EP0567183A1 - Tube à rayons X utilisamt la raie-M du spectre de rayonnement - Google Patents
Tube à rayons X utilisamt la raie-M du spectre de rayonnement Download PDFInfo
- Publication number
- EP0567183A1 EP0567183A1 EP93201081A EP93201081A EP0567183A1 EP 0567183 A1 EP0567183 A1 EP 0567183A1 EP 93201081 A EP93201081 A EP 93201081A EP 93201081 A EP93201081 A EP 93201081A EP 0567183 A1 EP0567183 A1 EP 0567183A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- ray tube
- anode
- radiation
- ray
- anode material
- 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.)
- Withdrawn
Links
- 230000005855 radiation Effects 0.000 title claims abstract description 12
- 238000001228 spectrum Methods 0.000 title abstract description 14
- 239000010405 anode material Substances 0.000 claims abstract description 16
- 229910052776 Thorium Inorganic materials 0.000 claims abstract description 3
- 238000002441 X-ray diffraction Methods 0.000 claims description 6
- 229910052770 Uranium Inorganic materials 0.000 claims description 4
- 230000005540 biological transmission Effects 0.000 claims description 4
- ZSLUVFAKFWKJRC-IGMARMGPSA-N 232Th Chemical compound [232Th] ZSLUVFAKFWKJRC-IGMARMGPSA-N 0.000 claims description 2
- 238000002083 X-ray spectrum Methods 0.000 claims description 2
- 238000000151 deposition Methods 0.000 claims description 2
- 239000000463 material Substances 0.000 claims description 2
- 238000000034 method Methods 0.000 claims description 2
- 238000004544 sputter deposition Methods 0.000 claims description 2
- VBWSWBQVYDBVGA-UHFFFAOYSA-N uranium Chemical compound [U].[U].[U] VBWSWBQVYDBVGA-UHFFFAOYSA-N 0.000 claims 1
- 238000004458 analytical method Methods 0.000 abstract description 12
- 239000013077 target material Substances 0.000 abstract 1
- JFALSRSLKYAFGM-UHFFFAOYSA-N uranium(0) Chemical compound [U] JFALSRSLKYAFGM-UHFFFAOYSA-N 0.000 description 6
- 229910052790 beryllium Inorganic materials 0.000 description 4
- ATBAMAFKBVZNFJ-UHFFFAOYSA-N beryllium atom Chemical compound [Be] ATBAMAFKBVZNFJ-UHFFFAOYSA-N 0.000 description 4
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- 238000010521 absorption reaction Methods 0.000 description 3
- 229910052802 copper Inorganic materials 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 229910052706 scandium Inorganic materials 0.000 description 3
- SIXSYDAISGFNSX-UHFFFAOYSA-N scandium atom Chemical compound [Sc] SIXSYDAISGFNSX-UHFFFAOYSA-N 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- 230000003595 spectral effect Effects 0.000 description 2
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 239000011888 foil Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
- 238000004846 x-ray emission Methods 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J35/00—X-ray tubes
- H01J35/02—Details
- H01J35/04—Electrodes ; Mutual position thereof; Constructional adaptations therefor
- H01J35/08—Anodes; Anti cathodes
- H01J35/112—Non-rotating anodes
Definitions
- the invention relates to an X-ray tube, comprising a cathode and an anode for generating X-rays.
- the invention also relates to an X-ray analysis apparatus comprising an X-ray tube in accordance with the invention.
- An X-ray tube of this kind is known from US 4,205,251.
- An X-ray tube described therein aims to generate X-rays in an effective spectral range for X-ray analysis of elements.
- a tube described therein is particularly suitable for generating copper K- ⁇ radiation having a characteristic wavelength of approximately 0.15 nm.
- the copper K- ⁇ wavelength is not very effective.
