1.
    发明专利
    未知

    公开(公告)号:DE60122713T2

    公开(公告)日:2007-09-20

    申请号:DE60122713

    申请日:2001-03-26

    Abstract: A method of identifying radiation detected in a wall-less proportional gas counter providing a stable pulse height spectrum. The method comprises i) transforming the detected pulse height spectrum (dn/dx) in accordance with the transform u=x 1/2 where x represents the energy of the detected pulses in the original pulse height spectrum; ii) generating a normalized spectrum in u-space comprising a representation of dn/du as a function of u, where n is the detected pulse count as a function of x; iii) deconvoluting the normalized spectrum in u-space to enhance the spectrum; and iv) determining from the enhanced spectrum the energy (or energies) and/or the intensity (or intensities) of the detected radiation.

    2.
    发明专利
    未知

    公开(公告)号:DE60122713D1

    公开(公告)日:2006-10-12

    申请号:DE60122713

    申请日:2001-03-26

    Abstract: A method of identifying radiation detected in a wall-less proportional gas counter providing a stable pulse height spectrum. The method comprises i) transforming the detected pulse height spectrum (dn/dx) in accordance with the transform u=x 1/2 where x represents the energy of the detected pulses in the original pulse height spectrum; ii) generating a normalized spectrum in u-space comprising a representation of dn/du as a function of u, where n is the detected pulse count as a function of x; iii) deconvoluting the normalized spectrum in u-space to enhance the spectrum; and iv) determining from the enhanced spectrum the energy (or energies) and/or the intensity (or intensities) of the detected radiation.

    3.
    发明专利
    未知

    公开(公告)号:AT338283T

    公开(公告)日:2006-09-15

    申请号:AT01915484

    申请日:2001-03-26

    Abstract: A method of identifying radiation detected in a wall-less proportional gas counter providing a stable pulse height spectrum. The method comprises i) transforming the detected pulse height spectrum (dn/dx) in accordance with the transform u=x 1/2 where x represents the energy of the detected pulses in the original pulse height spectrum; ii) generating a normalized spectrum in u-space comprising a representation of dn/du as a function of u, where n is the detected pulse count as a function of x; iii) deconvoluting the normalized spectrum in u-space to enhance the spectrum; and iv) determining from the enhanced spectrum the energy (or energies) and/or the intensity (or intensities) of the detected radiation.

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