US3197663A - Electron multiplier gate - Google Patents

Electron multiplier gate Download PDF

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Publication number
US3197663A
US3197663A US199798A US19979862A US3197663A US 3197663 A US3197663 A US 3197663A US 199798 A US199798 A US 199798A US 19979862 A US19979862 A US 19979862A US 3197663 A US3197663 A US 3197663A
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United States
Prior art keywords
channel
electrons
channels
output
electron multiplier
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Expired - Lifetime
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US199798A
Inventor
Norman James
Jr Hayden Smith
Robert R Thompson
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Bendix Corp
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Bendix Corp
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Publication date
Priority to NL132564D priority Critical patent/NL132564C/xx
Priority to NL293495D priority patent/NL293495A/xx
Application filed by Bendix Corp filed Critical Bendix Corp
Priority to US199798A priority patent/US3197663A/en
Priority to GB21737/63A priority patent/GB981659A/en
Priority to FR936898A priority patent/FR1358238A/en
Application granted granted Critical
Publication of US3197663A publication Critical patent/US3197663A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J43/00Secondary-emission tubes; Electron-multiplier tubes
    • H01J43/04Electron multipliers
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K17/00Electronic switching or gating, i.e. not by contact-making and –breaking
    • H03K17/51Electronic switching or gating, i.e. not by contact-making and –breaking characterised by the components used
    • H03K17/88By the use, as active elements, of beam-deflection tubes

Definitions

  • This invention relates to gating apparatus for channel electron multipliers.
  • a first channel electron multiplier which is to be gated has positioned at its output second and third channel electron multipliers which comprise the gating apparatus.
  • the electrons emerging from the first channel are gated into the second or third channel, depending upon the voltage applied to the inputs of these channels.
  • An object of this invention is to provide gating apparatus for the output of an electron multiplier.
  • Another object'is to provide gating apparatus comprising a pair of channel electron multipliers positioned at the output of an electron multiplier to gate the output through one channel or the other upon application of a suitable voltage to the input of the appropriate channel.
  • FIGURE 1 is a perspective view, partly broken away, illustrating an embodiment of this invention.
  • FIGURE 2 is a schematic diagram partly in block form and partly in cross section, illustrating the embodiment in FIGURE 1 and showing the associated electrical circuitry.
  • FIGURE 3 is another schematic diagram similar to FIGURE 2 which shows the path followed by electrons when certain electrical conditions exist.
  • a channel electron multiplier is posi tioned to receive particles, such as ions or electrons, from a source (not shown).
  • the channel 10 may receive ions from a time-offlight mass spectrometer of the type disclosed in US. Patent No. 2,685,035, issued to William C. Wiley and these ions would produce secondary emission of electrons upon striking the inside surface of the channel 10.
  • gating apparatus Positioned at the output of the channel 10 is gating apparatus generally indicated at 11 which includes a pair of channel electron multipliers 12 and 14.
  • the channels 12 and 14 are positioned to receive electrons emerging from the channel 10 and form a Y arrangement with the channel 10.
  • Anodes 16 and 18 are disposed respectively at the output ends of the channels 12 and 14 to collect electrons passing through the channels.
  • An insulator 20 provides insulation between the channels 12 and 14.
  • Direct voltages of suitable magnitude are applied to the elements disclosed above from a direct voltage source 3,197,663 Patented July 27, 1965 ice (not shown).
  • a direct voltage source 3,197,663 Patented July 27, 1965 ice (not shown).
  • direct voltages of 2,000 volts, 0 volts, '100 volts, +2,000 volts, and +2,100 volts may be applied respectively, to the input of the channel 10, the output of the channel 10, the inputs of the channels 12 and 14, the outputs of the. channels 12 and 14 and the anodes 16 and 13.
  • the inputs of the channels 12 and 14 at l00 volts are normally maintained at a negative potential with respect to the output of the channel 10 at 0 volts.
  • a pulse source 22 is connected to the inputs of the channels 12 and 14 through resistances 24 and 26 respectively.
  • the pulse source 22 is adapted to provide an input pulse, such as +200 volts, to either the channel 12 or the channel 14 to raise the input of the channel to a positive potential volt-s) with respect to the output of the channel 10 during application of the pulse.
  • a detector such as an oscilloscope 28, is connected to the anodes 16 and 18 through resistances 30 and 32, respectively, to detect the electrons striking the anodes.
  • channels 10, 12 and 14, and the anodes 16 and 18 operate in' a vacuum tube at a pressure of approximately 10* mm. Hg.
  • a positive voltage pulse is applied to the input of the appropriate channel from the pulse source 22. If the pulse is applied to channel 12, the electrons emerging from the channel 10 are permitted to enter the channel 12 where they successively strike the surface of the channel and are further multiplied before they impinge upon the anode 16. The path followed by the electrons is shown by the path 50 in FIGURE 3. The electrons striking anode 16 are indicated on the oscilloscope 28. The electrons would follow a similar path through the channel 14 if the pulse is applied to that channel. Thus, by applying a positive pulse to the channel 12 or to the channel 14, gating action results to direct the electrons at the output of the channel 10 through either the channel 12 or the channel 14.
  • the above gating apparatus would be particularly useful in connection with the time-of-flight mass spectrometer such as disclosed in the aforesaid US. Patent No. 2,685,- 035.
  • ions of different mass would arrive at the-input of the channel 10 at dilferent time-s. Accordingly, the electrons produced through secondary emission by the ions of different mass would also arrive at the output of the channel 10 at correspondingly different times.
  • the channel 12 may be pulsed to gate'the electrons through the channel for collection by the anode 16 and detection by the oscilloscope 28.
  • electrons produced by ions of a different mass would be gated through channel 14 upon the application of a pulse to that channel at the proper time.
  • channels (12 and 14) Although only two channels (12 and 14) have been used in describing this invention, it will be recognized that additional channels can be provided at the output of the channel 10 and the electrons gated through the one to which a pulse is applied. If desired, the electrons could be gated through more than one channel by applying pulses simultaneously to the inputs of .two or more channels.
  • a gate for a first channel electron multiplier comprising a plurality of channel electron multipliers positioned relative to the output of the first channel to receive electrons emerging from the first channel
  • a gate for a firstrchannel electron multiplier comprising a plurality of channel electron multipliers having their input-s positioned relative to the output of the first channel to receive electrons emerging from the first channel,
  • a gate for a first channel electron multiplier comprising second and third channel electron multipliers having their inputs positioned relative to the output of the first channel to receive electrons emerging from th first channel, 7
  • a gate for a first channel electron multiplier comprising a plurality of multiplier units positioned relative to the output of the first channel to receive electrons emerging from the first channel,
  • each multiplier unit including a channelelectron multiplier and collecting means positioned at the output of the channel

