US2950390A - Electron lenses - Google Patents

Electron lenses Download PDF

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Publication number
US2950390A
US2950390A US760397A US76039758A US2950390A US 2950390 A US2950390 A US 2950390A US 760397 A US760397 A US 760397A US 76039758 A US76039758 A US 76039758A US 2950390 A US2950390 A US 2950390A
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US
United States
Prior art keywords
specimen
electron
plate
pole
cylindrical
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
Application number
US760397A
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English (en)
Inventor
Haine Michael Edward
Mulvey Thomas
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Metropolitan Vickers Electrical Co Ltd
Original Assignee
Metropolitan Vickers Electrical Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Priority claimed from GB28674/57A external-priority patent/GB847266A/en
Application filed by Metropolitan Vickers Electrical Co Ltd filed Critical Metropolitan Vickers Electrical Co Ltd
Application granted granted Critical
Publication of US2950390A publication Critical patent/US2950390A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/02Details
    • H01J37/04Arrangements of electrodes and associated parts for generating or controlling the discharge, e.g. electron-optical arrangement, ion-optical arrangement
    • H01J37/10Lenses
    • H01J37/14Lenses magnetic
    • H01J37/141Electromagnetic lenses
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F42AMMUNITION; BLASTING
    • F42CAMMUNITION FUZES; ARMING OR SAFETY MEANS THEREFOR
    • F42C13/00Proximity fuzes; Fuzes for remote detonation
    • F42C13/04Proximity fuzes; Fuzes for remote detonation operated by radio waves
    • 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
    • G01N23/225Investigating 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 using electron or ion
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/02Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
    • G01S13/50Systems of measurement based on relative movement of target
    • G01S13/505Systems of measurement based on relative movement of target using Doppler effect for determining closest range to a target or corresponding time, e.g. miss-distance indicator
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/02Details
    • H01J37/20Means for supporting or positioning the objects or the material; Means for adjusting diaphragms or lenses associated with the support

Definitions

  • This invention relates to electron lenses and has an important application in X-ray analysing apparatus of the kind described in co-pending application Serial No. 760,472, in which analysis of elements is carried out by bombarding the surface of a specimen with a beam of electrons and examining the wavelengths of the X-rays thereby produced.
  • the electron beam shall be of small cross-section and also that there shall be a large electron current in order to obtain a satisfactory X-ray emission.
  • the current I is determined by the relationship where C is the spherical aberration coefficient of the lens, is the current density per unit solid angle from the cathode of the electron gun. Hence a small spherical aberration is necessary for a large current and in electron lens arrangements, as hitherto employed, this has usually been achieved by locating the specimen in a strong magnetic field between the pole pieces.
  • the main object of the invention is to provide an improved electron lens arrangement in which the difficulties above referred to are substantially avoided or minimised.
  • an electron lens arrangement comprises an annular magnet assembly adapted to encircle the beam path concentrically therewith and com-prising axially displaced annular poles of which one pole is formed by the edge of a small aperture in a plate extending transversely across the electron beam path and with the aperture centrally located for the beam and the other pole is formed by a cylindrical plate of large internal diameter relative to the working distance of the specimen and concentric with the beam path and spaced axially from said lateral plate together with means for positioning the specimen in the electron beam path in a region beyond said apertured plate and outside the magnetic structure and in which there is a negligible magnetic field.
  • working distance implies the distance between the last working surface of the lens and the focal point at which the specimen is located.
  • the working distance of the specimen beyond the structure is large to make it easy to extract the X-ray beam. It will be appreciated that with such an arrangement in which the specimen is located outside the magnetic structure it is possible to extract the X-rays without undue ditficulty as it is not necessary to provide an X-ray passage through the structure and this result is obtained without appreciably increasing the spherical aberration since the diameter of the cylindhical pole is larger.
  • the specimen is outside the magnetic field and the transverse apertured plate acts, to a large extent, as a screen between the specimen and the electron lens, it cannot appreciably distort the electron lens field and it is possible to examine specimens of magnetic material, e.g. iron.
  • Fig. l is a cross sectional view showing diagrammatically a known form of electron lens for purposes of comparison, whilst Fig. 2 shows an improved electron lens constructed in accordance with the invention, and
  • fig. 3 shows one embodiment of the invention.
  • the lens shown comprises an annular magnet winding 1 surrounded by a yoke '2, one pole piece is formed by the internal edge 3 of a plate 4 whilst the other pole piece 5 is formed by an internal lip on the end of a cylindrical wall 6; the specimen 7 in such arrangements is located substantially between the pole pieces 3 and 5 and in a region of strong magnetic field to reduce spherical aberration.
  • Fig. 2 shows an improved construction in accordance with the invention in which like parts have been given similar references with a prime
  • the transverse plate 4 is formed with a small central aperture 8 bordered by the annular pole pieces 3' and that this pole is of reduced section.
  • the gap between the pole pieces extends annularly between the pole pieces 5' and the lower face of the transverse plate 4' and the internal diameter of the cylindrical plate 6' is large compared with that of the arrangement of Fig, 1.
  • Fig. 3 shows an arrangement in which the specimen 7 is mounted on a rotatable carrier 9 mounted on a spindle 10 extending through the cylindrical casing wall 11 of the apparatus.
  • an electron lens arrangement comprising concentric cylindrical plates encircling the electron beam path, an energising winding located in the annular space between said cylindrical plates, at first annular end plate joining corresponding end edges of the cylindrical plates, an edge to the inner cylindrical plate at the opposite end to said annular plate which edge forms a 'firstmagnetic pole, a transverse plate extending across the electronbeam path in spaced relationship with the pole forming the edge of said innercylindrical plate and secured along its periphery to, the correspond ing end of the outer cylindrical plate, said transverse plate having a circular aperture defined by an edge-concentric with the beam path, saidedg'e forming a second magnetic pole face, means for positioning a specimen in the beam path beyond said transverse plate, a cylindrical casing extending axially of the beam path away from said transverse plate and encircling the beam path and specimen and an aperture in said casing adapted to permit X-ra-ys from the specimen to pass out from the