- solutions have been proposed such as, for example the use of scandium as the anode material as described in US 4,583,243 for analysis of notably light elements, or a double-layer anode as described in US 4,622,688 for generating a radiation spectrum which can be controlled by the anode voltage and which can be used for analysis of light as well as heavier elements.
- the anode thereof comprises a layer of scandium and, underneath the comparatively thin scandium layer, it comprises a layer of tungsten or molybdenum for analysis of heavier elements by means of an increased anode voltage.
- an X-ray tube of the kind set forth in accordance with the invention is characterized in that in order to generate an X-ray spectrum with an effective wavelength range for X-ray analysis, the anode contains a material in which effectively usable M-radiation can also be generated.
- the tube is suitable for analysis of light elements, to be excited notably by the M-radiation, as well as heavier elements, to be excited notably by means of, for example L-radiation and effective radiation from the continuous spectrum.
- the X-ray tube very effectively utilizes the M-radiation, experienced as a nuissance thus far and situated in an attractive wavelength range for the analysis of light elements if the anode material is suitably chosen.
- the anode contains an element from the group of heavy elements thorium (90), protactinium (91) and uranium (92) or mixtures thereof.
- M-radiation of these elements has a wavelength of approximately 0.4 nm and is sufficiently energetic for fast analysis of elements having an atomic number of between, for example 4 (beryllium) and 18 (argon).
- the continuous spectrum to be generated in such anode materials with the L-radiation of approximately 0.1 nm is sufficiently energetic for analysis of heavy elements as high as the anode material.
- An additional advantage consists in that an exit window of beryllium with a customary thickness of, for example 150 ⁇ m exhibits a comparatively high transmission for the M-radiation to be generated in these tubes.
- the anode material is notably low-radioactive U-238.
- the anode material is deposited on a support, for example in the form of an anode body in a side-window tube or an end-window tube, as a comparatively thin layer of, for example from 0.2 to 2.0 ⁇ m thickness.
- a thin layer of anode material is deposited on an exit window, preferably by sputtering or a CVD technique. Because of the necessary transmission for the X-rays to be generated therein, the layer then has a thickness of at the most, for example approximately 0.1 ⁇ m.
- the layer of anode material can alternatively be provided on an anode body as a foil. The thickness of the layer is then again determined by the deposition technique and the temperature conditions and may also be substantially greater than approximately 0.1 ⁇ m.
- An X-ray tube in accordance with the invention is particularly suitable for use in, for example an X-ray spectrometer because therein a wavelength range generated by a single, customary high voltage can be used for excitation of a wide range of elements.
- An X-ray tube 1 as shown in Fig. 1 comprises, accommodated in an envelope 2 with a connector 4 and an exit window 6, an electron emitter 10, for example in the form of a filament which is accommodated in a cathode sleeve 8. Electrons emitted by the emitter 10 are directed towards an anode 14 along paths 12. The electron paths are determined by the geometry of the cathode sleeve, of the cathode itself, and of the anode and by the shape of a conical portion 16 of the tube envelope. On an anode body 18 of the anode, being made of, for example copper, there is provided an anode target plate 19 of, for example uranium 238.
- an X-ray beam 20 is generated in a customary manner by the electrons incident along the paths 12, which beam emanates from the tube via the exit window 6 which consists of, for example a plate of beryllium having a thickness of 150 ⁇ m.
- Fig. 2 shows an X-ray tube 1 mounted in an X-ray analysis apparatus 20, which is in this case formed as a simultaneous spectrometer comprising a specimen table 30, a mounting plate 32, and a housing 36 for a number of measuring channels.
- the Figure shows two measuring channels 42 and 44 which are symmetrically arranged relative to an object or specimen 40 to be examined.
- Each measuring channel comprises an entrance slit 46, an analysis crystal 48, and a detector 50.
- Each of the measuring channels is oriented relative to the specimen in conformity with a respective element assigned thereto.