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  • Electron Tubes For Measurement (AREA)

Description

July 27, 1965 J. NORMAN ETAL 3,197,653
ELECTRON MULTIPLIER GATE Filed June 4, 1962 2 Sheets-Sheet 1 INPUT INVENTOR. JAMES NORMAN HAYDEN SMITH BY ROBERT THOMPSON AT RNEY y 27, 1955 J. NORMAN ETAL 3, 97,663
ELECTRON MULTIPLIER GATE Filed June 4, 1962 2 Sheets-Sheet PULSE SOURCE +2|oo v 30 -2ooo v OSC|LLO INPUT SCOPE INVENTOR. JAMES NORMAN HAYDEN SMITH BY ROBERT R.THOMPSON United States Patent 3,197,663 ELECTRON MULTIPLIER GATE Harries Norman, Blacksburg, Va., and Hayden Smith, In, Whitmore Lake, and Robert R. Thompson, Livonia, Mich, assignors to The Bendix Corporation, Southfield, Mich, a corporation of Delaware Filed June 4, 1962, Ser. No. 199,798 4 Claims. (Cl. 313103) This invention relates to a gate for an electron multiplier and more particularly to a gate for a channel electron multiplier.
In copending patent application U.S. Serial No. 23,574, filed April 20, 1960, by George W. Goodrich and W. C. Wiley, now Patent No. 3,128,408, there is fully'disclosed a tube type channel electron multiplier. In this type multiplier, the inside surface of the tube is conductive and has secondary emissive 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. 1 a
This invention relates to gating apparatus for channel electron multipliers. In accordance with the invention, a first channel electron multiplier which is to be gated has positioned at its output second and third channel electron multipliers which comprise the gating apparatus. The electrons emerging from the first channel are gated into the second or third channel, depending upon the voltage applied to the inputs of these channels.
An object of this invention is to provide gating apparatus for the output of an electron multiplier.
Another object'is to provide gating apparatus comprising a pair of channel electron multipliers positioned at the output of an electron multiplier to gate the output through one channel or the other upon application of a suitable voltage to the input of the appropriate channel.
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 perspective view, partly broken away, illustrating an embodiment of this invention.
'FIGURE 2 is a schematic diagram partly in block form and partly in cross section, illustrating the embodiment in FIGURE 1 and showing the associated electrical circuitry.
FIGURE 3 is another schematic diagram similar to FIGURE 2 which shows the path followed by electrons when certain electrical conditions exist.
In FIGURE 1, a channel electron multiplier is posi tioned to receive particles, such as ions or electrons, from a source (not shown). For example, the channel 10 may receive ions from a time-offlight mass spectrometer of the type disclosed in US. Patent No. 2,685,035, issued to William C. Wiley and these ions would produce secondary emission of electrons upon striking the inside surface of the channel 10. Positioned at the output of the channel 10 is gating apparatus generally indicated at 11 which includes a pair of channel electron multipliers 12 and 14. The channels 12 and 14 are positioned to receive electrons emerging from the channel 10 and form a Y arrangement with the channel 10. Anodes 16 and 18 are disposed respectively at the output ends of the channels 12 and 14 to collect electrons passing through the channels. An insulator 20 provides insulation between the channels 12 and 14.
Direct voltages of suitable magnitude are applied to the elements disclosed above from a direct voltage source 3,197,663 Patented July 27, 1965 ice (not shown). For example, as shown in FIGURE 2, direct voltages of 2,000 volts, 0 volts, '100 volts, +2,000 volts, and +2,100 volts may be applied respectively, to the input of the channel 10, the output of the channel 10, the inputs of the channels 12 and 14, the outputs of the. channels 12 and 14 and the anodes 16 and 13. The inputs of the channels 12 and 14 at l00 volts, are normally maintained at a negative potential with respect to the output of the channel 10 at 0 volts.
A pulse source 22 is connected to the inputs of the channels 12 and 14 through resistances 24 and 26 respectively. The pulse source 22 is adapted to provide an input pulse, such as +200 volts, to either the channel 12 or the channel 14 to raise the input of the channel to a positive potential volt-s) with respect to the output of the channel 10 during application of the pulse. A detector, such as an oscilloscope 28, is connected to the anodes 16 and 18 through resistances 30 and 32, respectively, to detect the electrons striking the anodes.
It should be understood that the channels 10, 12 and 14, and the anodes 16 and 18 operate in' a vacuum tube at a pressure of approximately 10* mm. Hg.
