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High spatial resolution scintigraphic device having collimator with integrated crystals

  • US 6,734,430 B2
  • Filed: 08/13/2001
  • Issued: 05/11/2004
  • Est. Priority Date: 05/23/2001
  • Status: Expired due to Fees
First Claim
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1. A high spatial resolution scintigraphic device having collimator with integrated crystals, comprising in succession from an open end of a container (5) coated with a shielding cladding (6) starting from the source of the event to be measured:

  • a collimator (1) made of a material with high atomic number, internally having a multiplicity of equal conduits (10) of determined length, identified and separated by septa (12) of thickness suited to the photons energy to be detected, terminating in a common end plane (12) on the opposite side from the source of the event to be measured;

    a scintillation crystal structure (2) able to convert the radiation from the source under examination into light radiation;

    at least a photomultiplier (3) of the type with crossed anodes or crossed wires receiving the light radiation emitted by the scintillation crystal structure (2) and generating electrical signals proportional to their intensity and identifying the single event position co-ordinates (X,Y);

    electronic circuits (4, 7, 8) able to execute the amplification and integration of the signals generated by the photomultiplier (3) for the determination of the event position co-ordinates (XY) and the related energy for their subsequent transfer to a conversion device and thence to an personal computer (9) which process them and displays them on a monitor in the form of an image, characterised in that said scintillation crystal structure (2) is constituted by a multiplicity of individual crystals (20) with polygonal section, with base faces (21, 22) and lateral surface (23), each integrally integrate in proximity to the end, oriented towards the photomultiplier (3), of each conduit 10) of the collimator (1), each conduit having a polygonal section corresponding to the polygonal section of each individual crystal, and positioned in such a way that all the base faces (21) of the crystals (20) oriented towards the photomultiplier (3) lie in a same plane parallel to said common end plane (12) of the collimator (1).

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