US3355615A - Ion source having critically dimensioned extraction means - Google Patents
Ion source having critically dimensioned extraction means Download PDFInfo
- Publication number
- US3355615A US3355615A US447792A US44779265A US3355615A US 3355615 A US3355615 A US 3355615A US 447792 A US447792 A US 447792A US 44779265 A US44779265 A US 44779265A US 3355615 A US3355615 A US 3355615A
- Authority
- US
- United States
- Prior art keywords
- enclosure
- ion source
- ion
- plasma
- ions
- 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
Links
- 238000000605 extraction Methods 0.000 title claims description 11
- 150000002500 ions Chemical class 0.000 claims description 40
- 239000000126 substance Substances 0.000 claims description 3
- TVFDJXOCXUVLDH-UHFFFAOYSA-N caesium atom Chemical compound [Cs] TVFDJXOCXUVLDH-UHFFFAOYSA-N 0.000 description 7
- 229910052792 caesium Inorganic materials 0.000 description 6
- 229910052715 tantalum Inorganic materials 0.000 description 6
- GUVRBAGPIYLISA-UHFFFAOYSA-N tantalum atom Chemical compound [Ta] GUVRBAGPIYLISA-UHFFFAOYSA-N 0.000 description 6
- 229910052751 metal Inorganic materials 0.000 description 5
- 239000002184 metal Substances 0.000 description 5
- 238000010438 heat treatment Methods 0.000 description 2
- 150000002739 metals Chemical class 0.000 description 2
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 2
- 229910052721 tungsten Inorganic materials 0.000 description 2
- 239000010937 tungsten Substances 0.000 description 2
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 description 1
- WHXSMMKQMYFTQS-UHFFFAOYSA-N Lithium Chemical compound [Li] WHXSMMKQMYFTQS-UHFFFAOYSA-N 0.000 description 1
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- ZLMJMSJWJFRBEC-UHFFFAOYSA-N Potassium Chemical compound [K] ZLMJMSJWJFRBEC-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 229910052744 lithium Inorganic materials 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- 230000007935 neutral effect Effects 0.000 description 1
- 229910052700 potassium Inorganic materials 0.000 description 1
- 239000011591 potassium Substances 0.000 description 1
- 229910052702 rhenium Inorganic materials 0.000 description 1
- WUAPFZMCVAUBPE-UHFFFAOYSA-N rhenium atom Chemical compound [Re] WUAPFZMCVAUBPE-UHFFFAOYSA-N 0.000 description 1
- 229910052701 rubidium Inorganic materials 0.000 description 1
- IGLNJRXAVVLDKE-UHFFFAOYSA-N rubidium atom Chemical compound [Rb] IGLNJRXAVVLDKE-UHFFFAOYSA-N 0.000 description 1
- 229910052708 sodium Inorganic materials 0.000 description 1
- 239000011734 sodium Substances 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J27/00—Ion beam tubes
- H01J27/02—Ion sources; Ion guns
- H01J27/26—Ion sources; Ion guns using surface ionisation, e.g. field effect ion sources, thermionic ion sources
Definitions
- the present invention relates to ion source, and especially to an improved mode of extracting the ions from the source.
- Another object of this invention is to provide an ion source capable of producing a high degree of ionization.
- Still another object of this invention is to provide an ion source of high efiiciency.
- a further object of the present invention is to provide an ion source in which the power required for heating the source is relatively reduced.
- a still further object of the invention is to provide an ion source of relatively simple construction.
- an ion source including an enclosure, means for producing a plasma in said enclosure by ionization of a gaseous substance, and means for extracting the ions from said enclosure, characterized by the fact that the extracting means comprise one or several grids having extraction holes of circular or other shape, the value of the diameter or the width of the holes being, in meters, equal to or less than 2R where T being the temperature in degrees Kelvin of the enclosure, and 11 the number of ions or electrons per m. of the plasma, the thickness of the grids being of the same order of magnitude as the diameter or the width of the holes.
- FIG. 1 represents diagrammatically an example of an embodiment of the invention
- FIGURES 2 and 3 explain the principle of the invention
- FIG. 4 is an example of an abacus usable in achieving the invention.
- an ion source comprising an ionization chamber or enclosure 1 having tantalum walls 2 that may be brought to a desired temperature for example, by means of a heater filament 3.
