US3240931A - Spatial discriminator for particle beams - Google Patents
Spatial discriminator for particle beams Download PDFInfo
- Publication number
- US3240931A US3240931A US226962A US22696262A US3240931A US 3240931 A US3240931 A US 3240931A US 226962 A US226962 A US 226962A US 22696262 A US22696262 A US 22696262A US 3240931 A US3240931 A US 3240931A
- Authority
- US
- United States
- Prior art keywords
- channel
- channels
- multipliers
- anodes
- particle beams
- 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
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J49/00—Particle spectrometers or separator tubes
- H01J49/02—Details
- H01J49/025—Detectors specially adapted to particle spectrometers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
- G01T1/2914—Measurement of spatial distribution of radiation
- G01T1/2921—Static instruments for imaging the distribution of radioactivity in one or two dimensions; Radio-isotope cameras
- G01T1/2957—Static instruments for imaging the distribution of radioactivity in one or two dimensions; Radio-isotope cameras using channel multiplier arrays
Definitions
- This invention relates to a high resolution spatial discriminator for particle beams.
- This invention provides improved means for detecting and measuring the cross-sectional spatial distribution of particle beams.
- an array of channel electron multipliers hereinafter described, are positioned to receive the particles in a beam.
- the particles of the beam are received in different channels depending on their spatial distribution, are multiplied in the channels through secondary emission and are detected at the output of these channels to provide an indication of the content of the beam. Because of the small size of the channels, very accurate determination can be made of the cross section of the beam and further, because of the multiplication provided low intensity and low energy beams can be analyzed.
- FIGURE 1 is a schematic diagram illustrating an embodiment of the invention and a source for providing a beam of particles.
- FIGURE 2 is a perspective view, partly broken away, of the multipliers shown in FIGURE 1. It also shows a portion of the electrical circuitry connected to the multipliers.
- a particle beam is obtained from the ion source 1 of a magnetic mass spectrometer.
- the ions exit through the slit 2 with equal velocities and a magnetic field deflects them spatially according to mass.
- the ions of different mass will travel different circular paths.
- the radius of travel of each ion is determined by the following equation:
- ions of a given mass M may travel along path 4
- ions of heavier mass M may travel along path 6
- ions of still heavier mass M may travel along path 8.
- the ions in each path will 3,240,931 Patented Mar. 15, 1966 be distributed in a plane perpendicular to the direction of travel.
- a substantially parallel array of channel electron multipliers Positioned to receive the ions from the source 1 is a substantially parallel array of channel electron multipliers generally indicated at 10.
- Tubular channel multipliers of the type used to construct the multipliers 10 are fully disclosed in copen-ding US. application serial No. 23,574, filed April 20, 1960, by George W. Goodrich and William C. Wiley, and issued on April 7, 1964, as US. Patent No. 3,128,408.
- Such tube type multipliers are provided with an inside surface which is conductive and has secondary emission properties. Upon the application of a voltage difference between the ends of the tube, current flows through the tube and produces an electric field in an axial direction through the region defined by the tube. Electrons entering the input end of the tube are multiplied through secondary emission before they emerge from the output end of the tube.
- the multipliers 10 are constructed with a plurality of bismuth-lead oxide glass tubes of very small inside diameter such as .001 inch. Initially, the glass tubes are placed in a hydrogen reducing furnace to reduce the bismuth and lead oxides. This converts the glass tubes from an insulator to a semi-conductor of relatively high resistance. Then a suflicient number of tubes are stacked in parallel relationship to one another and are fused together such as by heating them in a furnace to the softening point of the glass and allowing them to cool. A relatively small wafer, such as .050 inch, is then sliced from the fused tubes in a direction perpendicular to the axis of the tubes to form the multipliers 10.
- Adjoining the output ends of the multipliers 10 is a base 16 of insulating material, such as glass. Potted in the base 16 are anode wires corresponding in number to the number of multipliers 10, each wire positioned at the output of a particular channel to provide a collecting anode for said channel.
