The transmission function for neutron scattering instruments is developed
using acceptance diagrams.
This formalism clarifies why some optimisations (eg HRPD) work. This talk
develops the formalism for a Three Axis Spectrometer. Scan profiles are the
convolution of two 2D shapes corresponding to the neutrons scattered by the
sample and the secondary spectrometer transmission. An optimised scan matches
these shapes to each other and to the slope of any dispersion surface in the
scattering. Ideally the shapes are narrow in the scan direction and broad
perpendicular to that direction. Simple calculations show some surprising
results. Principal among these are that collimator widths and crystal mosaic
should be considerably larger in the secondary spectrometer than in the primary
spectrometer for a normal scan (E>0 and kF fixed) and that the plough or
long-chair configurations are superior to the W at sample scattering angles
less than about the monochromator take-off angle. The reflecting Soller
collimators developed at ILL are described. It is shown that the gains from
such collimators should be a factor of 3 on a HRPD and 5 on a TAS not the
factor of 2 previously expected. This may make them viable competitors to
horizontal focussing monochromators
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Last modified 23-May-2002