray fluorescence comprising an evacuated envelope filled With an inert gas, an anode, a cathode spaced from and surrounding said anode, said anode having a surface adapted for supporting said specimen, means for applying a potential between said anode and cathode for establishing a glow discharge therebetween and for bombardng said specirnen with electrons, a thin film window in the walls of said chamber adjacent said anode for passing therethrough X-rays emitted by said specnen in response to said bombardment, and X-ray reflection means positioned adjacent said thin film window for measuring the X-rays passing therethrough.
  • Apparatus as recited in claim 5 wherein said means for establishing a potential across said anode and cathode comprises a source of radio frequency potential.
  • said cathode has the shape of a hollow cylinder having an outward fiare at one end
  • said anode has the shape of a rod terminating in a disc positioned at right angles to said rod, said rod being concentric with said hollow cylinder and said disc being adjacent the outward fiare of sad cathode.

Description

March 25, 1969 s. D. SOFTKY GASEOUS GLOW DISCHARGE TUBE WITH CATHODE MEANS SURROUNDING ANODE MEANS Filed Jan. 4, 1966 OURCE OF Excm N e POTENTIAL A /AA/ W//////////////////// M w 8 WIHHF A NALYZER I INVENT OR. SHELDON D. Sol-'my BY Z z a e A TTO ?NEY United States Patert O GASEOUS GLOW DISCHARGE TUBE WITH CATHODE MEANS SURROUNDING ANODE NIEANS Sheidou D. Softky, Menlo Park, Calif., assignor to Stanford Research Institute, Menlo Park, Calif., a corporation of California Filed Jan. 4, 1966, Ser. No. 518,595 Int. CI. Gflln 23/20 US. Cl. 250-515 7 Claims ABSTRACT OF THE DISCLOSURE A sample to be analyzed is placed on the anode of a cold cathode gaseous glow discharge tube. The cathode effectively surrounds the anode and bombards the sample with electrons whereby X-ray fluorescence is excited, which is then used for analysis.
This invention relates to apparatus used for the analysis of materials wherein X-ray fluorescence is induced by the incidence of an electron beam on the material being analyzed, and more particularly to improvements therein.
The presently employed techniques for achieviug X-ray fluorescence of a material which is being studied, is to derive the bombarding electron beams from an electron gun in a cathode ray tube, which usually gives up to 50 kev. electrons. A thin exit window is employed at one end of this tube for enabling the beams to exit into the air. The equipment usually requires power supply regulators and other apparatus necessary to operate the electron gun.
An object of this invention is to provide a Simpler source for generating electrons for bombarding materials to achieve X-ray fiuorescence of such materials.
Another object of this invention is the provision of a novel and useful arrangement for securng bombarding electrons for X-ray fiuorescent analysis.
Still another object of the present invention is the provision of a relatively inexpensive system for generating electrons for bombarding a specimen to achieve X-ray fluorescence thereof.
These and other objects of the present invention are achieved by placing the sample to be analyzed on the anode of a cold cathode gaseous glow discharge arrangement. If the sample is an insulator, it may be coated with a metallic conducting layer (much thinner than the electron energy range) in order to prevent charge accumulation on the sample surface. The bombardment by energetic electrons from the gas discharge will excite X-ray fluorescence of the constituents of the sample, providing that the high Voltage across the discharge is made greater than the binding energies of either K, L, or M electron shells of the sample constituents. The spectrum of fluorescent X-rays thus excited may be examined by allowing a portion of these X-rays to pass a thin window adjacent to the discharge :into an X-ray spectrometer for analyzing the spectrum.
The novel features that are considered characteristic of this invention are set forth with particularity in the appended clairns. The invention itself both as to its organization and method of operation, as well as additional objects and advantages thereof, will best be understood from the following description when read in connection with the accompanying drawing, which is a schematic diagram of an embodiment of the invention.
Referring now to the drawing, which is a schematic illustration of the invention, walls 10 enclose an evacuated space in which a suitable gas for supporting a glow discharge is employed. The gas may be argon, neon, or xenon,
or other such inert gases. Within the space enclosed by the walls 10 there is placed a cathode structure 12 which, by way of illustrat-ion, has the form of a cylinder with an outward flaring end 12A. The cathode 12 is supported on an insulating ring 14. Within the cylinder 12, there is placed a second shiel-ding cylinder 16 made of insulating materials. An anode 18, comprising a long narrow rod which extends along the axis of the cylinder 12, has a disc 18D supported at right angles to the rod and attached to the end thereof which extends adjacent to the outward flanged end 12A of the cathode 12. A specimen 20 which is to be analyzed is placed on the disc portion of the anode.
A thin window 22, which can be penetrated by X-rays emitted from the material 20, is placed in the walls 10 adjacent the specimen 20. An X-ray eollimator 24 is placed adjacent the thin window. X-rays from the specimen can pass through the thin window and the -collimator to strike the analyzing crystal of the X-ray spectrometer, which is placed at the Bragg angle to reflect these X-rays into the detector 28.
The cathode 12 is connected to ground and to a source of exciting potential 30, and the anode is also connected to this source of potential. Connections are made through insulated openings in the walls 10. While a cold cathode discharge may be established in the gas within the envelope 10 by connecting the anode and cathode to a source of high current, high Voltage DC, it is preferred to use a source of radio frequency energy to induce the glow discharge. With DC glow discharge excitation, it is necessary to coat the surface of a sample which is an insulator with a thin couductve film to eliminate any `charge collection. The thickness of this film should be insufficient to prevent electron penetration. This is not necessary with RF excitation.
The electrons liberated by the glow discharge established between the anode and the cathode bombard the sample 20` where'by X-ray iluorescence of the constituents of the sample are excited, providing that the high voltage existing across the discharge is somewhat greater than the binding energies of either K, L, or M electron shells in the sample constituents. A spectrum of fluorescent X-rays thus excited is examined when the X-rays pass through the thin window which is positioned adjacent to the discharge into the X-ray spectrometer comprising the collimator, crystal, and detector.
The size of the electron current attainable to bombard a sample can easily be several thousand times as large as the bombarding current which is easily obtained from an electron gun. Such an increase in the intensity of X-rays thus excite-d can provide a higher resolution of the spectrum and greater sensitivity to measuring small amounts of contamination in samples.
Because no difiiculties are present of the type due to low electron energy in an electron gun, lower energy electrons can be used to bombard the sample than would be practical from an electron gun. As a consequence of this, shallower layers in a sample may be studied whereby the depth resolution of analysis may be improved.
By using the radio frequency source of exciting potential, instead o-f a direct current source of exciting potential, it has 'been indicated that an insulator may be analyzed without the need for a charge draining metallic coating. In this instance, the X-rays are observed which are produced 'during the half cycle when the sample is bombarded by the electrons. During the other or negative half cycle of voltage, the sample will be ion bombarded and thus its surface layer may be sputtered away allowing a fresh layer, previously deep in the sample, to be analyzed, and ultimatel'y yielding an analysis-versus-depth for the sample.
There has accordingly been described herei-n a novel,
useful and unique arrangement for bombarding a sample with electrons having an energy sufiicient to cause X-ray fiuorescerce of samples. While a specific embodiment of the electron producing structure has been described and claimed, it will be appreciated that those skilled in the art may depart from the structure shown without departing from the spirit of this invention nor the intended scope of the claims.
What is claimed is:
1. Apparatus for causing X-ray fiuorescence of the surface of a sample comprising walls defining an enclosed chamber, an inert gas within said cham ber, means for supporting said sample within said chamber, electrode means for establishing a gaseous glow discharge within said chamber adjacent said sample for bombardng said sample With electrons produced by said gaseous glow discharge, and thin window means in the wall of said chamber for passing X-rays produced by said electron bombardment of said sample out from said chamber.
2. Apparatus as recited in claim 1 wherein said means for establishing a gaseous glow discharge comprises an anode, a cathode spaced from said anode, said specimen being placed upon said anode, and means for applying a potential to said anode and cathode for establishing said glow discharge.
3. Apparatus as recited in claim 2 wherein said cathode has the shape of a hollow cylinder having an outward fiare at one end, and said anode has the shape of a rod terminating in a disc positioned at right angles to said rod, said rod being concentric With said hollow cylinder and said disc being adjacent the outward fiare of said cathode.
4. Apparatus as recited in claim 2 wherein said means for applying a potential to said anode and cathode applies said potential at a radio frequency.
5. Apparatus for bombarding the surface of a specimer with electrons to produce X-ray fluorescence comprising an evacuated envelope filled With an inert gas, an anode, a cathode spaced from and surrounding said anode, said anode having a surface adapted for supporting said specimen, means for applying a potential between said anode and cathode for establishing a glow discharge therebetween and for bombardng said specirnen with electrons, a thin film window in the walls of said chamber adjacent said anode for passing therethrough X-rays emitted by said specnen in response to said bombardment, and X-ray reflection means positioned adjacent said thin film window for measuring the X-rays passing therethrough.
6. Apparatus as recited in claim 5 wherein said means for establishing a potential across said anode and cathode comprises a source of radio frequency potential.
7. Apparatus as recited in claim 5 wherein said cathode has the shape of a hollow cylinder having an outward fiare at one end, and said anode has the shape of a rod terminating in a disc positioned at right angles to said rod, said rod being concentric with said hollow cylinder and said disc being adjacent the outward fiare of sad cathode.
References Cited UNITED STATES PATENTS 3,235,727 2/1966 Shapiro.
RALPH G. NILSON, Pr'mary Exam'ner.
S. C. SHEAR, Assistant Exam'ner.
U.S. Cl. X.R. 313-55, 59
US518595A 1966-01-04 1966-01-04 Gaseous glow discharge tube with cathode means surrounding anode means Expired - Lifetime US3435211A (en)

