Process and device for determining the spatial distribution of electrons emerging from the surface of a radioactive body

• US 5,032,729 A
• Filed: 10/18/1989
• Issued: 07/16/1991
• Est. Priority Date: 10/18/1989
• Status: Expired due to Term

• Current Assignee: Biospace Lab
• Original Assignee: Georges Charpak
• Inventors: Charpak, Georges
• Primary Examiner(s): FIELDS, CAROLYN
• Application Number:
  US07/422,958
• Time in Patent Office: 636 Days
• Field of Search: 250/374, 250/385.1
• US Class Current: 250/385.1
• CPC Class Codes: G01T 1/28 with secondary-emission detectors
• CPC Class Codes: H01J 47/02 Ionisation chambers

Abstract

A device according to the invention includes: a gas detector, comprising at least one chamber (2) and containing a noble gas and a gas or vapor that emits photons between two parallel electrodes (3a, 3b) between which a continuous high voltage (HT) is applied, whereby a first electrode (3a) is intended for receiving, against its external face, the surface of the radioactive body (5,6) to be observed; a brilliance amplifier (13) arranged for receiving the photons emitted by the excited atoms which are produced in the vicinity of a second electrode (3b) by the electron avalanche ascribable to the electrical field between the first and second electrodes; a camera (12) arranged behind the brilliance amplifier; and computing means (15) capable of computing, from the output signal of the camera, the entrance points (9) in said gas detector, at the first electrode, of the electrons emerging from said surface of the radioactive body.

Claims

1. A process for determining the spatial distribution of electrons or β

-rays emerging from a surface of a radioactive body, wherein said surface is placed to actuate a gas detector including at least one chamber with a first electrode and a second electrode and containing, between said first and second electrodes, a noble gas and a gas or vapor that emits photons in response to the impact of electrons, said radioactive body to be observed being placed directly against said first electrode, and wherein the position of the impacts, in the detector, of the electrons originating from said surface is determined by observing the photons, created by an electron avalanche resulting from a multiplication between these electrodes, by means detecting the photons and computing the center of gravity of the distribution of said photons.

2. A process according to claim 1, wherein the surface of the radioactive body placed against said first electrode of the gas detector is coated with an electrically conductive layer that is transparent to the electrons or β

-rays emitted by the radioactive body.

3. A device for determining the spatial distribution of the electrons emerging from a surface of a radioactive body, comprising:

a gas detector including at least one chamber with a pair of parallelly disposed electrodes and containing both a noble gas and a gas or vapor that emits photons between said electrodes, and means for applying a continuous high voltage between said electrodes, whereby a first electrode of said pair comprises means for receiving, against its external face, the surface of the radioactive body to be observed;

a brilliance amplifier arranged for receiving the photons that are emitted by excited atoms which are produced in the vicinity of the other electrode of said pair by electron avalanches resulting from an electrical field between said electrodes produced by said continuous high voltage;

a camera arranged behind the brilliance amplifier; and

computing means capable of computing, in response to an output signal of the camera, entrance points in said gas detector, at the first electrode, of the electrons emerging from said surface of the radioactive body.

4. A device according to claim 3, wherein said gas detector has one single chamber filled with a mixture of noble gas and photon-emitting gas or vapor.

5. A device according to claim 3, wherein said gas detector has two chambers arranged one behind the other, a first one of said two chambers performing a preliminary electron amplification and a second one of said two chambers transforming the electrons originating from the first chamber into a more intense avalanche, said two chambers being filled with the same gas or vapor that emits photons and with a noble gas.

6. A device according to claim 3, wherein said camera is of the CCD-type.

7. A device according to claim 3, wherein said electrodes are constituted by grids.

8. A device according to claim 3, wherein the noble gas is selected from the group consisting of xenon and argon.

9. A device according to claim 3, wherein the gas or vapor that emits photons is selected from the group consisting of triethylamine, tetrakis(dimethylamine)-ethylene, nitrogen and water vapor.

10. A device according to claim 3, wherein said computing means are programmed in order to compute the center of gravity or the maximum of the distribution of photons produced in the detector by an avalanche under the effect of the impact of an electron originating from the radioactive body.

11. A device according to claim 3, wherein said computing means include a memory capable of storing, in the form of digital data, the distribution of photons in various portions of the surface of the radioactive body, the computing means making it possible to recover said distribution by portions of the surface of the radioactive body by using the information contained in electrical signals originating from one of said electrodes.

12. A device according to claim 3, and further comprising a sample holder onto which said radioactive body or sample is placed, said sample holder being provided with spark initiating parts, wherein said parts are covered with a conductive layer set at a voltage intermediate between that of the electrodes.