US2005092928A1PendingUtilityA1

Bidimensional detector of ionizing radiation and manufacturing process for this detector

Assignee: COMMISSARIAT ENERGIE ATOMIQUEPriority: Feb 24, 1999Filed: Nov 17, 2004Published: May 5, 2005
Est. expiryFeb 24, 2019(expired)· nominal 20-yr term from priority
G01T 1/2935G01T 1/185
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Claims

Abstract

Bidimensional detector of ionizing radiation and manufacturing process for the detector. The detector includes a block created from a material which releases secondary particles by interaction with incident ionizing radiation with an energy level greater than or equal to 100 keV. The thickness of the block is at least equal to one-tenth of the mean free path traveled by the incident ionizing radiation particles in the material. Parallel slits run through the block and the slits are filled with a fluid configured to interact with the secondary particles to produce other particles representing the radiation. The block, and then the slits, are formed, for example, by waterjet cutting, electrical discharge machining, or roll-out stretch wire. The bidimensional detector can be used, for example, for radiographic purposes.

Claims

exact text as granted — not AI-modified
1 . Detector for incident ionizing radiation comprising primary particles whose energies are greater than or equal to 100 keV, the detector including: 
 a block of converting material configured to release secondary particles by interaction with the incident ionizing radiation, wherein a thickness of the block is at least equal to one-tenth of a mean free path traveled by the incident ionizing radiation through the converting material; and    parallel slits crossing the block, the slits filled with a fluid configured to interact with the secondary particles to produce tertiary particles indicative in intensity and position of the incident ionizing radiation,    wherein the block is positioned to ensure that the incident ionizing radiation comes in on a first block face where the slits terminate, wherein a first dimension of a cross-section of each of the parallel slits measured in a plane parallel to the first block face is greater than a second dimension of the cross-section of each of the parallel slits measured in the plane parallel to the first block face, and    wherein the first dimension of the cross-section of each of the parallel slits are parallel in the plane parallel to the first block face.    
   
   
       2 . Detector as described in  claim 1 , wherein the slits are perpendicular to the first face of the block.  
   
   
       3 . Detector as described in  claim 1 , wherein slit planes form an angle of between 1° and 5° with a line perpendicular to the first face of the block.  
   
   
       4 . Detector as described in  claim 1 , wherein the fluid is configured to be ionized by the secondary particles, thereby producing electrons as the tertiary particles, and the detector further includes means for creating an electric field for extracting the tertiary particles from the block.  
   
   
       5 . Detector as described in  claim 4 , wherein the fluid is a gas.  
   
   
       6 . Detector as described in  claim 4 , further comprising means for analyzing the electrons extracted from the block.  
   
   
       7 . Detector as described in  claim 6 , wherein the means for analyzing includes an avalanche gas amplifier for producing electron avalanches from the electrons extracted from the block.  
   
   
       8 . Detector as described in  claim 7 , wherein the fluid is a gas and is configured to convert the electron avalanches into visible or ultraviolet radiation, and the means for analyzing further includes means for detecting the visible or ultraviolet radiation.  
   
   
       9 . Detector as described in  claim 8 , wherein the means for detecting the visible or ultraviolet radiation includes a camera capable of detecting the visible or ultraviolet radiation, or a matrix of amorphous silicon photodiodes placed against the avalanche gas amplifier.  
   
   
       10 . Detector as described in  claim 4 , wherein the converting material is an electrical conductor and the block is formed from stacked layers of the converting material, wherein the stacked layers alternate with electrically insulating layers and the stacked layers begin with a conducting layer of the converting material on the first face of the block and end with a conducting layer of the converting material on a second face of the block, which is opposite the first face and on which the slits terminate, and the detector further includes means for applying electric voltages to the stacked layers, with electric voltages increasing from the first face to the second face, thereby creating said electric field.  
   
   
       11 . Detector as described in  claim 10 , further including a supplementary layer formed on an additional electrically insulating layer, the additional electrically insulating layer being formed on the last layer of the converting material, located at the second face of the block, wherein the supplementary layer is made of an electrically conducting material configured to absorb the secondary particles created in the last layer, and the supplementary and additional layers have slits running through them.  
   