- the enclosure 1 communicates 'by way of a channel 4 with a reservoir of caesium 5 which may likewise be brought to a desired temperature by appropriate means, not shown in this figure.
- the upper Wall of enclosure 1 is partially apertured and the apertures are covered by grids 6.
- An extractor electrode 7, disposed above enclosure 1 and set at a negative potential with respect to the enclosure by means of a source of potential (not shown) comprises apertures facing the grids 6.
- caesium vapor produced by heating the reservoir 5, penetrates into enclosure 1 which is maintained at a high temperature, say between 1400 K. and 2200 K., and the caesium atoms are dissociated into electrons and positive ions.
- This phenomenon known as surface ionization or contact ionization, results in the formation of a plasma in the interior of enclosure 1.
- the plasma that comprises electrons, positive ions also a certain proportion of neutral atoms
- a sheath composed to a great extent of ions, is comprised between the walls and the plasma if the work function of the walls is higher than the plasma potential.
- the ion density (number of ions per unit volume) is therefore considerably higher in the sheath adjacent the walls than in the plasma which occupies the remainder of the enclosure.
- FIGURES 2 and 3 permit to see what happens when the radius of the extraction orifice does or does not exceed the thickness of the ion sheath.
- the plasma is designated by reference numeral 8
- the enclosure wall by 2
- the ion sheath, indicated by the signs is designated by the reference 9.
- the radius of the orifice provided in wall 2 is greater than the thickness of sheath 9. Within this orifice the ions of sheath 9 surround a portion of plasma 8. On the contrary, in the case of FIGURE 3 where the orifice radius is equal to the thickness of sheath 9, only the ions of the sheath traverse the orifice without any portion of the plasma being drawn along. As a result, the mean density of the ion current and the ionization degree are much higher in the case of FIG. 3 than in the case of FIG. 2. I
- the orifices of the grids 6 are given a radius equal to or less than the thickness R of the ion sheath.
- the units employed are those of the international system (M.K.S.A.).
- FIGURE 4 is an abacus indicating the thickness R, in microns, of the ion layer in a tantalum enclosure versus the temperature T (in degrees Kelvin) of a caesium reservoir for different temperatures T of the tantalum. It may be seen on this abacus that, for example, for tantalum walls heated at 1600 K. and a reservoir of caesium at 425 K. the thickness of the ion sheath is 2071.. Under these conditions use is made, in accordance with the invention, of extraction orifices of a diameter that does not exceed 40 i, and thus ion currents of the order of 40 ma./cm. are obtained.
- the thickness of grids 6 is given a value of preferably the same order as the diameter or the width of the orifices. It has been found, in effect, that the ion current is not affected by the thickness of the grids. On the other hand, it is obvious that thick grids (deep holes) bring about pressure losses which are practically inexistent in thin grids (non-deep holes), so that with thin grids it sufiices to heat the reservoir that supplies the metal vapor, to a lower temperature than in the case of thick grids.
- caesium and tantalum have been mentioned, but instead of caesium other metals may be used that are easy to ionize (potassium, lithium, rubidium, sodium, etc.) and the tantalum may be replaced by other metals having a high work function (tungsten, molybdenum, rhenium, etc.).
- tungsten molybdenum, rhenium, etc.
- the extraction orifices may have a cross-section of any desired shape: circular, square, rectangular, triangular, etc., and the grids may be replaced by nets of parallel wires, separated by narrow intervals.
- the ion extraction is effected, in accordance with the invention, through passages whose width does not exceed the double of the thickness of the ion sheath, adjacent the walls of the isothermal cavity.
- An ion source including an enclosure, means for producing a plasma in said enclosure by ionization of a gaseous substance, andmeans for extracting the ions from said enclosure, said extracting means including at least one grid provided with substantially circular extraction holes having a diameter at most equal, in meters,
- T being the temperature in degrees Kelvin of the enclosure
- n the number of ions or electrons per m. of the plasma.
- T being the temperature in degrees Kelvin of the enclosure
- n the number of ions or electrons per m9 of the plasma.
