EP1670017A1 - Elektronendurchlässiges Fenster, Fenstereinheit und Elektronenstrahlerzeuger - Google Patents
Elektronendurchlässiges Fenster, Fenstereinheit und Elektronenstrahlerzeuger Download PDFInfo
- Publication number
- EP1670017A1 EP1670017A1 EP04257542A EP04257542A EP1670017A1 EP 1670017 A1 EP1670017 A1 EP 1670017A1 EP 04257542 A EP04257542 A EP 04257542A EP 04257542 A EP04257542 A EP 04257542A EP 1670017 A1 EP1670017 A1 EP 1670017A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- electron beam
- window
- electrically conductive
- beam window
- electron
- 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- Withdrawn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
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J5/00—Details relating to vessels or to leading-in conductors common to two or more basic types of discharge tubes or lamps
- H01J5/02—Vessels; Containers; Shields associated therewith; Vacuum locks
- H01J5/18—Windows permeable to X-rays, gamma-rays, or particles
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J33/00—Discharge tubes with provision for emergence of electrons or ions from the vessel; Lenard tubes
- H01J33/02—Details
- H01J33/04—Windows
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J5/00—Details relating to vessels or to leading-in conductors common to two or more basic types of discharge tubes or lamps
- H01J5/20—Seals between parts of vessels
- H01J5/22—Vacuum-tight joints between parts of vessel
Definitions
- This invention relates to an improved electron beam window, an electron beam window assembly, and to an electron gun provided therewith.
- the electron beam window needs to be mechanically robust to withstand the force generated by the pressure difference between the high vacuum chamber and the higher pressure environment, whilst being thin enough to prevent too much attenuation of the electron beam.
- CVD chemical vapour deposition
- the value of the destructive charge is proportional to the square of the beam voltage, and the beam current determines the rate at which this charge increases.
- US 2002/0048344 and US 2002/0048345 recognise that a diamond window, used in an X-ray radiation device, can develop a charge which can deflect, decelerate, or stop the passage of an electron ray, and teach that this problem can be solved by doping the diamond window to make it conductive. This doping is achieved by doping the diamond with boron during the gas phase deposition. Such beam deviation arises because the electric field generated external to the window, by the charging of the window, is large in comparison with the accelerating voltage of the electron beam. These is no recognition of the problem of a diamond window being damaged by an arc discharge.
- an electron beam window is formed from an insulating material to define a first surface for receiving a high energy electron beam and a second surface for transmitting the electron beam, which is protected from perforation by an electrically conductive path that prevents the electron beam from establishing any significant electrical field across the thickness of the window.
- the electrically conductive path may be provided by incorporating an electrically conductive dopant in the insulating material.
- the electron beam window is preferably formed from diamond incorporating a dopant selected from the group comprising phosphorus, sulphur, nitrogen and boron.
- the dopant may be incorporated only in a stratum of the diamond forming at least one of said surfaces.
- the electrically conductive path may be provided by ion implantation in at least one of said surfaces.
- the electrically conductive path may be provided by an electrically conductive layer which is adhered to one of said faces, the layer being sufficiently thin that it will not significantly impede the passage of electrons through the window.
- the electrically conductive layer may be adhered to both of said faces and the combined thickness of the layers is sufficiently thin that they will not significantly impede the passage of electrons through the window.
- the layers are preferably electrically connected.
- the layer thickness may be less than I micron and is preferably between 10 and 100 atoms.
- Each layer may be formed from a material chosen from the group comprising indium tin oxide, magnesium, aluminium, titanium, platinum, gold and silica doped to make it electrically conductive, preferably magnesium, aluminium or titanium, more preferably aluminium.
- the layer may be formed by vacuum deposition.
- an electron beam window assembly is formed by attaching an electron beam window, having any of the features detailed above, over an aperture defined by an electrically conductive mounting plate such that the electron beam window covers the aperture, and an hermetic seal is positioned between the electron beam window and the plate.