   
       12 . Detector manufactured according to  claim 10 , wherein the layer of the converting material located at the second face of the block is blackened out to prevent parasitic light reflections.  
   
   
       13 . Detector manufactured according to  claim 4 , wherein the converting material is electrically insulating, or highly resistive, and the block is formed from stacked layers of the converting material or is made from the converting material in a bulk state, wherein the block further includes first and second layers or grids which are electrically conducting and formed, respectively, on the first block face and on a second block face which is located opposite the first block face and on which the slits terminate, and the electric field is created by raising the first layer or grid to a first voltage and the second layer or grid to a second voltage which is greater than the first voltage.  
   
   
       14 . Detector as described in  claim 1 , wherein the block is made from a stack of strips made from an insulating or highly resistive converting material, and the strips are separated from each other by spacers which define the parallel slits of the block, wherein the block further includes first and second layers or grids which are electrically conducting and formed respectively, on the first block face and on a second block face which is located opposite the first face and on which the slits terminate, and the electric field is created by raising the first layer or grid to a first electric voltage and the second layer or grid to a second electric voltage which is greater than the first voltage.  
   
   
       15 . Manufacturing process for the detector of  claim 1 , wherein the block is firstly manufactured and then the slits are manufactured by one of the following techniques: 
 waterjet cutting,    electrical discharge machining,    roll-out stretch wire.    
   
   
       16 . Manufacturing process as described in  claim 15 , wherein the fluid is configured to be ionized by the secondary particles, thereby producing electrons as the tertiary particles, and the detector further includes means for creating an electric field for extracting the tertiary particles from the block, wherein the converting material is an electrical conductor and the block is formed from stacked layers of the converting material, wherein the stacked layers alternate with electrically insulating layers and the stacked layers begin with a conducting layer of the converting material on the first face of the block and end with a conducting layer of the converting material on a second face of the block, which is opposite the first face and on which the slits terminate, and the detector further includes means for applying electric voltages to the stacked layers, with electric voltages increasing from the first face to the second face, thereby creating said electric field, 
 wherein the layers are stuck to each other.    
   
   
       17 . Manufacturing process as described in  claim 15 , wherein, before creating each slit, a guide hole is made in the block which is then used to create the slit.  
   
   
       18 . Manufacturing process as described in  claim 15 , wherein the fluid is configured to be ionized by the secondary particles, thereby producing electrons as the tertiary particles, and the detector further includes means for creating an electric field for extracting the tertiary particles from the block, wherein the converting material is electrically insulating, or highly resistive, and the block is formed from stacked layers of the converting material or is made from the converting material in a bulk state, wherein the block further includes first and second layers or grids which are electrically conducting and formed, respectively, on the first block face and on a second block face which is located opposite the first block face and on which the slits terminate, and the electric field is created by raising the first layer or grid to a first voltage and the second layer or grid to a second voltage which is greater than the first voltage, 
 wherein the layers are stuck to each other.    
   
   
       19 . Detector for incident ionizing radiation comprising primary particles whose energies are greater than or equal to 100 keV, the detector including: 
 a block of converting material configured to release secondary particles by interaction with the incident ionizing radiation, wherein a thickness of the block is at least equal to one-tenth of a mean free path traveled by the incident ionizing radiation through the converting material; and    parallel holes crossing the block, the holes filled with a fluid configured to interact with the secondary particles to produce tertiary particles indicative in intensity and position of the incident ionizing radiation,    wherein the block is positioned to ensure that the incident ionizing radiation comes in on a first block face where the holes terminate,    wherein a first dimension of a cross-section of each of the parallel holes measured in a plane parallel to the first block face is greater than a second dimension of the cross-section of each of the parallel holes measured in the plane parallel to the first block face, and    wherein the first dimension of the cross-section of each of the parallel holes are parallel in the plane parallel to the first block face.

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