EP0459567A2 - Source quasi-monochromatique de rayons X - Google Patents
Source quasi-monochromatique de rayons X Download PDFInfo
- Publication number
- EP0459567A2 EP0459567A2 EP91201225A EP91201225A EP0459567A2 EP 0459567 A2 EP0459567 A2 EP 0459567A2 EP 91201225 A EP91201225 A EP 91201225A EP 91201225 A EP91201225 A EP 91201225A EP 0459567 A2 EP0459567 A2 EP 0459567A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- target
- screen
- radiation
- anode
- radiation source
- 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.)
- Granted
Links
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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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J35/00—X-ray tubes
- H01J35/02—Details
Definitions
- the invention relates to a radiation source for generating essentially monochromatic X-rays, with an anode for generating X-rays, a target enclosed by the anode for converting X-rays into fluorescent radiation, and with a screen located between the target and the anode for shielding the target against electrons .
- Such a radiation source is known from DE-OS 37 16 618.
- the metal screen has the task of keeping (scattering) electrons away from the target, which would lead to the fact that polychromatic brake radiation is generated in the target in addition to the practically monochromatic fluorescent radiation.
- This screen is penetrated by the X-ray radiation emitted from the anode, which is converted into fluorescence radiation in the target.
- the screen is as thin-walled as possible and consists of a low-atom material (e.g. titanium (for a target made of tantalum)).
- the object of the invention is to design a radiation source of the type mentioned at the outset in such a way that even more fluorescent radiation or monochromatic X-radiation can be generated.
- This object is achieved in that the screen contains an element with a high atomic number.
- the invention is based on the knowledge that a screen that has an element with a high atomic number ("high” in the sense of the invention is an atomic number whose deviation from the atomic number of the target material is small compared to the atomic number in question) in the periodic table of the elements contains more X-ray radiation from the anode than an equally strong screen made of a low-atom element, but that the radiation comprising an element with a high atomic number generates braking radiation which is converted in the target mainly into fluorescent radiation. In this way, the overall yield of fluorescent radiation can be increased.
- a preferred development of the invention provides that the screen and the target each contain the same element with a high atomic number. It is provided in a still further embodiment of the invention that the screen and the target consist of tantalum.
- the advantage of the further development is, on the one hand, that the thermal expansion of the target and screen is the same in both cases, so that mechanical stresses cannot occur when heated, and, on the other hand, that the spectral purity of the spectrum generated is deteriorated as little as possible, because the characteristic radiation generated in the screen has the same wavelength as the fluorescence radiation generated in the target.
- tantalum as the material for the target and the screen, the high melting point of this material is added, so that the radiation source can be subjected to a much greater electrical power than is possible with the known radiation source with a titanium screen.
- the radiation source comprises a piston which encloses an evacuated room in which the anode, the screen and the target are located. While in the known radiation source the screen hermetically seals the radiation source from the outside, so that the target and the surface facing it come into contact with the atmospheric oxygen, the target or this screen surface is in this development within the vacuum space of the radiation source. The screen and the target can therefore withstand high temperatures better.
- a collimator arrangement is provided which is designed such that only the radiation emanating from the target can pass through the collimator arrangement. As a result, the braking radiation generated in the screen is largely suppressed.
- the radiation source which is designed to be rotationally symmetrical with respect to an axis 1, comprises a cathode part 2 and an anode part 3, which are connected to one another in a vacuum-tight manner via a piston 4.
- the cathode part 2 is connected to the piston 4, which is made of metal, via an insulator, not shown, and carries a voltage of, for example, 160 kV or more. It comprises a filament 21 which surrounds the axis of symmetry 1 in a ring and a cathode die 22 which forms the paths of the electrons emitted from the filament 21 in the desired manner.
- the anode part 3 comprises a hollow body consisting of two parts 32 and 33, the cavity of which is flowed through in the operating state by a liquid coolant supplied from the outside in a manner not shown in detail.
- a partition 34 prevents the coolant in the shortest possible way from the coolant inlet to the coolant outlet (neither shown) flows.
- the parts 32 and 33 of the anode body can for example consist of copper.
- the part 32 of the anode body 32, 33 has an inner surface open towards the cathode part 2 in the form of a truncated cone surface 31.
- This lateral surface 31 is coated with a material that has a high atomic number, preferably with gold. The electrons emitted from the filament in the operating state hit this inner surface.
- the electrons impinging on the anode 31 generate X-rays with a spectrum which is continuous up to a quantum energy determined by the voltage between the anode part and the cathode part and on which the line spectrum of gold is superimposed with a K line at approximately 68.8 keV.
- the X-ray radiation strikes a target 36 made of tantalum through a thin cylindrical screen 35, which has the shape of a cone, the tip of which points away from the cathode part 2.
- the target essentially converts X-ray quanta with an energy above the K absorption edge of the target (for tantalum approx. 67.4 keV) into monochromatic fluorescence radiation, the quantum energy of which is the characteristic energy of the target material (for tantalum: 57.5 keV) corresponds.