Landscapes
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Combustion & Propulsion (AREA)
- Electron Sources, Ion Sources (AREA)
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| FR972401A FR1402020A (fr) | 1964-04-27 | 1964-04-27 | Perfectionnements aux sources d'ions |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US3355615A true US3355615A (en) | 1967-11-28 |
Family
ID=8828750
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US447792A Expired - Lifetime US3355615A (en) | 1964-04-27 | 1965-04-13 | Ion source having critically dimensioned extraction means |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US3355615A (fr) |
| DE (1) | DE1261605B (fr) |
| FR (1) | FR1402020A (fr) |
| GB (1) | GB1033447A (fr) |
Cited By (24)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3660715A (en) * | 1970-08-18 | 1972-05-02 | Atomic Energy Commission | Ion source with mosaic ion extraction means |
| US3864575A (en) * | 1970-07-25 | 1975-02-04 | Nujeeb Hashmi | Contact ionization ion source |
| US3930163A (en) * | 1974-03-22 | 1975-12-30 | Varian Associates | Ion beam apparatus with separately replaceable elements |
| US3955091A (en) * | 1974-11-11 | 1976-05-04 | Accelerators, Inc. | Method and apparatus for extracting well-formed, high current ion beams from a plasma source |
| US4001582A (en) * | 1974-06-28 | 1977-01-04 | Agence Nationale De Valorisation De La Recherche (Anvar) | Local surface analysis |
| EP0021140A1 (fr) * | 1979-06-29 | 1981-01-07 | International Business Machines Corporation | Source ionique dans une chambre sous vide et procédé pour son fonctionnement |
| US4246481A (en) * | 1978-02-08 | 1981-01-20 | Max-Planck-Gesellschaft Zur Foerderung Der Wissenschaften E.V. | Contact ionization apparatus |
| US4833319A (en) * | 1987-02-27 | 1989-05-23 | Hughes Aircraft Company | Carrier gas cluster source for thermally conditioned clusters |
| US20020108933A1 (en) * | 2000-03-17 | 2002-08-15 | Applied Materials, Inc. | Plasma reactor with overhead RF electrode tuned to the plasma with arcing suppression |
| US6586886B1 (en) | 2001-12-19 | 2003-07-01 | Applied Materials, Inc. | Gas distribution plate electrode for a plasma reactor |
| US20040226657A1 (en) * | 2003-05-16 | 2004-11-18 | Applied Materials, Inc. | Plasma density, energy and etch rate measurements at bias power input and real time feedback control of plasma source and bias power |
| US20050178748A1 (en) * | 2000-03-17 | 2005-08-18 | Applied Materials, Inc. | Plasma reactor overhead source power electrode with low arcing tendency, cylindrical gas outlets and shaped surface |
| US7141757B2 (en) | 2000-03-17 | 2006-11-28 | Applied Materials, Inc. | Plasma reactor with overhead RF source power electrode having a resonance that is virtually pressure independent |
| US7186943B2 (en) | 2000-03-17 | 2007-03-06 | Applied Materials, Inc. | MERIE plasma reactor with overhead RF electrode tuned to the plasma with arcing suppression |
| US7220937B2 (en) | 2000-03-17 | 2007-05-22 | Applied Materials, Inc. | Plasma reactor with overhead RF source power electrode with low loss, low arcing tendency and low contamination |
| US7359177B2 (en) | 2005-05-10 | 2008-04-15 | Applied Materials, Inc. | Dual bias frequency plasma reactor with feedback control of E.S.C. voltage using wafer voltage measurement at the bias supply output |
| US7452824B2 (en) | 2003-05-16 | 2008-11-18 | Applied Materials, Inc. | Method of characterizing a chamber based upon concurrent behavior of selected plasma parameters as a function of plural chamber parameters |
| US7470626B2 (en) | 2003-05-16 | 2008-12-30 | Applied Materials, Inc. | Method of characterizing a chamber based upon concurrent behavior of selected plasma parameters as a function of source power, bias power and chamber pressure |
| US7795153B2 (en) | 2003-05-16 | 2010-09-14 | Applied Materials, Inc. | Method of controlling a chamber based upon predetermined concurrent behavior of selected plasma parameters as a function of selected chamber parameters |