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  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Radar, Positioning & Navigation (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Electromagnetism (AREA)
  • General Engineering & Computer Science (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Analysing Materials By The Use Of Radiation (AREA)
  • Radar Systems Or Details Thereof (AREA)
US760397A 1957-09-11 1958-09-11 Electron lenses Expired - Lifetime US2950390A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
GB28674/57A GB847266A (en) 1960-12-15 1957-09-11 Improvements relating to electron lenses
FR846971A FR1283259A (fr) 1960-12-15 1960-12-15 Dispositif permettant la mesure de la distance de deux objets dont un au moins est mobile

Publications (1)

Publication Number Publication Date
US2950390A true US2950390A (en) 1960-08-23

Family

ID=32395580

Family Applications (2)

Application Number Title Priority Date Filing Date
US760397A Expired - Lifetime US2950390A (en) 1957-09-11 1958-09-11 Electron lenses
US159374A Expired - Lifetime US3140488A (en) 1957-09-11 1961-12-14 Miss distance indicator

Family Applications After (1)

Application Number Title Priority Date Filing Date
US159374A Expired - Lifetime US3140488A (en) 1957-09-11 1961-12-14 Miss distance indicator

Country Status (5)

Country Link
US (2) US2950390A (fr)
CH (1) CH364373A (fr)
DE (2) DE1096061B (fr)
FR (1) FR1203259A (fr)
GB (1) GB1004873A (fr)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1806891A1 (de) * 1967-11-03 1969-06-19 Nat Res Dev Einrichtung zur Fokussierung von aus geladenen Teilchen bestehenden Strahlen
US4209702A (en) * 1977-07-25 1980-06-24 Kabushiki Kaisha Akashi Seisakusho Multiple electron lens

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1265996B (de) * 1964-05-22 1968-04-11 Dornier System Gmbh Schatungsanordnung zur Erfassung der Anzahl von Treffern
DE1428724A1 (de) * 1964-08-27 1969-03-06 Dornier System Gmbh Verfahren zum Erfassen von Treffern bzw. vorbeifliegenden Geschossen mittels elektromagnetischer Strahlung
US3390348A (en) * 1966-04-28 1968-06-25 Aga Ab System for generating a signal representing the time delay of a signal patch
GB1434532A (en) * 1972-05-03 1976-05-05 Decca Ltd Multiple frequency continuous wave radars
FR2204811B1 (fr) * 1972-10-31 1977-04-01 Thomson Csf
SE431253B (sv) * 1977-08-10 1984-01-23 Microwave & Electronic Syst System for metning av minimiavstand mellan forsta och andra foremal som ror sig i forhallande till varandra
DE3215479A1 (de) * 1982-04-24 1988-08-18 Krupp Atlas Elektronik Gmbh Verfahren zum bestimmen von zeitspannen

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SE113186C1 (fr) * 1941-11-29 1945-02-13
US2440640A (en) * 1946-11-27 1948-04-27 Research Corp Electron microanalyzer
US2849619A (en) * 1948-10-01 1958-08-26 Siemens Ag Electron microscope having a multiplespecimen carrier

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SE113186C1 (fr) * 1941-11-29 1945-02-13
US2440640A (en) * 1946-11-27 1948-04-27 Research Corp Electron microanalyzer
US2849619A (en) * 1948-10-01 1958-08-26 Siemens Ag Electron microscope having a multiplespecimen carrier

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1806891A1 (de) * 1967-11-03 1969-06-19 Nat Res Dev Einrichtung zur Fokussierung von aus geladenen Teilchen bestehenden Strahlen
US4209702A (en) * 1977-07-25 1980-06-24 Kabushiki Kaisha Akashi Seisakusho Multiple electron lens

Also Published As

Publication number Publication date
GB1004873A (en) 1965-09-15
US3140488A (en) 1964-07-07
DE1096061B (de) 1960-12-29
DE1251828B (fr)
CH364373A (de) 1962-09-15
FR1203259A (fr) 1960-01-18

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