TOPAZ is a neutron wavelength-resolved time-of-flight (TOF) Laue single-crystal diffractometer at the Spallation Neutron Source (SNS). This guide focuses on the steps most users need to get started: determine the UB matrix, plan sample orientations, reduce TOPAZ data to an HKL file, and continue to nuclear, magnetic, or diffuse-scattering analysis.
TOPAZ workflow:
UB matrix → experiment plan → data collection → TOPAZ Data Reduction (ReductionGUI) → HKL → nuclear or magnetic structure refinement.
Diffuse-scattering workflow:
UB matrix → GARNET → normalized 3D reciprocal-space data → 3D-ΔPDF and/or diffuse-scattering modeling.
TOPAZ experiment data are stored under:
/SNS/TOPAZ/IPTS-#####/
where IPTS-##### is the experiment proposal number. Use the experiment shared area for analysis products and files used with the TOPAZ team:
/SNS/TOPAZ/IPTS-#####/shared/
The NDIP application page should be treated as the authoritative source for the currently deployed software versions.
A reliable orientation matrix (UB) is required for experiment planning, indexing, and integrated-intensity reduction. Use NeuXtalViz UB Tools with one or more initial TOPAZ runs.
Tutorials:
Most strong Bragg peaks should be indexed by the selected cell and UB matrix. Systematic unindexed peaks can indicate a second domain, twinning, a superstructure, modulation, or magnetic scattering.
If satellite reflections are present, use the NeuXtalViz Modulation Tools to identify candidate modulation vectors before final integration.
After obtaining a stable UB matrix, use the NeuXtalViz Experiment Planner to choose sample orientations that provide the reciprocal-space coverage required for the experiment.
See Experiment Plan with Silicon Data for a step-by-step TOPAZ example.
During data collection, inspect representative peaks and reciprocal-space slices before committing to the full orientation series. Check the UB matrix, peak shapes and mosaicity, unindexed peaks, satellites, and the reciprocal-space regions being measured.
For standard Bragg diffraction, the immediate reduction goal is a corrected, integrated HKL reflection file for nuclear or magnetic structure analysis. Open NDIP Single Crystal Diffraction and start TOPAZ Data Reduction.
For experiments using the shared analysis directories, reduction and calibration files are normally kept under:
/SNS/TOPAZ/IPTS-#####/shared/ReductionGUI/
/SNS/TOPAZ/IPTS-#####/shared/calibration/
Before running the final reduction, confirm:
The TOPAZ reduction workflow indexes and integrates reflections and applies the instrument- and sample-dependent corrections required to place observations on a consistent intensity scale. These include incident-spectrum, detector-response, Lorentz, and wavelength-dependent sample-absorption corrections. Extinction is normally handled during structure refinement when required.
Primary output: TOPAZ integrated reflections can be exported in SHELX HKLF 2 TOF-Laue format. Each observation retains the Miller indices, integrated intensity and uncertainty, batch identifier, and neutron wavelength.
Before proceeding to refinement, inspect representative strong, medium, and weak reflections. Check integration, background, detector-edge cases, overlapping peaks, and any wavelength- or run-dependent anomalies.
After ReductionGUI produces the HKL file, continue directly on the NDIP Single Crystal Diffraction platform.
For magnetic diffraction, first establish which reflections or satellites are magnetic, determine the propagation vector when applicable, and use magnetic symmetry or representation analysis before refinement. JANA2020 is the preferred NDIP environment for combined nuclear/magnetic refinement, multiple propagation vectors, modulation, or complex symmetry.
Additional software and refinement resources are available on the Single-Crystal Diffraction Software Resources page.
Diffuse-scattering experiments follow a different analysis path from Bragg-only structure refinement. For TOPAZ, use GARNET for reciprocal-space reconstruction and normalization, followed by 3D-ΔPDF and/or model-based diffuse-scattering analysis.
See NeuXtalViz 3D-ΔPDF with Tb5Ru6Sn18 Data for step-by-step TOPAZ example.
See the Single-Crystal Diffraction Software Resources page for additional diffuse-scattering tools.
Publications containing TOPAZ data should include the required facility acknowledgment:
This research [or, A portion of this research] used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory.
Instrument reference: Coates L., Cao H.B., Chakoumakos B.C., Frontzek M., Hoffmann C., Kovalevsky A., Liu Y., Meilleur F., dos Santos A.M., Myles D.A., Wang X.P., Ye F., "A suite-level review of the neutron single-crystal diffraction instruments at Oak Ridge National Laboratory", Review of Scientific Instruments, 89, 092802 (2018).
Please submit publications, theses, patents, and other research products to PuSH (Publications of SNS and HFIR).
Contact the TOPAZ Instrument Team for experiment-specific questions about UB determination, experiment planning, integration, absorption, twinning, modulation, magnetic diffraction, or diffuse scattering. For computing and data-access problems, use the support information on the Single-Crystal Diffraction Documentation and Data Management pages.
Oak Ridge National Laboratory is managed by UT-Battelle LLC for the US Department of Energy