When electrons are introduced to the input end of the multiplier 10, they successively strike the surface of the channel 10 as shown by the path 40 in FIGURE 2 and are multiplied through secondary emission. Since the inputs of channels 12 and 14 are normally maintained at a negative potential with respect to the output of the channel 10, the electrons passing through the channel 10 cannot enter the channels 12 or 14. The electrons reach the end of the channel 10 are eventually \lost to the inner surface of the channel.
When it is desired to gate the electrons through the channel 12 or the channel 14, a positive voltage pulse is applied to the input of the appropriate channel from the pulse source 22. If the pulse is applied to channel 12, the electrons emerging from the channel 10 are permitted to enter the channel 12 where they successively strike the surface of the channel and are further multiplied before they impinge upon the anode 16. The path followed by the electrons is shown by the path 50 in FIGURE 3. The electrons striking anode 16 are indicated on the oscilloscope 28. The electrons would follow a similar path through the channel 14 if the pulse is applied to that channel. Thus, by applying a positive pulse to the channel 12 or to the channel 14, gating action results to direct the electrons at the output of the channel 10 through either the channel 12 or the channel 14.
The above gating apparatus would be particularly useful in connection with the time-of-flight mass spectrometer such as disclosed in the aforesaid US. Patent No. 2,685,- 035. From the mass spectrometer, ions of different mass would arrive at the-input of the channel 10 at dilferent time-s. Accordingly, the electrons produced through secondary emission by the ions of different mass would also arrive at the output of the channel 10 at correspondingly different times. At the times that electrons produced by the ions of a particular mass are expected at the output of the channel, the channel 12 may be pulsed to gate'the electrons through the channel for collection by the anode 16 and detection by the oscilloscope 28. Similarly, electrons produced by ions of a different mass would be gated through channel 14 upon the application of a pulse to that channel at the proper time.
Although only two channels (12 and 14) have been used in describing this invention, it will be recognized that additional channels can be provided at the output of the channel 10 and the electrons gated through the one to which a pulse is applied. If desired, the electrons could be gated through more than one channel by applying pulses simultaneously to the inputs of .two or more channels.
anevgeea 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 ourinvention, we claim:
1. A gate for a first channel electron multiplier comprising a plurality of channel electron multipliers positioned relative to the output of the first channel to receive electrons emerging from the first channel,
and means. for changing'the potential of at least one of the channels in the plurality to cause'the electrons emerging from, the first channel to enter only said channel in the plurality.
2. A gate for a firstrchannel electron multiplier comprising a plurality of channel electron multipliers having their input-s positioned relative to the output of the first channel to receive electrons emerging from the first channel,
means for applyingbiasing'voltages to the inputs of each of the plurality ofchannels to prevent the entrance of electrons emerging from the first channel, and means for applyinga-voltage pulse to'at least one of the inputs of the plurality of channels to cause the electrons emerging from the first channel to enter the pulsed: channel during application of the pulse.
3 A gate for a first channel electron multiplier comprising second and third channel electron multipliers having their inputs positioned relative to the output of the first channel to receive electrons emerging from th first channel, 7
means for applying a biasing voltage to the inputs of the second and third channels to prevent the entrance of electrons emerging from the first channel,
and means for applying a voltage pulse to the input of the second or third channel to cause the electrons emerging from the first channel to enter the pulsed channel during application of the pulse.
4. A gate for a first channel electron multiplier comprising a plurality of multiplier units positioned relative to the output of the first channel to receive electrons emerging from the first channel,
each multiplier unit including a channelelectron multiplier and collecting means positioned at the output of the channel,
and means for changing the potential of at least one of the multiplier units in the plurality to cause the electrons emerging from'the first channel to enter only the channel in said-onemultiplier unit and to reach the collecting means positioned at its output.
References Gited by i the Examiner UNITED STATES PATENTS 2,826,704 3/58 Wiley 313-405 FOREIGN PATENTS 814,134 5/59 Great Brita-in.
DAVID J. GALVIN, Primary Examiner.