- the conductive layer is preferably connected to the electrically conductive mounting plate.
- an electron gun arranged to produce a high energy electron beam within a vacuum chamber and to direct the electron beam through an electron beam window into a region of higher pressure, has an electron beam window which is formed from an insulating material and is protected from perforation by an electrically conductive path that prevents the establishment of any potentially damaging electrical charge across the thickness of the electron beam window by the passage of the electron beam.
- an electron beam window 10 is positioned inside a typical electron gun 11 with its periphery supported by a structure 12 which connects a vacuum chamber 13 to a chamber 14 that is to receive an electron beam 15 from an electron beam generator 16.
- the vacuum chamber 13 is evacuated to generate a vacuum of typically 10 -6 mbar.
- the chamber 14 defines a region of higher pressure, as is well known in the art, the electron beam window 10 serving as a physical barrier to preserve the pressure difference between the chambers 13 and 14. Consequently, the electron beam window 10 must withstand a force equal to its cross sectional area multiplied by the pressure difference between chambers 13 and 14, this force being transmitted to the structure 12.
- FIGs 2 and 3 illustrate the mounting of the electron beam window 10 to the structure 12 in much greater detail.
- the structure 12 is a cast web of stainless steel formed with a cylindrical orifice 17 through which the electron beam will pass towards the electron beam window 10.
- An annular copper sealing gasket 18 is trapped between the electron beam window 10 and an annular edge 19 formed integral of the structure 12.
- a bracket 20 is slidably mounted on an array of stainless steel bolts 21 and is urged against the electron beam window 10 by corresponding lock-nuts 22.
- the arrangement illustrated is diagrammatic and the actual mounting of the window would generally include a compliant member positioned between the bracket 20 and the electron beam window 10.
- the bracket 20 is formed with a central aperture 23 to allow free passage of the electron beam.
- the heads of the bolts 21 are within the vacuum chamber 13, they are provided with respective copper sealing washers as shown.
- the electron beam window 10 is formed from diamond by chemical vapour deposition as this is much less costly than using natural diamond. Various methods are known for the synthetic production and shaping of the diamond.
- US Patents 5,264,071 and 5,349,922 teach the production of monolithic diamond sheet by passing a mixture of hydrogen and a hydrocarbon at a high temperature over a cooled substrate on which diamond is deposited.
- the CVD diamond may be single crystal or polycrystalline, the latter being more available.
- the electron beam window 10 comprises a cylindrical disk of polycrystalline diamond which has been ion beam etched to define a thinner pane, as shown, for the passage of the electron beam 15.
- the thickness of the pane is sufficient to withstand a predetermined pressure differential across it and is typically between 25 microns and 5 microns, and is preferably about 10 microns.
- the electron beam window 10 defines a first surface 24 for receiving a high energy electron beam 15, and a second surface 25 for transmitting the electron beam into the higher pressure chamber 14.
- the passage of the high energy electron beam 15 through the electron beam window 10 generates an electrical charge which will increase until it attains a value that generates an arc-discharge through the thin diamond window pane.
- This destructive electrical charge is proportional to the square of the beam voltage and increases at a rate dependant on the beam current.
- the electron beam window is physically damaged, such damage typically taking the form of a hole punched right through the electron beam window 10, surrounded by collateral crazing of the polycrystalline diamond.
- This invention provides three alternative solutions to this problem, each of which comprises the provision of an electrically conductive path that prevents the electron beam from establishing any significant electrical field across the thickness of the electron beam window 10.
- the electrically conductive path is provided by an electrically conductive layer 26 which adheres to surface 24. It is, of course, important for the electrically conductive layer 26 to be sufficiently thin that it will not significantly impede the passage of electrons through the electron beam window 10. From Figure 2 it will be noted that the conductive layer 26 extends radially outwards to make good electrical contact with the copper sealing gasket 18 which now performs the additional function of earthing the conductive layer 26 to the structure 12.
