<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Peng K</submitter><funding>United States Department of Defense | United States Navy | Office of Naval Research</funding><funding>United States Department of Defense | United States Army | U.S. Army Research, Development and Engineering Command | Army Research Office</funding><funding>U.S. Department of Energy</funding><funding>Gordon and Betty Moore Foundation (Gordon E. and Betty I. Moore Foundation)</funding><funding>Nebraska Public Power District through the Nebraska Center for Energy Sciences Research</funding><funding>Ernest S. Kuh Endowed Chair Professorship</funding><funding>United States Department of Defense | United States Navy | Office of Naval Research (ONR)</funding><funding>Gordon and Betty Moore Foundation</funding><funding>National Science Foundation (NSF)</funding><funding>United States Department of Defense | United States Army | U.S. Army Research, Development and Engineering Command | Army Research Office (ARO)</funding><funding>Canada Research Chairs</funding><funding>National Science Foundation</funding><pagination>7388</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9712507</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>13(1)</volume><pubmed_abstract>Quantum fluids exhibit quantum mechanical effects at the macroscopic level, which contrast strongly with classical fluids. Gain-dissipative solid-state exciton-polaritons systems are promising emulation platforms for complex quantum fluid studies at elevated temperatures. Recently, halide perovskite polariton systems have emerged as materials with distinctive advantages over other room-temperature systems for future studies of topological physics, non-Abelian gauge fields, and spin-orbit interactions. However, the demonstration of nonlinear quantum hydrodynamics, such as superfluidity and Čerenkov flow, which is a consequence of the renormalized elementary excitation spectrum, remains elusive in halide perovskites. Here, using homogenous halide perovskites single crystals, we report, in bo</pubmed_abstract><journal>Nature communications</journal><pubmed_title>Room-temperature polariton quantum fluids in halide perovskites.</pubmed_title><pmcid>PMC9712507</pmcid><funding_grant_id>N00014-22-1-2322</funding_grant_id><funding_grant_id>W911NF1810149</funding_grant_id><funding_grant_id>N00014-21-1-2099</funding_grant_id><funding_grant_id>5722</funding_grant_id><funding_grant_id>DMR-2143041</funding_grant_id><funding_grant_id>OIA-2044049</funding_grant_id><pubmed_authors>Kena-Cohen S</pubmed_authors><pubmed_authors>Jin D</pubmed_authors><pubmed_authors>Zhang X</pubmed_authors><pubmed_authors>Bao W</pubmed_authors><pubmed_authors>Tao R</pubmed_authors><pubmed_authors>Haeberle L</pubmed_authors><pubmed_authors>Li Q</pubmed_authors><pubmed_authors>Fleming GR</pubmed_authors><pubmed_authors>Peng K</pubmed_authors></additional><is_claimable>false</is_claimable><name>Room-temperature polariton quantum fluids in halide perovskites.</name><description>Quantum fluids exhibit quantum mechanical effects at the macroscopic level, which contrast strongly with classical fluids. Gain-dissipative solid-state exciton-polaritons systems are promising emulation platforms for complex quantum fluid studies at elevated temperatures. Recently, halide perovskite polariton systems have emerged as materials with distinctive advantages over other room-temperature systems for future studies of topological physics, non-Abelian gauge fields, and spin-orbit interactions. However, the demonstration of nonlinear quantum hydrodynamics, such as superfluidity and Čerenkov flow, which is a consequence of the renormalized elementary excitation spectrum, remains elusive in halide perovskites. Here, using homogenous halide perovskites single crystals, we report, in bo</description><dates><release>2022-01-01T00:00:00Z</release><publication>2022 Nov</publication><modification>2026-06-03T13:20:56.044Z</modification><creation>2026-04-28T03:10:16.434Z</creation></dates><accession>S-EPMC9712507</accession><cross_references><pubmed>36450719</pubmed><doi>10.1038/s41467-022-34987-y</doi></cross_references></HashMap>