- anode wires 18 at the outputs of the channels in column 20 are connected through a common terminal to an ammeter 22 for providing an indication of the signal detected by the anodes 18.
- anode wires 24, 26, 28 and 30 at the outputs of the channels in columns 32, 34, 36 and 38, respectively, are connected through common terminals to ammeters 4-0, 42, 44 and 46 respectively.
- the ammeters 22, 4d, 42, 44 and 46 have their second terminal grounded.
- Direct voltages of suitable magnitude are applied to the elements disclosed above from a direct voltage source (not shown). For example, as shown in FIGURE 2, direct voltages such as 2,000 volts and volts are applied respectively to the coatings 12 and 14. Also direct voltages such as +50 volts are applied to the anodes 13, 24, 26, 28 and 30 from the voltage source.
- the ion source 1, the multipliers 10 and the base 16 operate in a vacuum tube at a pressure of approximately 10- mm' Hg. Also, a magnetic field is provided in the vacuum tube to cause the ions to travel in the paths shown in FIGURE 2.
- the multipliers 10 are positioned relative to the source 1 to receive the ions emerging from the source. As shown in FIGURE 1, the ions following paths 4, 6 and 8 will enter the channels in columns 20, 34, and 38 respectively. When the ions strike the internal surface of the channels, they will produce secondary emission of electrons which are multiplied through further secondary emission as they pass through the channels.
- the ion signals from masses M M and M multiplied in this manner are collected by the anode wires 18, 26, and 30 respectively, and the ammeters 22, 42 and 46 will provide an indication of the relative quantities of these different masses.
- the discriminator disclosed above has definite advantages. It has extremely high resolution because of the small size of the channels which have a diameter on the order of .001 inch or less. Further, because of the multiplication produced in the channels, it can be very efiectively used to determine the cross section of low intensity particle beams.
- the discriminator can be used for detecting particle beams of all types. For example, it can be used to determine the cross section of beams produced by particle accelerators and of experimental molecular beams. In such cases it may be desirable to have a separate indicator connected to the anode of each channel instead of having a plurality of anodes connected to a common indicator as shown in FIGURE 2. By providing a separate indicator for each channel, excellent analysis can be made of the cross section of a beam.
- a spatial discriminator for determining the cross section of a particle beam comprising,
- each channel receiving a difiierent part of the beam, each channel having a diameter of less than .010 inch,
- a spatial discriminator for determining the cross section of a particle beam comprising,
- channel electron multipliers positioned to receive the beam at its input, different groups of the channels being positioned to receive different portions of the beam, each channel having a diameter of less than .010 inch,
- each common terminal and means connected to each common terminal to provide an indication of the particles in the portion of beam received by the group of channels associated with the common terminal.
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Electron Tubes For Measurement (AREA)
- Measurement Of Radiation (AREA)
Description
March 15, 1966 W. C. WILEY ETAL SPATIAL DISCRIMINATOR FOR PARTICLE BEAMS Filed Sept. 28, 1962 INVENTOR. GEORGE W. GOODRICH ROBERT R. THOMPSON WILLIAM C. WILEY fizz ATT NEY United States Patent 3,240,931 SPATIAL DHSCRIMINATOR FOR PARTICLE BEAMS William C. Wiley, Northville, Robert R. Thompson, Li-
vonia, and George W. Goodrich, Oak Park, Mich., assignors to The Bendix Corporation, Southfield, Mich, a corporation of Delaware Filed Sept. 28, 1962, Ser. No. 226,962
2 Claims. (Cl. 250-413) This invention relates to a high resolution spatial discriminator for particle beams.
Many situations arise in physics and engineering where one has a beam of particles which rnust be detected. Mass spectrometers, particle accelerators, vacuum tube investigations and molecular beam experiments are but a few such cases. item, it is desirable to hrave a detector which permits easy determination of the cross-sectional spatial distribution of the beam. One method which has been employed for this purpose in the past is the use of nuclear emulsion films. Another method is the use of phosphor screens. These methods are disadvantageous in that they are slow, insensitive, or work only for high energy particles.
