2010
DOI: 10.1088/0957-0233/22/1/015903
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Calculation of background effects on the VESUVIO eV neutron spectrometer

Abstract: The VESUVIO spectrometer at the ISIS pulsed neutron source measures the momentum distribution ) (p n of atoms by "neutron Compton scattering" (NCS) . Measurements of ) (p n provide a unique window on the quantum behaviour of atomic nuclei in condensed matter systems. The VESUVIO 6 Li doped neutron detectors at forward scattering angles were replaced in Feb 2008 by Yttrium Aluminium Perovskite doped (YAP) γ-ray detectors. These provide a much superior resolution and general performance, but suffer from a sample… Show more

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Cited by 29 publications
(34 citation statements)
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“…The latter eliminates any possible spurious distortion due to inaccurate subtraction of the O, Al contributions. 25 The uncertainty in the determined mean kinetic energy, E K , 11% in the previous measurements, 8 is 2% in the present case. Moreover, the current resolution line shape has a finite variance, allowing us also to carry out non parametric determinations of E K as outlined below.…”
Section: Introductionmentioning
confidence: 49%
See 1 more Smart Citation
“…The latter eliminates any possible spurious distortion due to inaccurate subtraction of the O, Al contributions. 25 The uncertainty in the determined mean kinetic energy, E K , 11% in the previous measurements, 8 is 2% in the present case. Moreover, the current resolution line shape has a finite variance, allowing us also to carry out non parametric determinations of E K as outlined below.…”
Section: Introductionmentioning
confidence: 49%
“…The R l (y, q) functions have been determined using a standard procedure successfully employed for DINS experiments in a variety of systems: 35 the modified DINSMS Monte Carlo code 31 has been used to simulate the scattering of a polycrystalline Pb sample, which is currently used as a resolution calibration standard on VESUVIO. 25 DINS scattering from lead is dominated by the spectrometer's resolution, therefore a comparison between simulated and measured scattering from Pb provides an assessment of the reliability of the code to describe the spectrometer's response. A simulation of DINS scattering spectra in the IA is carried out for a fictitious sample with mass = 1.0079 amu and momentum distribution width σ = 0.001 Å −1 , i.e., assuming a scattering sample with infinitely narrow momentum distribution.…”
Section: B Data Analysismentioning
confidence: 99%
“…As an example of the quality of data for each of the 48 detectors used in the experiment, we report in Fig. 1 the raw time of flight data recorded by a single detector, after gamma background correction [47], together with the evaluation of the multiple scattering contribution, for ice Ih at T = 5 K.…”
Section: Methodsmentioning
confidence: 99%
“…A detailed discussion of this effect is beyond the scope of this paper. Instead, the reader is referred to [103] for an in depth description of this background component and a discussion of how to deal with its effect. As an illustration of how the gamma rays emitted by the cycling foil can distort a DINS FCT signal, figure 32 shows an analytical calculation of the effect of a 20 cm × 20 cm 2 Au cycling foil, moving by 20 cm, for a Pb sample and a sample to detector distance of 55 cm.…”
Section: Residual Backgroundmentioning
confidence: 99%
“…As an illustration of how the gamma rays emitted by the cycling foil can distort a DINS FCT signal, figure 32 shows an analytical calculation of the effect of a 20 cm × 20 cm 2 Au cycling foil, moving by 20 cm, for a Pb sample and a sample to detector distance of 55 cm. The residual background is not easily prevented, but, in most cases, can be removed with a simple data processing algorithm [103].…”
Section: Residual Backgroundmentioning
confidence: 99%