Detector and method for detection of ionizing radiation
AssigneeXCounter AB
InventorTom Francke
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AssigneeXCounter AB
InventorTom Francke
Estimating the term…
A detector for detection of ionizing radiation comprises a chamber (13) filled with an ionizable gas, and including a first (17, 19) and a second (21) electrode arrangement between which a first voltage (U1, U2) is applicable, a radiation entrance (33) arranged such that radiation (1) can enter the chamber between and substantially in parallel with the first and second electrode arrangements, for ionization of the ionizable gas, an electron avalanche amplification arrangement (15) including an avalanche cathode arrangement (25) and an avalanche anode arrangement (27), between which a second voltage (Ua) is applicable, and a read-out arrangement (29), wherein the first voltage is applicable for drifting electrons created during ionization towards the electron avalanche amplification arrangement, the second voltage is applicable for avalanche amplification of said electrons, and the read-out arrangement is arranged for detection of the electron avalanches and/or correspondingly produced ions. The invention comprises that the chamber is arranged such that radiation entering through the radiation entrance will firstly enter a first chamber section having a first distance (d1) between the first and second electrode arrangements and then enter a second chamber section having a second distance (d2) between the first and second electrode arrangements, the first (d1) and second (d2) distances being substantially different, and that the read-out arrangement is arranged such that electron avalanches, and/or correspondingly produced ions, derivable mainly from ionization in the respective chamber section are separately detectable.
A detector for detection of ionizing radiation, comprising:
A method for detection of ionizing radiation in a detector comprising a chamber filled with an ionizable gas, and including a first and a second electrode arrangement, substantially in parallel with each other, a radiation entrance, an electron avalanche amplification arrangement including an avalanche cathode arrangement and an avalanche anode arrangement, and a read-out arrangement, said method comprising:
A detector for detection of ionizing radiation comprising:
A method for detection of ionizing radiation in a detector comprising a chamber filled with an ionizable substance, and including a first and a second electrode arrangement, substantially in parallel with each other, a radiation entrance, an electron avalanche amplification arrangement, and a read-out arrangement, said method comprising:
Dependencies are inferred from the claim text.
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Tubes for determining the presence, intensity, density or energy of radiation or particles: ionisation chambers
Measuring radiation intensity: with ionisation chamber arrangements
Electric discharge tubes or discharge lamps
Measurement of nuclear or x-radiation
Term ended 14 Apr 2020 (estimated)
USPTO file history isn’t available for this patent, so only indexed dates are shown.
The present invention generally relates to the detection of ionizing radiation, and particularly to the detection of X-rays.
More specifically, the invention relates to a detector for detection of ionizing radiation, to a device for use in planar beam radiography, and to a method for detection of ionizing radiation.
Gaseous detectors, in general, are very attractive at photon energies lower than approximately 10 keV. The main advantages of gaseous detectors are that they are cheap to manufacture compared to solid state detectors, and that they can employ gas multiplication to strongly (on orders of magnitude) amplify the signal amplitudes. However, at energies exceeding 10 keV the gaseous detectors are less attractive as the stopping power of the gas decreases rapidly with increased photon energy. This results in a heavily deteriorated spatial resolution due to extended tracks of so-called long-range electrons, which are created as a result of the X-ray absorption.
The present invention will become more fully understood from the detailed description of embodiments of the present invention given hereinbelow and the accompanying FIGS. 1-7, which are given by way of illustration only, and thus are not limitative of the invention.
FIG. 1 illustrates schematically, in a cross sectional view, a device for planar beam radiography, according to an embodiment of the invention.
FIG. 2 is a diagram showing the mean free path of X-rays due to absorption in argon, krypton, and xenon, respectively, as a function of X-ray energy at standard temperature and pressure (STP).
In the following description, for purposes of explanation and not limitation, specific details are set fourth, such as particular techniques and applications in order to provide a thorough understanding of the present invention. However, it will be apparent to one skilled in the art that the present invention may be practiced in other embodiments that depart from these specific details. In other instances, detailed descriptions of well-known methods and apparatuses are omitted so as not to obscure the description of the present invention with unnecessary details.
FIG. 1 is a sectional view in a plane orthogonal to the plane of a planar X-ray beam 1 of a device for planar beam radiography, according to an embodiment of the present invention. The device includes an X-ray source 3, which together with a first thin collimator window 5 produces the planar fan-shaped X-ray beam 1, for irradiation of an object 7 to be imaged. The first thin collimator window 5 can be replaced by other means for forming an essentially planar X-ray beam, such as an X-ray diffraction mirror or an X-ray lens etc.
The beam transmitted through the object 7 enters a detector 9. Optionally a thin slit or second collimator window 11, which is aligned with the X-ray beam, forms the entrance for the X-ray beam 1 to the detector 9.