- the screen 35 which carries the target 36, is fastened in a central bore in the disk-shaped part 33 of the anode body 32, 33, which is closed in a vacuum-tight manner by a window 37.
- the invention uses the impact of the electrons on the screen 35 to generate additional X-rays.
- the screen must consist of an element with a high atomic number or contain such an element to a sufficient extent.
- the atomic number of this element should at most be slightly lower than that of the target, but if possible greater than 50.
- the electron bombardment of the screen generates not only characteristic radiation but also polychromatic (braking) radiation. A much larger portion of this hits the target than of the radiation from the anode because the screen closely surrounds the target.
- a suitable element - because of its high atomic number (74) and its high thermal resilience - would be tungsten, for example.
- a screen made of tantalum is even cheaper than a screen made of tungsten.
- the quantum energy of the characteristic radiation from tungsten is about 2 keV higher than that from tantalum. Even if the X-rays emitted by the screen were prevented from directly reaching the outside, this radiation could not be prevented from causing elastic or Compton scattering processes at the target, and in this way reaching the outside and impairing the spectral purity of the radiation.
- the screen must be thick enough to keep the scattering electrons away from the target 36, but on the other hand it must be sufficiently thin so that the radiation emitted by the anode 31 is not weakened too much.
- a suitable value for the wall thickness of the screen is 0.1 mm. Although this screen absorbs more X-rays than a titanium screen of the same strength, because of the additionally generated X-rays there is a higher emission of quasi-monochromatic radiation from the target 36 than with a titanium screen with the same wall thickness.
- the screen becomes in operation due to its smaller area and wall thickness, and because of the lack of cooling, much hotter than the anode body.
- the electrical power that can be supplied to the radiation source is therefore limited by the temperature resistance of the screen 35.
- a tantalum umbrella is also superior to a titanium umbrella because of its much higher melting point. In connection with the significantly improved conversion of the electrical power into fluorescence radiation, this means that the intensity of the quasi-monochromatic radiation can be several times greater than in the case of a radiation source with a titanium screen.
- the screen In order to take advantage of the high thermal load capacity of the tantalum components, it must be avoided that the tantalum parts come into contact with atmospheric oxygen. Therefore, the screen must not hermetically seal the radiation source from the outside - as in DE-OS 37 16 618, but must be provided with one or more small openings, not shown, so that the vacuum inside the bulb also the interior of the screen Fulfills.
- the central hole in which the screen 35 is inserted is closed to the outside by the radiation exit window 37.
- the radiation exit window is formed by a plate, which can also consist of tantalum. Because of the material used between the target and the radiation exit window, the absorption coefficient of the radiation exit window for the fluorescence radiation generated in the target is relatively low.
- diaphragm arrangement In front of the radiation exit window there is e.g. from two perforated diaphragms 5, 6 provided diaphragm arrangement which is connected to the radiation source in a manner not shown.
- the openings in this diaphragm arrangement are dimensioned such that the directly emerging X-ray radiation generated in the screen is largely suppressed by the diaphragm arrangement. This prevents the continuous spectrum of the radiation generated in the screen from affecting the spectral purity of the fluorescent radiation which passes through the diaphragm arrangement.
- This diaphragm arrangement preferably consists of the same material as the target 36 and the window 37 — in the example, therefore, of tantalum.
Landscapes
- X-Ray Techniques (AREA)
- Cathode-Ray Tubes And Fluorescent Screens For Display (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE4017002A DE4017002A1 (de) | 1990-05-26 | 1990-05-26 | Strahlenquelle fuer quasimonochromatische roentgenstrahlung |
DE4017002 | 1990-05-26 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0459567A2 true EP0459567A2 (fr) | 1991-12-04 |
EP0459567A3 EP0459567A3 (en) | 1992-01-02 |
EP0459567B1 EP0459567B1 (fr) | 1996-01-31 |
Family
ID=6407256
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP91201225A Expired - Lifetime EP0459567B1 (fr) | 1990-05-26 | 1991-05-22 | Source quasi-monochromatique de rayons X |