- FIG. 3 which is identical to Figure 2 except in so far as a second conductive layer 27 is adhered to the second surface 25 of the electron beam window 10.
- This second conductive layer 27 extends radially to form an electrical contact with the bracket 20 which is earthed to the structure 12 by the bolts 21 and their copper washers.
- the electrically conductive layers 26, 27 may be joined together by extending them around the peripheral edge of the electron beam window 10.
- the electrically conductive layer 26, or the electrically conductive layers 26, 27, are preferably formed of aluminium, but may also be formed of magnesium, titanium, platinum, gold, indium tin oxide, and silica doped to make it electrically conductive.
- Each electrically conductive layer may be multilayered, for example, a titanium layer adhered to the window to enhance adhesion and electrical contact, and covered by an aluminium layer to provide the bulk of the electrical conductivity. We have found that a layer thickness of less than one micron is satisfactory and that the layer thickness should normally be between 10 and 100 atoms.
- Each layer may be adhered to its respective surface 24 or 25 by any process known in the art. With an aluminium layer, vacuum deposition or sputtering is convenient.
- the material used for forming the electrically conductive layer 24 and or 25 should have a low attenuation coefficient for high energy electrons (that is ideally to have a low atomic number), a high electrical conductivity when less than than 1000nm thick, be capable of deposition on to diamond with a minimal amount of stress but with adequate adhesion, be realisable onto planar and non-planar diamond surfaces, and be compatible with mounting of the diamond electron beam window to a suitable frame or support 12 such that the layer 24 or 25 is electrically grounded.
- the third solution is not illustrated but can readily be visualised with reference to the general structures illustrated in Figures 2 and 3. Instead of adhering a conductive layer 26 to the surface 24, or a conductive layer 27 to the surface 25, the diamond forming the electron beam window 10 can be treated to render it conductive.
- One method of making CVD diamond conductive is to introduce a dopant, during growth of the diamond, to introduce an impurity that makes the diamond electrically conductive or semi-conductive.
- One such impurity is boron which, in the dopant range of 10 15 to 10 21 , makes CVD diamond electrically semi-conducting or conducting.
- the introduction of boron as a dopant is conveniently achieved by introducing 1,000 ppm of diborane (B 2 H 6 ) into the process gases whilst the CVD diamond is being grown.
- Another option for rendering the electron beam window 10 conductive is to implant dopant atoms within the first micron of the surfaces 24 or 24 and 25 by ion implantation. Such ion implantation generally requires a subsequent annealing process to reduce lattice damage in the diamond and to activate the dopant.
- Another approach is to use a composite electron beam window of which the bulk is pure CVD diamond which has the advantage of high thermal conductivity, but the surfaces 24 and 25 are made as an electrically conducting stratum either by ion implantation of carbon or boron atoms, or by boron doping.
- the main advantage of this solution is that the electron beam window retains high bulk thermal conductivity whilst having very robust, diamond-based electrically conducting surface.
- this solution has the disadvantage in that it is more complex to fabricate. Whilst growing CVD diamond, it is possible to make a first stratum electrically conducting by using a suitable dopant, then stopping the introduction of the dopant whilst the bulk of the CVD diamond is grown, and then by resuming doping for the last stratum of diamond growth.
- the electron beam window 10 is preferably part of an electron beam assembly (not illustrated) which incorporates an electrically conductive mounting plate defining an aperture, the electron beam window being positioned over this aperture, and an hermetic seal being formed between the electron beam window and the mounting plate.
- this electron beam assembly would be positioned over the orifice 17 and secured to the structure 12 by any convenient means, such as the bolts 21 and lock-nuts 22.
- the mounting plate would, of course, need to be sealed to the structure 12 and this can be achieved by arranging a copper gasket between them.
- the hermetic seal must be electrically conducting and can take the form of a mechanical seal, an adhesive, solder, or brazing securing the window 10 to the mounting plate.
