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Technical Information - Taipan
Taipan

Technical Information - Taipan

Specifications, Beryllium Filter, User Manual, Instrument reference

Specifications

Angular ranges 
  • 15° < 2θM< 85°
  • -145° < 2θs< 115°
  • -110°< 2θA< 110°
     
Monochromator    
  • 200 mm x 200 mm in 9 x 11 segments (width x height) 
  • Continuous horizontal and vertical focussing 
  • Pyrolytic Graphite (002) 24' mosaic with Incident Energy Range: ~ 5 - 60 meV) 
  • Copper (200) 20' mosaic with Incident Energy Range: ~ 14 - 160 meV)

Sample area    

  • Beam size at monochromator shielding exit 50mm x 130 mm (W x H) 
  • Flux at sample position is projected to be ~ 2x108 ncm2s-1 at 50 meV

Analyser

  • 160 mm x 140 mm in 5 x 7 segments (width x height) 
  • Continuous horizontal and vertical focusing 
  • Pyrolytic Graphite (002) 24' mosaic
Soller collimators
  • Pre-monochromator collimators 15', 30', Open; 90 x 185 mm2 (W x H) 
  • Post-monochromator, pre-analyser and pre-detector, collimators: 20', 40', Open; 50 x 130 mm2 (WxH)
Detector    
  • 3He detector, (diameter)25mm x 100 mm, p=10 bars 
  • Or (diameter)50mm x 100 mm, p=5 bars

Beryllium Filter

In 2014, commissioned a major new option on our Taipan thermal-neutron 3-axis spectrometer, namely a beryllium-filter secondary spectrometer option, dedicated to molecular-spectroscopy studies.  In the most part, this is useful for studying normal modes in hydrogenous molecules, and the method complements optical spectroscopy methods like infra-red and Raman spectroscopy. 

Beryllium filter

As in the normal, triple-axis spectrometer the incident neutron energy is determined using a large focussing crystal monochromator, but rather than using a similar analyser crystal, we use a large assembly of cooled polycrystalline beryllium transmission filters, which only allow very low-energy neutrons through.  In order to clean the signal up further, there are additional filters of graphite and bismuth.

The advantage of this method is that one can collect a vastly increased solid angle of scattered neutrons from the sample, at the expense of having more constrained dynamic range in Q.  The latter does not matter very much for non-dispersive modes like those in molecules, or in the measurement of powder-averaged densities of phonon states in solids.

Our Be-filter option on Taipan, is closely modelled on the BT-4 Filter Analyzer Neutron Spectrometer at NIST, albeit with some improvements, and we are very grateful to our colleagues at the National Centre for Neutron Science at NIST for their substantial advice and assistance. 

This project received substantial external funding in 2009 from the Australian Research Council, via a $400k LIEF Grant submitted by AINSE, with the additional support of 8 Australian research organisations (UNSW, Griffith U., Sydney U., U. of Wollongong, Curtin U., UWS, U. of Melbourne and ANU).  In fact the contributions from these universities bring the inward investment to this project at OPAL up to approx. $1M.

Within ANSTO, Don Kearley was responsible for proposal writing and fundraising, and the project was initially managed by Anton Stampfl.  After January 2013, the project was managed by Andrew Eltobaji.

Users Manual

 

Instrument reference for publications

S. A. Danilkin, G. Horton, R. Moore, G. Braoudakis and M. E. Hagen, J. Neutron Res. 15, 55-60 (2007).