PHYS01200804001 Sohrab Abbas - Homi Bhabha National Institute
PHYS01200804001 Sohrab Abbas - Homi Bhabha National Institute
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