Claims (1)

  1. 2. A GATE FOR A FIRST CHANNEL ELECTRON MULTIPLIER COMPRISING A PLURALITY OF CHANNEL ELECTRON MULTIPLIERS HAVING THEIR INPUTS POSITIONED RELATIVE OT THE OUTPUT OF THE FIRST CHANNEL TO RECEIVE ELECTRONS EMERGING FROM THE FIRST CHANNEL, MEANS FOR APPLYING BIASING VOLTAGES TO THE INPUTS OF EACH OF THE PLURALITY OF CHANNELS TO PREVENT THE ENTRANCE OF ELECTRONS EMERGING FROM THE FIRST CHANNEL, AND MEANS FOR APPLYING A VOLTAGE PULSE TO AT LEAST ONE OF THE INPUTS OF THE PLURALITY OF CHANNELS TO CAUSE THE ELECTRONS EMERGING FROM THE FIRST CHANNEL TO ENTER THE PULSED CHANNEL DURING APPLICATION OF THE PULSE.
US199798A 1962-06-04 1962-06-04 Electron multiplier gate Expired - Lifetime US3197663A (en)

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Application Number Priority Date Filing Date Title
NL132564D NL132564C (en) 1962-06-04
NL293495D NL293495A (en) 1962-06-04
US199798A US3197663A (en) 1962-06-04 1962-06-04 Electron multiplier gate
GB21737/63A GB981659A (en) 1962-06-04 1963-05-30 Electron multiplier gate
FR936898A FR1358238A (en) 1962-06-04 1963-06-04 Particle multiplier equipped with a switching device

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Cited By (5)

* Cited by examiner, † Cited by third party
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
US5086248A (en) * 1989-08-18 1992-02-04 Galileo Electro-Optics Corporation Microchannel electron multipliers
US5367218A (en) * 1991-05-21 1994-11-22 Commissariat A L'energie Atomique Ceramic electron multiplying structure, particularly for a photomultiplier and its production process
US20040183028A1 (en) * 2003-03-19 2004-09-23 Bruce Laprade Conductive tube for use as a reflectron lens
US20100090098A1 (en) * 2006-03-10 2010-04-15 Laprade Bruce N Resistive glass structures used to shape electric fields in analytical instruments

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7687978B2 (en) 2006-02-27 2010-03-30 Itt Manufacturing Enterprises, Inc. Tandem continuous channel electron multiplier

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2826704A (en) * 1955-01-03 1958-03-11 Bendix Aviat Corp Magnetic electron multiplier gate
GB814134A (en) * 1955-02-28 1959-05-27 Bendix Aviat Corp Magnetic electron multiplier

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2826704A (en) * 1955-01-03 1958-03-11 Bendix Aviat Corp Magnetic electron multiplier gate
GB814134A (en) * 1955-02-28 1959-05-27 Bendix Aviat Corp Magnetic electron multiplier

Cited By (7)

* Cited by examiner, † Cited by third party
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
US5086248A (en) * 1989-08-18 1992-02-04 Galileo Electro-Optics Corporation Microchannel electron multipliers
US5367218A (en) * 1991-05-21 1994-11-22 Commissariat A L'energie Atomique Ceramic electron multiplying structure, particularly for a photomultiplier and its production process
US20040183028A1 (en) * 2003-03-19 2004-09-23 Bruce Laprade Conductive tube for use as a reflectron lens
US7154086B2 (en) 2003-03-19 2006-12-26 Burle Technologies, Inc. Conductive tube for use as a reflectron lens
US20100090098A1 (en) * 2006-03-10 2010-04-15 Laprade Bruce N Resistive glass structures used to shape electric fields in analytical instruments
US8084732B2 (en) 2006-03-10 2011-12-27 Burle Technologies, Inc. Resistive glass structures used to shape electric fields in analytical instruments

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