This invention provides improved means for detecting and measuring the cross-sectional spatial distribution of particle beams. In accordance with the invention an array of channel electron multipliers, hereinafter described, are positioned to receive the particles in a beam. The particles of the beam are received in different channels depending on their spatial distribution, are multiplied in the channels through secondary emission and are detected at the output of these channels to provide an indication of the content of the beam. Because of the small size of the channels, very accurate determination can be made of the cross section of the beam and further, because of the multiplication provided low intensity and low energy beams can be analyzed.
Other objects and advantages will become apparent from the following detailed description and from the appended drawings and claims.
In the drawings:
FIGURE 1 is a schematic diagram illustrating an embodiment of the invention and a source for providing a beam of particles.
FIGURE 2 is a perspective view, partly broken away, of the multipliers shown in FIGURE 1. It also shows a portion of the electrical circuitry connected to the multipliers.
In the embodiment illustrated, a particle beam is obtained from the ion source 1 of a magnetic mass spectrometer. The ions exit through the slit 2 with equal velocities and a magnetic field deflects them spatially according to mass. The ions of different mass will travel different circular paths. The radius of travel of each ion is determined by the following equation:
where r=radius v=velocity of the ion e=charge of the ion B=magnetic field strength m=mass of ion For example, as shown in FIGURE 1, ions of a given mass M may travel along path 4, ions of heavier mass M may travel along path 6 and ions of still heavier mass M may travel along path 8. The ions in each path will 3,240,931 Patented Mar. 15, 1966 be distributed in a plane perpendicular to the direction of travel.
Positioned to receive the ions from the source 1 is a substantially parallel array of channel electron multipliers generally indicated at 10. Tubular channel multipliers of the type used to construct the multipliers 10 are fully disclosed in copen-ding US. application serial No. 23,574, filed April 20, 1960, by George W. Goodrich and William C. Wiley, and issued on April 7, 1964, as US. Patent No. 3,128,408. Such tube type multipliers are provided with an inside surface which is conductive and has secondary emission properties. Upon the application of a voltage difference between the ends of the tube, current flows through the tube and produces an electric field in an axial direction through the region defined by the tube. Electrons entering the input end of the tube are multiplied through secondary emission before they emerge from the output end of the tube.
The multipliers 10 are constructed with a plurality of bismuth-lead oxide glass tubes of very small inside diameter such as .001 inch. Initially, the glass tubes are placed in a hydrogen reducing furnace to reduce the bismuth and lead oxides. This converts the glass tubes from an insulator to a semi-conductor of relatively high resistance. Then a suflicient number of tubes are stacked in parallel relationship to one another and are fused together such as by heating them in a furnace to the softening point of the glass and allowing them to cool. A relatively small wafer, such as .050 inch, is then sliced from the fused tubes in a direction perpendicular to the axis of the tubes to form the multipliers 10.
A conductive coating 12, such as silver, is applied to the input ends of the multipliers 1G and a similar coating 14 is applied to the output ends to provide connecting terminals. Adjoining the output ends of the multipliers 10 is a base 16 of insulating material, such as glass. Potted in the base 16 are anode wires corresponding in number to the number of multipliers 10, each wire positioned at the output of a particular channel to provide a collecting anode for said channel. As clearly shown in FIG- URE 2, anode wires 18 at the outputs of the channels in column 20 are connected through a common terminal to an ammeter 22 for providing an indication of the signal detected by the anodes 18. Similarly, anode wires 24, 26, 28 and 30 at the outputs of the channels in columns 32, 34, 36 and 38, respectively, are connected through common terminals to ammeters 4-0, 42, 44 and 46 respectively. The ammeters 22, 4d, 42, 44 and 46 have their second terminal grounded.