| US7901952B2 (en) | 2003-05-16 | 2011-03-08 | Applied Materials, Inc. | Plasma reactor control by translating desired values of M plasma parameters to values of N chamber parameters |
| US7910013B2 (en) | 2003-05-16 | 2011-03-22 | Applied Materials, Inc. | Method of controlling a chamber based upon predetermined concurrent behavior of selected plasma parameters as a function of source power, bias power and chamber pressure |
| US7955986B2 (en) | 2002-05-22 | 2011-06-07 | Applied Materials, Inc. | Capacitively coupled plasma reactor with magnetic plasma control |
| US8048806B2 (en) | 2000-03-17 | 2011-11-01 | Applied Materials, Inc. | Methods to avoid unstable plasma states during a process transition |
| US8617351B2 (en) | 2002-07-09 | 2013-12-31 | Applied Materials, Inc. | Plasma reactor with minimal D.C. coils for cusp, solenoid and mirror fields for plasma uniformity and device damage reduction |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3268180B2 (ja) * | 1994-11-18 | 2002-03-25 | 株式会社東芝 | イオン発生装置、イオン照射装置、及び半導体装置の製造方法 |
| USD978226S1 (en) * | 2020-11-10 | 2023-02-14 | Emart International Inc | Collapsible screen |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3185849A (en) * | 1962-11-30 | 1965-05-25 | Exxon Production Research Co | Pulsed neutron source utilizing an accelerator tube |
| US3263415A (en) * | 1961-03-06 | 1966-08-02 | Aerojet General Co | Ion propulsion device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR1327142A (fr) * | 1961-04-10 | 1963-05-17 | Du Pont | Procédé de polymérisation des composés éthyléniquement non saturés et catalyseur pour ce procédé |
-
1964
- 1964-04-27 FR FR972401A patent/FR1402020A/fr not_active Expired
-
1965
- 1965-04-13 US US447792A patent/US3355615A/en not_active Expired - Lifetime
- 1965-04-21 GB GB16692/65A patent/GB1033447A/en not_active Expired
- 1965-04-27 DE DEC35700A patent/DE1261605B/de active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3263415A (en) * | 1961-03-06 | 1966-08-02 | Aerojet General Co | Ion propulsion device |
| US3185849A (en) * | 1962-11-30 | 1965-05-25 | Exxon Production Research Co | Pulsed neutron source utilizing an accelerator tube |
Cited By (31)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3864575A (en) * | 1970-07-25 | 1975-02-04 | Nujeeb Hashmi | Contact ionization ion source |
| US3660715A (en) * | 1970-08-18 | 1972-05-02 | Atomic Energy Commission | Ion source with mosaic ion extraction means |
| US3930163A (en) * | 1974-03-22 | 1975-12-30 | Varian Associates | Ion beam apparatus with separately replaceable elements |
| US4001582A (en) * | 1974-06-28 | 1977-01-04 | Agence Nationale De Valorisation De La Recherche (Anvar) | Local surface analysis |
| US3955091A (en) * | 1974-11-11 | 1976-05-04 | Accelerators, Inc. | Method and apparatus for extracting well-formed, high current ion beams from a plasma source |
| US4246481A (en) * | 1978-02-08 | 1981-01-20 | Max-Planck-Gesellschaft Zur Foerderung Der Wissenschaften E.V. | Contact ionization apparatus |
| EP0021140A1 (fr) * | 1979-06-29 | 1981-01-07 | International Business Machines Corporation | Source ionique dans une chambre sous vide et procédé pour son fonctionnement |
| US4833319A (en) * | 1987-02-27 | 1989-05-23 | Hughes Aircraft Company | Carrier gas cluster source for thermally conditioned clusters |
| US7186943B2 (en) | 2000-03-17 | 2007-03-06 | Applied Materials, Inc. | MERIE plasma reactor with overhead RF electrode tuned to the plasma with arcing suppression |
| US20050178748A1 (en) * | 2000-03-17 | 2005-08-18 | Applied Materials, Inc. | Plasma reactor overhead source power electrode with low arcing tendency, cylindrical gas outlets and shaped surface |
| US7030335B2 (en) | 2000-03-17 | 2006-04-18 | Applied Materials, Inc. | Plasma reactor with overhead RF electrode tuned to the plasma with arcing suppression |
| US7141757B2 (en) | 2000-03-17 | 2006-11-28 | Applied Materials, Inc. | Plasma reactor with overhead RF source power electrode having a resonance that is virtually pressure independent |