- the specimen is irradiated by an X-ray beam 52 which, as a result of the use of an anode material in accordance with the invention, covers a wide effective wavelength range and is hence suitable for simultaneous excitation of a wide range of elements.
- a first favourable effect consists in that this maximum, and hence the entire continuous spectrum, reaches a level which increases in proportion to the atomic number of the anode material.
- Single lines in the continuous spectrum denote the line spectrum with N-lines at approximately 0.88 nm, M-lines at approximately 0.39 nm and L-lines at approximately 0.09 nm. In the case of 60 kV, K-lines in uranium of approximately 0.01 nm are not excited.
Landscapes
- X-Ray Techniques (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| EP93201081A EP0567183A1 (fr) | 1992-04-21 | 1993-04-14 | Tube à rayons X utilisamt la raie-M du spectre de rayonnement |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| EP92201104 | 1992-04-21 | ||
| EP92201104 | 1992-04-21 | ||
| EP93201081A EP0567183A1 (fr) | 1992-04-21 | 1993-04-14 | Tube à rayons X utilisamt la raie-M du spectre de rayonnement |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| EP0567183A1 true EP0567183A1 (fr) | 1993-10-27 |
Family
ID=26131341
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP93201081A Withdrawn EP0567183A1 (fr) | 1992-04-21 | 1993-04-14 | Tube à rayons X utilisamt la raie-M du spectre de rayonnement |
Country Status (1)
| Country | Link |
|---|---|
| EP (1) | EP0567183A1 (fr) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2003065772A3 (fr) * | 2002-01-31 | 2004-02-26 | Univ Johns Hopkins | Source de rayons x et procede pour la production plus efficace de frequences de rayons x au choix |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR690718A (fr) * | 1929-03-30 | 1930-09-25 | Philips Nv | Tube à rayons chi |
| GB1184947A (en) * | 1966-06-28 | 1970-03-18 | Radiologie Cie Gle | Improvements in or relating to a Method of Producing an X-Ray Picture of an Object |
| US3835341A (en) * | 1973-06-25 | 1974-09-10 | W Zingaro | Selectable multi-window x-ray tube |
| US4477921A (en) * | 1981-11-27 | 1984-10-16 | Spire Corporation | X-Ray lithography source tube |
| EP0127230A1 (fr) * | 1983-05-25 | 1984-12-05 | Koninklijke Philips Electronics N.V. | Tube à rayons X comprenant deux couches successives de matériau anodique |
-
1993
- 1993-04-14 EP EP93201081A patent/EP0567183A1/fr not_active Withdrawn
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR690718A (fr) * | 1929-03-30 | 1930-09-25 | Philips Nv | Tube à rayons chi |
| GB1184947A (en) * | 1966-06-28 | 1970-03-18 | Radiologie Cie Gle | Improvements in or relating to a Method of Producing an X-Ray Picture of an Object |
| US3835341A (en) * | 1973-06-25 | 1974-09-10 | W Zingaro | Selectable multi-window x-ray tube |
| US4477921A (en) * | 1981-11-27 | 1984-10-16 | Spire Corporation | X-Ray lithography source tube |
| EP0127230A1 (fr) * | 1983-05-25 | 1984-12-05 | Koninklijke Philips Electronics N.V. | Tube à rayons X comprenant deux couches successives de matériau anodique |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2003065772A3 (fr) * | 2002-01-31 | 2004-02-26 | Univ Johns Hopkins | Source de rayons x et procede pour la production plus efficace de frequences de rayons x au choix |
| US7186022B2 (en) | 2002-01-31 | 2007-03-06 | The Johns Hopkins University | X-ray source and method for more efficiently producing selectable x-ray frequencies |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
| AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): DE FR GB NL |
|
| RAP1 | Party data changed (applicant data changed or rights of an application transferred) |
Owner name: N.V. PHILIPS' GLOEILAMPENFABRIEKEN |
|
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
| 18D | Application deemed to be withdrawn |
Effective date: 19940428 |