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Time of flight, neutron scattering

Count-rates in time of flight neutron scattering experiments... [Pg.447]

Further information on time-of-flight neutron diffraction (and other time-of-flight neutron scattering methods) can be obtained from the Web site of the ISIS Pulsed Neutron and Muon Facility, Rutherford Appleton Laboratory, UK (ISIS 2003). [Pg.1531]

Figure 3.5 High resolution time-of-flight neutron powder diffraction collected on deuterated AlMePO-p (Al2(CD3P03)3) at station HRPD at the pulsed neutron source ISIS, Oxfordshire, UK. The diffraction is measured at detectors at scattering angles of 168° (above left and, expanded, below) and 90° (above right). The profile has been fitted using Rietveld profile analysis in which the positions of 49 atoms were refined. [Reproduced from reference 43 with permission. Copyright 1999 Elsevier.] ""... Figure 3.5 High resolution time-of-flight neutron powder diffraction collected on deuterated AlMePO-p (Al2(CD3P03)3) at station HRPD at the pulsed neutron source ISIS, Oxfordshire, UK. The diffraction is measured at detectors at scattering angles of 168° (above left and, expanded, below) and 90° (above right). The profile has been fitted using Rietveld profile analysis in which the positions of 49 atoms were refined. [Reproduced from reference 43 with permission. Copyright 1999 Elsevier.] ""...
The calorimetric observation of two class transitions and their dependence on composition can be reasonably well explained by the above Ansatz. This is partly tme also for the dynamic features observed by inelastic neutron scattering on PEO/ PMMA. Incoherent scattering measured by direct time-of-flight neutron spectroscopy reveals two relaxation processes in the ps range and on the monomeric length scale. The fast process found is insensitive to mixing and resembles one of the... [Pg.356]

Figures Comparison of nuciear reactor and pulsed spaliation sources. For reactor sources (steady-state method), a narrow band of wavelengths is seiected with a monochromator crystal and the scattering angle (26,) Is varied to scan dspacings. Pulsed sources (time-of-flight method) use almost the entire avail-abie neutron spectrum, fix the scattering angie (26,), and simultaneousiy detect a neutron while determining its time of flight. Figures Comparison of nuciear reactor and pulsed spaliation sources. For reactor sources (steady-state method), a narrow band of wavelengths is seiected with a monochromator crystal and the scattering angle (26,) Is varied to scan dspacings. Pulsed sources (time-of-flight method) use almost the entire avail-abie neutron spectrum, fix the scattering angie (26,), and simultaneousiy detect a neutron while determining its time of flight.
Experimentally, scattering cross sections are measured as a function of the time of flight, t, of scattered neutron over a fixed distance, /. Final neutron energy, hiOy is related to (///) as... [Pg.132]

Fig. 1. Energy distribution of neutrons scattered by hydrogen in liquid argon at 100"K and 26.5 atm, as a function of time of flight for various scattering angles, 6. Solid curve, interpolation model. Dashed curve, Sears itinerant oscillator model. Jagged curve, Experiment. Abscissa is time of flight in usec/m and ordinate is cross section in mb sr-1 usee-1. Fig. 1. Energy distribution of neutrons scattered by hydrogen in liquid argon at 100"K and 26.5 atm, as a function of time of flight for various scattering angles, 6. Solid curve, interpolation model. Dashed curve, Sears itinerant oscillator model. Jagged curve, Experiment. Abscissa is time of flight in usec/m and ordinate is cross section in mb sr-1 usee-1.
Inelastic neutron scattering, on the other hand, usually employs a monochromatic neutron beam and records the intensity of the scattered neutron beam as a function of neutron kinetic energy. Such inelastic collision spectra are monitored as a function of the applied field and the (usually low) temperature. The observed peaks then represent the energy differences of thermally populated and excited unpopulated multiplet states. Inelastic neutron scattering experiments can be conducted using triple-axis, backscattering, or time-of-flight spectrometers. [Pg.85]

The theory of the magnetic scattering of thermal neutrons has been described in some detail by Marshall and Lovesey (1). Only a brief outline of those relations relevant to the present discussion will be given here. This limits the discussion to elastic scattering by spin-only systems ). Experimental techniques such as time-of-flight diffractometery are not discussed as no applications have yet been made to the subject under discussion. [Pg.21]


See other pages where Time of flight, neutron scattering is mentioned: [Pg.493]    [Pg.111]    [Pg.115]    [Pg.493]    [Pg.111]    [Pg.115]    [Pg.4513]    [Pg.123]    [Pg.640]    [Pg.304]    [Pg.4512]    [Pg.5]    [Pg.40]    [Pg.321]    [Pg.493]    [Pg.26]    [Pg.249]    [Pg.215]    [Pg.21]    [Pg.70]    [Pg.155]    [Pg.185]    [Pg.21]    [Pg.132]    [Pg.396]    [Pg.255]    [Pg.466]    [Pg.183]    [Pg.137]    [Pg.153]    [Pg.78]    [Pg.104]    [Pg.4526]    [Pg.6138]    [Pg.6142]    [Pg.6158]    [Pg.29]    [Pg.248]    [Pg.340]    [Pg.372]    [Pg.286]    [Pg.5]    [Pg.5]    [Pg.6]   
See also in sourсe #XX -- [ Pg.29 ]




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Flight time

Neutron scattering

Scattering of neutrons

Scattering time

Time-of-flight

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