| US20020108933A1 (en) * | 2000-03-17 | 2002-08-15 | Applied Materials, Inc. | Plasma reactor with overhead RF electrode tuned to the plasma with arcing suppression |
| US7196283B2 (en) | 2000-03-17 | 2007-03-27 | Applied Materials, Inc. | Plasma reactor overhead source power electrode with low arcing tendency, cylindrical gas outlets and shaped surface |
| US7220937B2 (en) | 2000-03-17 | 2007-05-22 | Applied Materials, Inc. | Plasma reactor with overhead RF source power electrode with low loss, low arcing tendency and low contamination |
| US8048806B2 (en) | 2000-03-17 | 2011-11-01 | Applied Materials, Inc. | Methods to avoid unstable plasma states during a process transition |
| US6586886B1 (en) | 2001-12-19 | 2003-07-01 | Applied Materials, Inc. | Gas distribution plate electrode for a plasma reactor |
| US7955986B2 (en) | 2002-05-22 | 2011-06-07 | Applied Materials, Inc. | Capacitively coupled plasma reactor with magnetic plasma control |
| US8617351B2 (en) | 2002-07-09 | 2013-12-31 | Applied Materials, Inc. | Plasma reactor with minimal D.C. coils for cusp, solenoid and mirror fields for plasma uniformity and device damage reduction |
| US7585685B2 (en) | 2003-05-16 | 2009-09-08 | Applied Materials, Inc. | Method of determining wafer voltage in a plasma reactor from applied bias voltage and current and a pair of constants |
| US7452824B2 (en) | 2003-05-16 | 2008-11-18 | Applied Materials, Inc. | Method of characterizing a chamber based upon concurrent behavior of selected plasma parameters as a function of plural chamber parameters |
| US7470626B2 (en) | 2003-05-16 | 2008-12-30 | Applied Materials, Inc. | Method of characterizing a chamber based upon concurrent behavior of selected plasma parameters as a function of source power, bias power and chamber pressure |
| US7521370B2 (en) | 2003-05-16 | 2009-04-21 | Applied Materials, Inc. | Method of operating a plasma reactor chamber with respect to two plasma parameters selected from a group comprising ion density, wafer voltage, etch rate and wafer current, by controlling chamber parameters of source power and bias power |
| US7553679B2 (en) | 2003-05-16 | 2009-06-30 | Applied Materials, Inc. | Method of determining plasma ion density, wafer voltage, etch rate and wafer current from applied bias voltage and current |
| US7795153B2 (en) | 2003-05-16 | 2010-09-14 | Applied Materials, Inc. | Method of controlling a chamber based upon predetermined concurrent behavior of selected plasma parameters as a function of selected chamber parameters |
| US7901952B2 (en) | 2003-05-16 | 2011-03-08 | Applied Materials, Inc. | Plasma reactor control by translating desired values of M plasma parameters to values of N chamber parameters |
| US7910013B2 (en) | 2003-05-16 | 2011-03-22 | Applied Materials, Inc. | Method of controlling a chamber based upon predetermined concurrent behavior of selected plasma parameters as a function of source power, bias power and chamber pressure |
| US7247218B2 (en) * | 2003-05-16 | 2007-07-24 | Applied Materials, Inc. | Plasma density, energy and etch rate measurements at bias power input and real time feedback control of plasma source and bias power |
| US20040226657A1 (en) * | 2003-05-16 | 2004-11-18 | Applied Materials, Inc. | Plasma density, energy and etch rate measurements at bias power input and real time feedback control of plasma source and bias power |
| US7375947B2 (en) | 2005-05-10 | 2008-05-20 | Applied Materials, Inc. | Method of feedback control of ESC voltage using wafer voltage measurement at the bias supply output |
| US7359177B2 (en) | 2005-05-10 | 2008-04-15 | Applied Materials, Inc. | Dual bias frequency plasma reactor with feedback control of E.S.C. voltage using wafer voltage measurement at the bias supply output |
Also Published As
| Publication number | Publication date |
|---|---|
| FR1402020A (fr) | 1965-06-11 |
| GB1033447A (en) | 1966-06-22 |
| DE1261605B (de) | 1968-02-22 |
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