- this layer is preferably formed over at least part of a surface of the mounting plate to provide electrical continuity.
- This invention enables diamond electron beam windows to be used for transmitting electron beams having a significantly higher intensity than hitherto.
- the electron beam windows may be of any convenient shape or geometry, for instance curved or part of a spherical shell presenting a convex face towards the higher pressure domain.
- the electron beam window may incorporate supports and/or coolant means as are already known in the art.
Landscapes
- Cold Cathode And The Manufacture (AREA)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP04257542A EP1670017A1 (de) | 2004-12-03 | 2004-12-03 | Elektronendurchlässiges Fenster, Fenstereinheit und Elektronenstrahlerzeuger |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP04257542A EP1670017A1 (de) | 2004-12-03 | 2004-12-03 | Elektronendurchlässiges Fenster, Fenstereinheit und Elektronenstrahlerzeuger |
Publications (1)
Publication Number | Publication Date |
---|---|
EP1670017A1 true EP1670017A1 (de) | 2006-06-14 |
Family
ID=34930879
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP04257542A Withdrawn EP1670017A1 (de) | 2004-12-03 | 2004-12-03 | Elektronendurchlässiges Fenster, Fenstereinheit und Elektronenstrahlerzeuger |
Country Status (1)
Country | Link |
---|---|
EP (1) | EP1670017A1 (de) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106409637A (zh) * | 2010-12-02 | 2017-02-15 | 利乐拉瓦尔集团及财务有限公司 | 电子出射窗箔 |
RU2680823C1 (ru) * | 2018-02-27 | 2019-02-27 | Общество С Ограниченной Ответственностью "Твинн" | Электронная отпаянная пушка для вывода электронного потока в атмосферу или иную газовую среду |
Citations (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3211937A (en) * | 1962-04-20 | 1965-10-12 | Ross E Hester | Carbon-coated electron-transmission window |
US3611418A (en) * | 1967-10-03 | 1971-10-05 | Matsushita Electric Ind Co Ltd | Electrostatic recording device |
US3815094A (en) * | 1970-12-15 | 1974-06-04 | Micro Bit Corp | Electron beam type computer output on microfilm printer |
DE2501885A1 (de) * | 1975-01-18 | 1976-07-22 | Licentia Gmbh | Elektronendurchlaessiges fenster und verfahren zu dessen herstellung |
EP0736780A1 (de) * | 1995-04-07 | 1996-10-09 | Rikagaku Kenkyusho | Verfahren zur Bestimmung und Messung der Lage eines Röntgenstrahls |
WO2001016991A1 (en) * | 1999-08-31 | 2001-03-08 | 3M Innovative Properties Company | Electron beam apparatus having a low loss beam path |
US20020048344A1 (en) * | 2000-10-13 | 2002-04-25 | Bachmann Peter Klaus | Method of manufacturing a window transparent to electron rays, and window transparent to electron rays |
US20020048345A1 (en) * | 2000-10-13 | 2002-04-25 | Bachmann Peter Klaus | Window transparent to electron rays |
US20030131787A1 (en) * | 1998-05-15 | 2003-07-17 | Linares Robert C. | Tunable CVD diamond structures |
US20040222733A1 (en) * | 2001-03-21 | 2004-11-11 | Advanced Electron Beams, Inc. | Electron beam emitter |
-
2004
- 2004-12-03 EP EP04257542A patent/EP1670017A1/de not_active Withdrawn
Patent Citations (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3211937A (en) * | 1962-04-20 | 1965-10-12 | Ross E Hester | Carbon-coated electron-transmission window |
US3611418A (en) * | 1967-10-03 | 1971-10-05 | Matsushita Electric Ind Co Ltd | Electrostatic recording device |