Country Status (4)
Country | Link |
---|---|
US (1) | US5157704A (fr) |
EP (1) | EP0459567B1 (fr) |
JP (1) | JP3105292B2 (fr) |
DE (2) | DE4017002A1 (fr) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6141400A (en) * | 1998-02-10 | 2000-10-31 | Siemens Aktiengesellschaft | X-ray source which emits fluorescent X-rays |
Families Citing this family (19)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19639241C2 (de) * | 1996-09-24 | 1998-07-23 | Siemens Ag | Monochromatische Röntgenstrahlenquelle |
DE19805290C2 (de) * | 1998-02-10 | 1999-12-09 | Siemens Ag | Monochromatische Röntgenstrahlenquelle |
DE19905802A1 (de) * | 1999-02-12 | 2000-08-17 | Philips Corp Intellectual Pty | Röntgenröhre |
US7180981B2 (en) | 2002-04-08 | 2007-02-20 | Nanodynamics-88, Inc. | High quantum energy efficiency X-ray tube and targets |
US7158612B2 (en) * | 2003-02-21 | 2007-01-02 | Xoft, Inc. | Anode assembly for an x-ray tube |
CN1302510C (zh) * | 2003-05-15 | 2007-02-28 | 谭大刚 | 基于透射阳极x线机的可变换准单能或双能荧光x线源 |
EP1627409B1 (fr) * | 2003-05-19 | 2008-09-03 | Koninklijke Philips Electronics N.V. | Source a rayons x fluorescents |
US7200203B2 (en) * | 2004-04-06 | 2007-04-03 | Duke University | Devices and methods for targeting interior cancers with ionizing radiation |
WO2006049051A1 (fr) * | 2004-11-08 | 2006-05-11 | Sii Nanotechnology Inc. | Dispositif d’analyse à rayons x fluorescents |
US20070089227A1 (en) * | 2005-10-26 | 2007-04-26 | Joseph Battiston | Transfer seat with rotatable wing |
WO2007088934A1 (fr) * | 2006-02-01 | 2007-08-09 | Toshiba Electron Tubes & Devices Co., Ltd. | Source de rayons x et dispositif d'analyse de rayons x fluorescents |
JP4738189B2 (ja) * | 2006-02-01 | 2011-08-03 | 東芝電子管デバイス株式会社 | X線源および蛍光x線分析装置 |
US7876883B2 (en) * | 2008-04-10 | 2011-01-25 | O'hara David | Mammography X-ray homogenizing optic |
JP2012524374A (ja) | 2009-04-16 | 2012-10-11 | エリック・エイチ・シルバー | 単色x線の方法および装置 |
WO2014175762A1 (fr) | 2013-04-25 | 2014-10-30 | Siemens Aktiengesellschaft | Dispositif et procédé de génération de rayons x |
EP3641651A4 (fr) * | 2017-05-19 | 2021-04-07 | Imagine Scientific, Inc. | Systèmes et procédés d'imagerie par rayons x monochromatiques |
US10818467B2 (en) * | 2018-02-09 | 2020-10-27 | Imagine Scientific, Inc. | Monochromatic x-ray imaging systems and methods |
JP7299226B2 (ja) | 2018-02-09 | 2023-06-27 | イマジン サイエンティフィック,インコーポレイテッド | 単色x線撮像システム及び方法 |
WO2020056281A1 (fr) | 2018-09-14 | 2020-03-19 | Imagine Scientific, Inc. | Systèmes de composant de rayons x monochromatiques et procédés |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2205297A (en) * | 1938-07-23 | 1940-06-18 | Gen Electric | X-ray tube |
US3567928A (en) * | 1969-06-12 | 1971-03-02 | Du Pont | Fluorescent analytical radiation source for producing soft x-rays and secondary electrons |
US3920999A (en) * | 1972-12-05 | 1975-11-18 | Strahlen Und Umweltforachung M | X-Ray source |
EP0292055A2 (fr) * | 1987-05-18 | 1988-11-23 | Philips Patentverwaltung GmbH | Source de rayonnement pour la génération de rayons X essentiellement monochromatiques |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3963922A (en) * | 1975-06-09 | 1976-06-15 | Nuclear Semiconductor | X-ray fluorescence device |
-
1990
- 1990-05-26 DE DE4017002A patent/DE4017002A1/de not_active Withdrawn
-
1991
- 1991-05-22 DE DE59107329T patent/DE59107329D1/de not_active Expired - Lifetime
- 1991-05-22 US US07/704,241 patent/US5157704A/en not_active Expired - Lifetime
- 1991-05-22 EP EP91201225A patent/EP0459567B1/fr not_active Expired - Lifetime
- 1991-05-23 JP JP03118628A patent/JP3105292B2/ja not_active Expired - Lifetime
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2205297A (en) * | 1938-07-23 | 1940-06-18 | Gen Electric | X-ray tube |
US3567928A (en) * | 1969-06-12 | 1971-03-02 | Du Pont | Fluorescent analytical radiation source for producing soft x-rays and secondary electrons |
US3920999A (en) * | 1972-12-05 | 1975-11-18 | Strahlen Und Umweltforachung M | X-Ray source |
EP0292055A2 (fr) * | 1987-05-18 | 1988-11-23 | Philips Patentverwaltung GmbH | Source de rayonnement pour la génération de rayons X essentiellement monochromatiques |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6141400A (en) * | 1998-02-10 | 2000-10-31 | Siemens Aktiengesellschaft | X-ray source which emits fluorescent X-rays |
Also Published As
Publication number | Publication date |
---|---|
EP0459567A3 (en) | 1992-01-02 |
JP3105292B2 (ja) | 2000-10-30 |
DE4017002A1 (de) | 1991-11-28 |
EP0459567B1 (fr) | 1996-01-31 |
JPH04229539A (ja) | 1992-08-19 |
DE59107329D1 (de) | 1996-03-14 |
US5157704A (en) | 1992-10-20 |
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