<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Zhang X</submitter><funding>National Natural Science Foundation of China</funding><funding>Youth Innovation Promotion Association of the Chinese Academy of Sciences</funding><funding>West Light Foundation of the Chinese Academy of Sciences</funding><pagination>2454-2461</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC8979095</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>12(4)</volume><pubmed_abstract>A series of &lt;i>in situ&lt;/i> high-pressure Raman spectroscopy and electrical conductivity experiments have been performed to investigate the vibrational and electrical transport properties of SnS&lt;sub>2&lt;/sub> under non-hydrostatic and hydrostatic environments. Upon compression, an coupled structural-electronic transition in SnS&lt;sub>2&lt;/sub> occurred at 30.2 GPa under non-hydrostatic conditions, which was evidenced by the splitting of the E&lt;sub>g&lt;/sub> mode and the discontinuities in Raman shifts, Raman full width at half maximum (FWHM) and electrical conductivity. However, the coupled structural-electronic transition took place at a higher pressure of 33.4 GPa under hydrostatic conditions, which may be due to the influence of the pressure medium. Furthermore, our first-principles theoretical calculations results revealed that the bandgap energy of SnS&lt;sub>2&lt;/sub> decreased slowly with increasing pressure and it closed in the pressure range of 30-40 GPa, which agreed well with our Raman spectroscopy and electrical conductivity results. Upon decompression, the recoverable Raman peaks and electrical conductivity indicated that the coupled structural-electronic transition was reversible, which was further confirmed by our HRTEM observations.</pubmed_abstract><journal>RSC advances</journal><pubmed_title>Pressure-induced coupled structural-electronic transition in SnS&lt;sub>2&lt;/sub> under different hydrostatic environments up to 39.7 GPa.</pubmed_title><pmcid>PMC8979095</pmcid><funding_grant_id>41774099</funding_grant_id><funding_grant_id>42072055</funding_grant_id><funding_grant_id>2019390</funding_grant_id><funding_grant_id>41772042</funding_grant_id><pubmed_authors>Hong M</pubmed_authors><pubmed_authors>Dai L</pubmed_authors><pubmed_authors>Li C</pubmed_authors><pubmed_authors>Zhang X</pubmed_authors><pubmed_authors>Hu H</pubmed_authors></additional><is_claimable>false</is_claimable><name>Pressure-induced coupled structural-electronic transition in SnS&lt;sub>2&lt;/sub> under different hydrostatic environments up to 39.7 GPa.</name><description>A series of &lt;i>in situ&lt;/i> high-pressure Raman spectroscopy and electrical conductivity experiments have been performed to investigate the vibrational and electrical transport properties of SnS&lt;sub>2&lt;/sub> under non-hydrostatic and hydrostatic environments. Upon compression, an coupled structural-electronic transition in SnS&lt;sub>2&lt;/sub> occurred at 30.2 GPa under non-hydrostatic conditions, which was evidenced by the splitting of the E&lt;sub>g&lt;/sub> mode and the discontinuities in Raman shifts, Raman full width at half maximum (FWHM) and electrical conductivity. However, the coupled structural-electronic transition took place at a higher pressure of 33.4 GPa under hydrostatic conditions, which may be due to the influence of the pressure medium. Furthermore, our first-principles theoretical calculations results revealed that the bandgap energy of SnS&lt;sub>2&lt;/sub> decreased slowly with increasing pressure and it closed in the pressure range of 30-40 GPa, which agreed well with our Raman spectroscopy and electrical conductivity results. Upon decompression, the recoverable Raman peaks and electrical conductivity indicated that the coupled structural-electronic transition was reversible, which was further confirmed by our HRTEM observations.</description><dates><release>2022-01-01T00:00:00Z</release><publication>2022 Jan</publication><modification>2025-04-19T12:58:31.136Z</modification><creation>2025-04-19T12:58:31.136Z</creation></dates><accession>S-EPMC8979095</accession><cross_references><pubmed>35425242</pubmed><doi>10.1039/d1ra08632d</doi></cross_references></HashMap>