Ionizing radiation detector system

• US 4,931,653 A
• Filed: 06/16/1988
• Issued: 06/05/1990
• Est. Priority Date: 06/16/1988
• Status: Expired due to Fees

• Current Assignee: George S. Hurst, James E. Turner, Robert N. Hamm, Scott R. Hunter
• Original Assignee: Pellissippi International
• Inventors: Turner, James E., Hamm, Robert N., Hunter, Scott R., Wright, Harvel A., Hurst, George S.
• Primary Examiner(s): Hannaher, Constantine
• Application Number:
  US07/207,723
• Time in Patent Office: 719 Days
• Field of Search: 250/385.1, 250/386, 250/387, 250/363.01, 250/362, 250/361 C, 250/361 R
• US Class Current: 250/385.1
• CPC Class Codes: G01T 1/2935 using ionisation detectors

Abstract

An optical ionizing radiation detector system (10) for determining the three-dimensional spatial distribution of all of the secondary electrons produced by the passage of ionizing radiation through a selected gas is provided. The detector system (10) can be used over a wide range of particle energies and gas pressures. The ionizing radiation passing through the gas produces prompt fluorescence and secondary electrons. A coincidence detector (30) recognizes coincident events of prompt fluorescence in the gas contained within that chamber to initialize the system cycle. At that time, an AC electric field is generated by an R.F. pulse generator (40) to localize the secondary electrons proximate their respective positions of production. Cameras (42) and 42'"'"'), preferably of a digital type, produce an image of the localized electrons to determine their three-dimensional spatial positions. After such positions are determined, a unidirectional electric field is generated by clearing power supply (36) for clearing all charges from the gas chamber.

Claims

1. An ionizing radiation detector system comprising:

a chamber containing a selected fluid;

a source of ionizing radiation which passes ionizing radiation into said fluid to produce thermal electrons;

dynamic electric field generating means for proportional amplification of the number of said thermal electrons and for localizing said thermal electrons proximate their respective positions of production; and

means for measuring the number and spatial distribution of at least one of said localized thermal electrons.

2. The ionizing radiation detector system of claim 1 wherein said means for measuring the spatial distribution of said localized thermal-electrons comprises an optical device.

3. An optical ionizing radiation detector system comprising:

a gas chamber containing a selected gas under pressure;

a source of ionizing radiation which passes ionizing radiation into said gas to produce prompt fluorescence and thermal electrons;

means for detecting prompt fluorescence in said gas chamber for commencing the system cycle;

dynamic electric field generation means for localizing said thermal electrons proximate their respective positions of production;

camera means for producing an image of said localized electrons to determine their number and spatial positions; and

further electric field generation means for clearing all charges from said gas chamber.

4. The system of claim 3 including timer means for controlling the cycle of said system.

5. The system of claim 4 wherein said timer means commences the controlled cycle of said system upon the detection of prompt fluorescence and terminates the cycle of said system when said charges are cleared from said chamber.

6. The system of claim 3 including first and further electrodes positioned at spaced locations within said chamber such that gas is disposed between said electrodes.

7. The system of claim 6 wherein said means for localizing said thermal electrons proximate their position of production comprises a time dependent field generator having an output connected to said first and further of said electrodes such that application of the time dependent field to said electrodes causes said thermal electrons to oscillate about their respective positions of production.

8. The system of claim 3 wherein said camera means comprises first and further cameras positioned such that their directions of viewing gas within said chamber are at separate viewing angles to provide information concerning the location of said secondary electrons, and means for storing and correlating outputs from said cameras concerning spatial positions of said electrons to determine their respective three-dimensional positions within said chamber.

9. The system of claim 3 wherein said cycle commencement means consists of the detection of the coincidental occurrence of a number of prompt fluorescence events within a preselected time interval.

10. An optical ionizing radiation detector system comprising:

a gas chamber containing a selected gas under pressure;

a source of ionizing radiation which passes ionizing radiation into said gas to produce prompt fluorescence and thermal electrons;

means for detecting coincident events of prompt fluorescence in said gas chamber for commencing the system cycle;

electric field generation means for localizing said thermal electrons proximate their respective positions of production;

camera means for producing an image of said localized electrons to determine their number and spatial positions;

further electric field generation means for clearing all charges from said gas chamber;

first and further electrodes positioned at spaced locations within said chamber such that gas is disposed between said electrodes; and

means for localizing said thermal electrons proximate their position of production, comprising an R.F. pulse generator having an output connected to said first and further of said electrodes such that application of an R.F. pulse to said electrodes causes said thermal electrons to oscillate about their respective positions of production.

11. An optical ionizing radiation detector system comprising:

a gas chamber containing a selected gas under pressure;

a source of ionizing radiation which passes ionizing radiation into said gas to produce prompt fluorescence and thermal electrons;

means for detecting coincident events of prompt fluorescence in said gas chamber for commencing the system cycle;

electric field generation means for localizing said thermal electrons proximate their respective positions of production;

camera means for producing an image of said localized electrons to determine their number and spatial positions;

further electric field generation means for clearing all charges from said gas chamber;

camera means comprising first and further cameras positioned such that their directions of viewing gas within said chamber are perpendicular such that each camera images two-dimensional information concerning the location of said secondary electrons; and

means for storing and correlating outputs from said cameras concerning spatial positions of said electrons to determine their respective three-dimensional positions within said chamber.

12. An optical ionizing radiation detector system comprising:

a gas chamber containing a selected gas under pressure;

a source of ionizing radiation which passes ionizing radiation into said gas to produce prompt fluorescence and thermal electrons;

means for detecting coincident events of prompt fluorescence in said gas chamber for commencing the system cycle;

electric field generation means for localizing said thermal electrons proximate their respective positions of production;

camera means for producing an image of said localized electrons to determine their number and spatial positions;

further electric field generation means for clearing all charges from said gas chamber; and

means for detecting coincident events of prompt fluorescence comprising a coincidence detector which detects a plurality of prompt fluorescence events within a preselected time interval representative of the occurrence of a particle track in said gas chamber.