Direct voltages of suitable magnitude are applied to the elements disclosed above from a direct voltage source (not shown). For example, as shown in FIGURE 2, direct voltages such as 2,000 volts and volts are applied respectively to the coatings 12 and 14. Also direct voltages such as +50 volts are applied to the anodes 13, 24, 26, 28 and 30 from the voltage source.
It should be understood that the ion source 1, the multipliers 10 and the base 16 operate in a vacuum tube at a pressure of approximately 10- mm' Hg. Also, a magnetic field is provided in the vacuum tube to cause the ions to travel in the paths shown in FIGURE 2.
The multipliers 10 are positioned relative to the source 1 to receive the ions emerging from the source. As shown in FIGURE 1, the ions following paths 4, 6 and 8 will enter the channels in columns 20, 34, and 38 respectively. When the ions strike the internal surface of the channels, they will produce secondary emission of electrons which are multiplied through further secondary emission as they pass through the channels. The ion signals from masses M M and M multiplied in this manner are collected by the anode wires 18, 26, and 30 respectively, and the ammeters 22, 42 and 46 will provide an indication of the relative quantities of these different masses.
The discriminator disclosed above has definite advantages. It has extremely high resolution because of the small size of the channels which have a diameter on the order of .001 inch or less. Further, because of the multiplication produced in the channels, it can be very efiectively used to determine the cross section of low intensity particle beams.
Although the description above relates to the detection of an ion beam from a magnetic mass spectrometer, persons skilled in the art will recognize the discriminator can be used for detecting particle beams of all types. For example, it can be used to determine the cross section of beams produced by particle accelerators and of experimental molecular beams. In such cases it may be desirable to have a separate indicator connected to the anode of each channel instead of having a plurality of anodes connected to a common indicator as shown in FIGURE 2. By providing a separate indicator for each channel, excellent analysis can be made of the cross section of a beam.
Although this invention has been disclosed and illustrated with reference to particular applications, the principles involved are susceptible of numerous other applications which will be apparent to persons skilled in the art. The invention is, therefore, to be limited only as indicated by the scope of the appended claims.
Having thus described our invention, We claim:
1. A spatial discriminator for determining the cross section of a particle beam comprising,
an array of channel electron multipliers positioned to receive the beam at its input, each channel receiving a difiierent part of the beam, each channel having a diameter of less than .010 inch,
a separate anode positioned at the output end of each channel to detect the signal produced by the particles entering each channel,
insulating means for supporting the anodes at the outputs of their channels, and
means connected to the anodes to provide an indication of the detected signal.
2. A spatial discriminator for determining the cross section of a particle beam comprising,
an array of channel electron multipliers positioned to receive the beam at its input, different groups of the channels being positioned to receive different portions of the beam, each channel having a diameter of less than .010 inch,
a separate anode positioned at the output end of each channel to detect the signal produced by the particles entering each channel,
a common terminal for connecting the anodes of each diiferent group of channels,
and means connected to each common terminal to provide an indication of the particles in the portion of beam received by the group of channels associated with the common terminal.
References Cited by the Examiner UNITED STATES PATENTS 2,601,097 6/1952 Crawford 250--4l.9 2,674,661 4/1952 Law 313- X 2,851,606 9/1958 Sink et a1. 2504l.9
OTHER REFERENCES Allen: The Detection of Single Positive Ions, Electrons and Photons by a Secondary Electron Multiplier, Physical Review, volume 55, May 15, 1939, pages 966- 971.
RALPH G. NILSON, Primary Examiner.