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3852596A (en) * 1970-03-20 1974-12-03 Philips Corp Cold cathode gaseous discharge device for producing electrons in an x-ray fluorescence analysis apparatus
US3919549A (en) * 1972-03-17 1975-11-11 Aquitaine Petrole Portable X-ray spectrometer
US3974381A (en) * 1973-10-31 1976-08-10 Mahle Gmbh Method of electron beam welding with X-ray detection
US4217517A (en) * 1978-01-24 1980-08-12 Compagnie Generale De Radiologie Small divergence x-ray tube

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3235727A (en) * 1961-03-02 1966-02-15 First Pennsylvania Banking And Electron probe system

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3235727A (en) * 1961-03-02 1966-02-15 First Pennsylvania Banking And Electron probe system

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3852596A (en) * 1970-03-20 1974-12-03 Philips Corp Cold cathode gaseous discharge device for producing electrons in an x-ray fluorescence analysis apparatus
US3919549A (en) * 1972-03-17 1975-11-11 Aquitaine Petrole Portable X-ray spectrometer
US3974381A (en) * 1973-10-31 1976-08-10 Mahle Gmbh Method of electron beam welding with X-ray detection
US4217517A (en) * 1978-01-24 1980-08-12 Compagnie Generale De Radiologie Small divergence x-ray tube

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