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PHYS01200804001 Sohrab Abbas - Homi Bhabha National Institute

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4.5 Tightening the neutron collimation still further<br />

The tight collimation of neutrons increases their transverse coherence length to greater than 100<br />

μm FWHM and hence forms a nearly plane wave of monochromatic neutrons. The neutron<br />

collimation may be tightened further by reducing the neutron wavelength. For instance, the same<br />

Bragg prism monochromator-analyser pair optimised for 5.26 Å neutrons can super collimate 1.75<br />

Å neutrons using the {333} reflection in the same geometric configuration down further by a factor<br />

of 9. The {333} Si Debye Waller factor is less than that for {111}, since<br />

<br />

<br />

<br />

<br />

2<br />

B<br />

with parameters B=0.422Å 2 , ΔB=0.028Å 2 at 293 K [157]. The<br />

DW exp (B B) sin /<br />

corresponding reduction in F H should improve the collimation further. With an optimised 1.75 Å<br />

neutron incidence between 8 and 32 mm from the prism apex, the Bragg prism monochromator is<br />

expected to deliver an angular profile of 0.062 arcsec FWHM (Fig.48). An analyser operating in<br />

opposite asymmetry with S =−51 o and A=16 o with neutron incidence between 34 and 67 mm from<br />

the prism apex would likewise accept a pair of 0.023 arcsec wide neutron peaks separated by 0.22<br />

arcsec (black curve in Fig.49). The rocking curve of the analyser, viz. the convolution of the<br />

monochromator beam profile with analyser acceptance, comprises two 0.065 arcsec wide peaks<br />

separated by 0.25 arcsec (red curve in Fig.49).<br />

One may envisage tightening the neutron collimation further with Bragg prisms operating at still<br />

smaller wavelengths.<br />

89

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