Claims (1)
1. A SPATIAL DISCRIMINATOR FOR DETERMINING THE CROSS SECTION OF A PARTICLE BEAM COMPRISING, AN ARRAY OF CHANNEL ELECTRON MULTIPLIERS POSITIONED TO RECEIVE THE BEAM AT ITS INPUT, EACH CHANNEL RECEIVING A DIFFERENT PART OF THE BEAM, EACH CHANNEL HAVING A DIAMETER OF LESS THAN .010 INCH, A SEPARATE ANODE POSITIONED AT THE OUTPUT END OF EACH CHANNEL TO DETECT THE SIGNAL PRODUCED BY THE PARTICLES ENTERING EACH CHANNEL, INSULATING MEANS FOR SUPPORTING THE ANODES AT THE OUTPUTS OF THEIR CHANNELS, AND MEANS CONNECTED TO THE ANODES TO PROVIDE AN INDICATION OF THE DETECTED SIGNAL.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US226962A US3240931A (en) | 1962-09-28 | 1962-09-28 | Spatial discriminator for particle beams |
GB37386/63A GB995188A (en) | 1962-09-28 | 1963-09-23 | Spatial discriminator for analyzing the cross-section of particle beams |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US226962A US3240931A (en) | 1962-09-28 | 1962-09-28 | Spatial discriminator for particle beams |
Publications (1)
Publication Number | Publication Date |
---|---|
US3240931A true US3240931A (en) | 1966-03-15 |
Family
ID=22851189
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US226962A Expired - Lifetime US3240931A (en) | 1962-09-28 | 1962-09-28 | Spatial discriminator for particle beams |
Country Status (2)
Country | Link |
---|---|
US (1) | US3240931A (en) |
GB (1) | GB995188A (en) |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3374380A (en) * | 1965-11-10 | 1968-03-19 | Bendix Corp | Apparatus for suppression of ion feedback in electron multipliers |
US3461332A (en) * | 1965-11-26 | 1969-08-12 | Edward E Sheldon | Vacuum tubes with a curved electron image intensifying device |
US3522428A (en) * | 1966-05-17 | 1970-08-04 | Ass Elect Ind | Mass spectrometer having a plurality of relatively movable collectors |
US3612946A (en) * | 1967-08-01 | 1971-10-12 | Murata Manufacturing Co | Electron multiplier device using semiconductor ceramic |
US3676676A (en) * | 1970-10-30 | 1972-07-11 | Bendix Corp | Low energy particle counter with two-dimensional position sensing |
US3946227A (en) * | 1973-04-12 | 1976-03-23 | Associated Electrical Industires Limited | Mass spectrographs and ion collector systems therefor |
US3979621A (en) * | 1969-06-04 | 1976-09-07 | American Optical Corporation | Microchannel plates |
US4126804A (en) * | 1975-10-24 | 1978-11-21 | International Telephone And Telegraph Corporation | Strip microchannel electron multiplier array support structure |
US4829179A (en) * | 1986-07-12 | 1989-05-09 | Nissin Electric Company, Limited | Surface analyzer |
US5017779A (en) * | 1990-04-30 | 1991-05-21 | The United States Of America As Represented By The United States Department Of Energy | Real time Faraday spectrometer |
US5471059A (en) * | 1993-02-12 | 1995-11-28 | Fisons Plc | Multiple-detector system for detecting charged particles |
US5665966A (en) * | 1995-09-29 | 1997-09-09 | Lockheed Martin Idaho Technologies Company | Current measuring system |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2253302A (en) * | 1991-02-05 | 1992-09-02 | Kratos Analytical Ltd | Ion detector |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2601097A (en) * | 1949-07-20 | 1952-06-17 | Arthur R Crawford | Mass spectrometer for simultaneous multiple gas determinations |
US2674661A (en) * | 1948-08-12 | 1954-04-06 | Rca Corp | Electron multiplier device |
US2851606A (en) * | 1955-09-30 | 1958-09-09 | Cons Electrodynamics Corp | Mass spectrometer anticipator circuit |
-
1962
- 1962-09-28 US US226962A patent/US3240931A/en not_active Expired - Lifetime
-
1963
- 1963-09-23 GB GB37386/63A patent/GB995188A/en not_active Expired
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2674661A (en) * | 1948-08-12 | 1954-04-06 | Rca Corp | Electron multiplier device |
US2601097A (en) * | 1949-07-20 | 1952-06-17 | Arthur R Crawford | Mass spectrometer for simultaneous multiple gas determinations |
