In collaboration with the instrument staff, members of the Carnegie IDT team (Guthrie, Boehler, Li, Machida) have increased the maximum pressure for measuring structural refinement-quality data to 57 GPa. At this (unofficial) record-breaking pressure Bragg intensities were clearly visible down to ~0.75 Å and full structural refinements have conducted.
On increasing the pressure further, there was a failure of the carbide seat (at an estimated 60 GPa). In ongoing developments, these seats will be replaced with a sintered diamond variant, with the aim of extending the maximum pressure further into the 100 GPa range.
The figure shows a Rietveld fit to a typical data set from a test sample of D2O at around 3 GPa measured on SNAP.
Wednesday, April 11, 2012
Friday, March 30, 2012
Zr gasket provides new window at high d
For crystalline systems with structure at high d-spacings 7-10 Å, including many magnetic systems, it has been so far necessary to use detectors in a low-angle geometry, with concurrent loss in resolution. Another possibility has been to use the bandwidth choppers to use very long wavelength neutrons to probe this structure with increased resolution. However, the substantial attenuation of the gasket and pressure vessel has made this unfeasible.
Xiaojia Chen has used IDT time to successfully test a pure Zr gasket in place of the more conventional TiZr alloys. The low absorption cross-section of Zr (0.185 barn at 2200m/s) versus Ti (6.09 barn at 2200m/s) means that a much stronger sample signal is accessible with the new gaskets. These measurements use a vertical geometry with the beam entering and exiting through the gasket and both detectors at 90 degrees. Testing has shown that the resulting data shows sharp strong Bragg peaks on very low backgrounds.
Xiaojia Chen has used IDT time to successfully test a pure Zr gasket in place of the more conventional TiZr alloys. The low absorption cross-section of Zr (0.185 barn at 2200m/s) versus Ti (6.09 barn at 2200m/s) means that a much stronger sample signal is accessible with the new gaskets. These measurements use a vertical geometry with the beam entering and exiting through the gasket and both detectors at 90 degrees. Testing has shown that the resulting data shows sharp strong Bragg peaks on very low backgrounds.
Tuesday, March 20, 2012
Pellet mass calculator
Jamie has released a mass calculator for typical pellets used with the PE toroidal anvils...you may find this useful:
http://neutrons.ornl.gov/instruments/SNS/SNAP/calc.shtml
http://neutrons.ornl.gov/instruments/SNS/SNAP/calc.shtml
Thursday, February 23, 2012
IDT time allocated for 2012-A
The IDT allocation committee have met and decided on the beamtime allocations. We received requests for 62 days of beamtime with a total of 24 days available this cycle. In making the allocations, the committee followed the core priorities of the IDT. Here's looking forwards to a successful cycle!
Monday, February 13, 2012
Magnetic order in new polymorph of Mn3O4
As part of the ongoing development of low-temperature capabilities on SNAP, IDT member Shigeto Hirai has determined the magnetic structure of the orthorhombic Mn3O4 measured at ambient pressure and below the Neel temperature. As part of an IDT focus on low-temperature capabilities for SNAP, Shigeto aims to extend these measurements combining high pressure and lower temperature.
Figure shows Shigeto's Rietveld fit to the new magnetically ordered low temperature phase.
Friday, January 27, 2012
IDT Proposal deadline today!
Today is the deadline for submitting proposals for IDT beamtime. There are 24 days available in the upcoming cycle from Feb-June 2012.
Sunday, December 18, 2011
IDT team reaches 44 GPa on SNAP!
An IDT team including Malcolm Guthrie, Reini Boehler and Kuo Li (all Geophysical Laboratory) has achieved a new pressure record for SNAP. Using specially designed anvils inside a panoramic cell driven by a PE press, a sample of ice VII (D2O) was compressed to 44 GPa at room temperature. The panoramic cell can be gas loaded, adding and adds this important capability to the instrument. Also, optical access facilitates in-situ measurement of pressure via ruby fluorescence.
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