US3815094A (en) * | 1970-12-15 | 1974-06-04 | Micro Bit Corp | Electron beam type computer output on microfilm printer |
DE2501885A1 (de) * | 1975-01-18 | 1976-07-22 | Licentia Gmbh | Elektronendurchlaessiges fenster und verfahren zu dessen herstellung |
EP0736780A1 (de) * | 1995-04-07 | 1996-10-09 | Rikagaku Kenkyusho | Verfahren zur Bestimmung und Messung der Lage eines Röntgenstrahls |
US20030131787A1 (en) * | 1998-05-15 | 2003-07-17 | Linares Robert C. | Tunable CVD diamond structures |
WO2001016991A1 (en) * | 1999-08-31 | 2001-03-08 | 3M Innovative Properties Company | Electron beam apparatus having a low loss beam path |
US20020048344A1 (en) * | 2000-10-13 | 2002-04-25 | Bachmann Peter Klaus | Method of manufacturing a window transparent to electron rays, and window transparent to electron rays |
US20020048345A1 (en) * | 2000-10-13 | 2002-04-25 | Bachmann Peter Klaus | Window transparent to electron rays |
US20040222733A1 (en) * | 2001-03-21 | 2004-11-11 | Advanced Electron Beams, Inc. | Electron beam emitter |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106409637A (zh) * | 2010-12-02 | 2017-02-15 | 利乐拉瓦尔集团及财务有限公司 | 电子出射窗箔 |
RU2680823C1 (ru) * | 2018-02-27 | 2019-02-27 | Общество С Ограниченной Ответственностью "Твинн" | Электронная отпаянная пушка для вывода электронного потока в атмосферу или иную газовую среду |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US7271333B2 (en) | Apparatus and method of production of thin film photovoltaic modules | |
US20040256975A1 (en) | Electrode and associated devices and methods | |
US9020101B2 (en) | Target for X-ray generator, method of manufacturing the same and X-ray generator | |
US4443488A (en) | Plasma ion deposition process | |
US5789859A (en) | Field emission display with non-evaporable getter material | |
JP3044063B2 (ja) | 縁部分の気密シールおよびその製造方法 | |
CN101894725B (zh) | 离子源 | |
CA2006124C (en) | Distributed feedback laser for frequency modulation communication systems | |
JP3689651B2 (ja) | 電子線装置 | |
US10832885B2 (en) | Electron transparent membrane for cold cathode devices | |
EP3170195B1 (de) | Anode, röntgenröhre und radiographiesystem | |
EP2365515A1 (de) | Drehbares Target, Stützrohr, Sputter-Installation und Verfahren zur Herstellung eines drehbaren Targets | |
WO2011011278A1 (en) | Emitter exit window | |
EP1670017A1 (de) | Elektronendurchlässiges Fenster, Fenstereinheit und Elektronenstrahlerzeuger | |
CN103107054B (zh) | 场发射装置 | |
JP2002156499A (ja) | 電子線を通す窓 | |
JPH03140463A (ja) | 薄膜形成装置 | |
US7759871B2 (en) | High temperature seal for electric lamp | |
EP1667189A1 (de) | Fenster für geladenen Teilchen, Fenster-Anordnung, und Teilchenkanone | |
JP3454384B2 (ja) | イオンビーム発生装置及び方法 | |
KR20020097290A (ko) | 디스플레이 소자들을 실링하는 방법 | |
CN102254765A (zh) | 场发射装置的制备方法 | |
US4966095A (en) | Apparatus for forming a thin film | |
JP2729502B2 (ja) | 高速原子線源装置 | |
JPH05205647A (ja) | イオン発生用引出グリッド及びその製造方法並びにこのグリッドを利用したイオン発生装置 |
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): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HU IE IS IT LI LT LU MC NL PL PT RO SE SI SK TR |
|
AX | Request for extension of the european patent |
Extension state: AL BA HR LV MK YU |
|
AKX | Designation fees paid | ||
REG | Reference to a national code |
Ref country code: DE Ref legal event code: 8566 |
|
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: 20061215 |