US2851606A (en) * | 1955-09-30 | 1958-09-09 | Cons Electrodynamics Corp | Mass spectrometer anticipator circuit |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3374380A (en) * | 1965-11-10 | 1968-03-19 | Bendix Corp | Apparatus for suppression of ion feedback in electron multipliers |
US3461332A (en) * | 1965-11-26 | 1969-08-12 | Edward E Sheldon | Vacuum tubes with a curved electron image intensifying device |
US3522428A (en) * | 1966-05-17 | 1970-08-04 | Ass Elect Ind | Mass spectrometer having a plurality of relatively movable collectors |
US3612946A (en) * | 1967-08-01 | 1971-10-12 | Murata Manufacturing Co | Electron multiplier device using semiconductor ceramic |
US3979621A (en) * | 1969-06-04 | 1976-09-07 | American Optical Corporation | Microchannel plates |
US3676676A (en) * | 1970-10-30 | 1972-07-11 | Bendix Corp | Low energy particle counter with two-dimensional position sensing |
US3946227A (en) * | 1973-04-12 | 1976-03-23 | Associated Electrical Industires Limited | Mass spectrographs and ion collector systems therefor |
US4126804A (en) * | 1975-10-24 | 1978-11-21 | International Telephone And Telegraph Corporation | Strip microchannel electron multiplier array support structure |
US4829179A (en) * | 1986-07-12 | 1989-05-09 | Nissin Electric Company, Limited | Surface analyzer |
US5017779A (en) * | 1990-04-30 | 1991-05-21 | The United States Of America As Represented By The United States Department Of Energy | Real time Faraday spectrometer |
US5471059A (en) * | 1993-02-12 | 1995-11-28 | Fisons Plc | Multiple-detector system for detecting charged particles |
US5665966A (en) * | 1995-09-29 | 1997-09-09 | Lockheed Martin Idaho Technologies Company | Current measuring system |
Also Published As
Publication number | Publication date |
---|---|
GB995188A (en) | 1965-06-16 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US3621240A (en) | Apparatus and methods for detecting and identifying trace gases | |
Goulding et al. | Identification of nuclear particles | |
US3240931A (en) | Spatial discriminator for particle beams | |
US3639757A (en) | Apparatus and methods employing ion-molecule reactions in batch analysis of volatile materials | |
Fricke et al. | Single particle counting of heavy ions with a channeltron detector | |
US3209201A (en) | Beam position identification means | |
Girard et al. | Heavy ion timing with channel-plates | |
JPS5917500B2 (en) | Neutral particle detection device | |
US2769911A (en) | Mass spectrometer for analysing substances or indicating a small amount of a determined substance | |
US3808441A (en) | Devices for measuring the dose rate of a beam of ionising radiation | |
US4649279A (en) | Negative ion source | |
Knibbeler et al. | Novel two‐dimensional position‐sensitive detection system | |
US3731096A (en) | High resolution, high etendue, retarding-potential electron concentrator | |
US3774028A (en) | Ion beam intensity measuring apparatus | |
US2944146A (en) | Mass spectrometer | |
US3272984A (en) | Electron multiplier for measuring the flow of positively charged particles | |
US2798162A (en) | Mass spectrometer | |
Burroughs | Collection efficiency of continuous dynode electron multiple arrays | |
US3217161A (en) | Electrode means to electrostatically focus ions separated by a mass spectrometer on a detector | |
Lang et al. | A fast zero-time detector for time-of-flight measurements with heavy ions | |
US4150290A (en) | Focal-surface detector for heavy ions | |
US3435207A (en) | Apparatus for measuring velocity of low energy electrons | |
US4882480A (en) | Apparatus for detecting the position of incidence of particle beams including a microchannel plate having a strip conductor with combed teeth | |
US5777333A (en) | Asymmetric radiation detector system | |
Dietz et al. | Improved zero-time detector for heavy ion time-of-flight spectroscopy |