“…Closed cycle or cryogen-free cryo-cooler systems are increasingly popular since their operation is cheaper as no liquid helium is needed and a considerable progress in isolating the sample chamber from the cooler unit vibrations has been achieved. Long et al (1983) have demonstrated that the ideal sample absorber thickness, t ideal , that allows us to obtain the desired results in the shortest time and with the best signal to noise ratio, lies between the reverse of the mass absorption coefficient of the sample and twice this value. The value of t ideal for samples with high electronic absorption when compared with the resonant Mössbauer absorption should be close to the former value.…”
The use of general descriptive names, registered names, trademarks, service marks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use.
“…Closed cycle or cryogen-free cryo-cooler systems are increasingly popular since their operation is cheaper as no liquid helium is needed and a considerable progress in isolating the sample chamber from the cooler unit vibrations has been achieved. Long et al (1983) have demonstrated that the ideal sample absorber thickness, t ideal , that allows us to obtain the desired results in the shortest time and with the best signal to noise ratio, lies between the reverse of the mass absorption coefficient of the sample and twice this value. The value of t ideal for samples with high electronic absorption when compared with the resonant Mössbauer absorption should be close to the former value.…”
The use of general descriptive names, registered names, trademarks, service marks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use.
“…Some use the height [6] or the area [7] of the spectral lines; others use the signal-to-noise ratio ðS=NÞ [8][9][10][11][12]. Some use the height [6] or the area [7] of the spectral lines; others use the signal-to-noise ratio ðS=NÞ [8][9][10][11][12].…”
Section: Estimation Of the Optimal Thicknessmentioning
Abstract. In this course we will give examples for experimental techniques used in particle physics experiments. After a short introduction, we will discuss applications in silicon microstrip detectors, wire chambers, and single photon detection in Ring Imaging Cherenkov (RICH) counters. A short discussion of the relevant physics processes, mainly different forms of energy loss in matter, is enclosed.
“…A useful contribution on the optimization of the absorption thickness for Mossbauer experiments is given by Sarma et al (256), who determined the signal-to-noise ratio as a function of tbe effective thickness for various values of the effective absorption coefficient.…”
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