10.1002/anie.202005056
Angewandte Chemie International Edition
Caution! SO3 is a strong oxidizer which needs careful handling. During the reaction and even after cooling down to room
temperature the glass tube might be under pressure. The tube should be cooled with liquid nitrogen before opened.
Structure determination
Crystal structure determination has been performed at the P24.1 beamline of the PETRA III facility at German Electron
Synchrotron (DESY) Hamburg (Germany). Therefore, single crystals of S6N2O15 were prepared under inert oil and selected
with the aid of a polarization filter of a light microscope. Attached to a micromount, one single crystal was positioned in the
cold nitrogen gas stream (100.0(2) K) of the single crystal diffractometer (Huber 4-circle Kappa, P24 Beamline, Petra III) and
intensity data was collected. Both the collect intensity data were reduced, and a cell refinement was carried out.[1] The structure
solution under the assumption of the respective space group was successful by intrinsic phasing (SHELXT).[2] Finally,
anisotropic displacement parameters were introduced and a multi-scan absorption correction was applied to the reflection data.
Atomic positions and further details of the crystal structures can be obtained from the joint CCDC/FIZ Karlsruhe deposition
service on quoting the deposition number 1901458.
IR analysis
IR spectroscopic data were collected with a Bruker Alpha Platinum spectrometer, using the ATR method (attenuated total
reflection) in transmission mode. The spectra were measured in the bulk phase on several collected crystals in the range from
4000 to 570 cm–1. The IR spectroscopic data were processed and corrected for atmospheric influence by using the OPUS 7.5
software. Important IR bands in cm–1 (exptl./calcd.): 1512/1535, 1478/1487, 1232/1253, 889/893, 850/831, 699/708, 531/560,
414/403.
Calculation method
A full geometry optimization of the trimer of S6N2O15 was performed within density functional theory (DFT) using the PBE0
exchange-correlation functional and a cc-pVTZ basis set. The calculations were also used for assigning the IR frequencies.
Throughout the study the Turbomole program package was used.
Acknowledgement
We acknowledge DESY (Hamburg, Germany), a member of the Helmholtz Association HGF, for the provision of experimental
facilities. Parts of this research were carried out at PETRA III and we would like to thank Carsten Paulmann and Heiko Schulz-
Ritter for assistance in using the P24 EH1 X-ray Diffraction Kappa-diffractometer. Furthermore, we are indebted to André
Santos Martins for technical assistance.
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