Determination of detecting system response function
Fourier-transform and generalised least-squares (GLS) methods have been used to determine the detecting system response function b( E) from the deconvolution equation: b(E) = u(E) ∗ ∗i(E), where u(E) is the measured spectrum and i( E) is the initial spectrum. In order to obtain a physical and unique...
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| Published in | Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Vol. 254; no. 3; pp. 611 - 615 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
Elsevier B.V
01.03.1987
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| Online Access | Get full text |
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| Summary: | Fourier-transform and generalised least-squares (GLS) methods have been used to determine the detecting system response function
b(
E) from the deconvolution equation:
b(E) = u(E)
∗
∗i(E),
where u(E)
is the measured spectrum and
i(
E) is the initial spectrum. In order to obtain a physical and unique solution of
b(
E), a minimization procedure min
f|u(E) − i(E) ∗ b(E)|
2
with a regularization parameter f has been involved. |
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| ISSN: | 0168-9002 1872-9576 |
| DOI: | 10.1016/0168-9002(87)90037-4 |