2002
DOI: 10.1007/3-540-45823-9_16
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Neutron Spin Echo Spectrometers of the Next Generation — Where Are the Limits?

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Cited by 3 publications
(5 citation statements)
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“…For each Q the data are normalized by measuring graphite as the resolution sample with equal count statistics like that of the sample. Details of NSE measurement techniques can be found elsewhere. ,, …”
Section: Methodsmentioning
confidence: 99%
“…For each Q the data are normalized by measuring graphite as the resolution sample with equal count statistics like that of the sample. Details of NSE measurement techniques can be found elsewhere. ,, …”
Section: Methodsmentioning
confidence: 99%
“…The emerging shape of the magnetic field somehow resembles a smoothed version of the piecewise combination of the parabolic shapes of equation (11) with the cusp at the tip of the triangle. The degree of cusp smoothing obviously represents the compromise between the zero contribution of the pure parabola shape and the large additional term caused by the naked cusp.…”
Section: Optimum Shapes For Low Inhomogeneity: An Analytic Approachmentioning
confidence: 99%
“…figure 1) are sufficient to correct for all field integral inhomogeneities of an arrangement of ideal cylindrical solenoids [9]. If their axial positions are carefully selected/adjusted in practice two correctors can be sufficient [10,11]. In particular this holds since at the moment the technical ability to realize the correcting current distributions with the required accuracy is limited.…”
Section: Introductionmentioning
confidence: 99%
“…. Q 24 [2]. For a source with a given repetition frequency the intensity gain factor can only be increased by reducing the moderator detector distance, e.g.…”
Section: Tof Wavelength Managementmentioning
confidence: 99%
“…The width of the usable wavelength frame between two pulses Dl # 1=nL D h=m n with h=m n ¼ 395:6 £ 10 29 m 2 =s is inversely proportional to the moderator detector distance L D and the pulse repetition frequency n and independent from the chosen wavelength band. Compared to a sequence of experiments at a continuous source the gain factor is [2] g ¼ ln l max l min =ðD FWHM l=lÞ:…”
Section: Tof Wavelength Managementmentioning
confidence: 99%