{"id":"W2064812944","doi":"10.1103/physrevlett.100.217003","title":"Uncovering a Pressure-Tuned Electronic Transition in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>Bi</mml:mi><mml:mn>1.98</mml:mn></mml:msub><mml:msub><mml:mi>Sr</mml:mi><mml:mn>2.06</mml:mn></mml:msub><mml:msub><mml:mi mathvariant=\"normal\">Y</mml:mi><mml:mn>0.68</mml:mn></mml:msub><mml:msub><mml:mi>Cu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant=\"normal\">O</mml:mi><mml:mrow><mml:mn>8</mml:mn><mml:mo>+</mml:mo><mml:mi>δ</mml:mi></mml:mrow></mml:msub></mml:math>using Raman Scattering and X-Ray Diffraction","year":2008,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Physics of Superconductivity and Magnetism","field":"Physics and Astronomy","cited_by":19,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Waterloo","funders":"","keywords":"Raman spectroscopy; Physics; Cuprate; Condensed matter physics; Critical point (mathematics); Phonon; Materials science; Doping; Quantum mechanics; Mathematics","routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0001375793,0.0002516547,0.0002499729,0.0004207089,0.001040916,0.0007396371,0.0008218376,0.0009828415,0.04724712],"category_scores_gemma":[0.0005002882,0.0003056713,0.0001613832,0.0005856091,0.0004526875,0.001118321,0.0006583049,0.001547221,0.003384645],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0005064696,"about_ca_system_score_gemma":0.000219988,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002302226,"about_ca_topic_score_gemma":0.004146198,"domain_scores_codex":[0.99985,0.00000802074,0.000003373756,0.00003592429,0.00005665791,0.00004603888],"domain_scores_gemma":[0.9998854,0.00004238317,0.00001496395,0.0000206375,0.0000204886,0.00001597016],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.001558003,0.0003570966,0.004797169,0.001321657,0.00007997332,0.00347149,0.002027939,0.00567947,0.5886577,0.07011601,0.2432736,0.07865995],"study_design_scores_gemma":[0.0001826081,0.0009606467,0.02548835,0.0002109833,0.00006119843,0.001085153,0.001663042,0.05044085,0.6982552,0.01507283,0.2063964,0.0001827074],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.7577766,0.001337754,0.01628477,0.007208453,0.001379407,0.00002849646,0.005112211,0.003761917,0.2071104],"genre_scores_gemma":[0.9655201,0.0003672469,0.002695296,0.0007486401,0.00005646515,0.00002907458,0.002485204,0.0005525736,0.02754535],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.04724712,"threshold_uncertainty_score":0.1580573,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01539596290597591,"score_gpt":0.2352968317412046,"score_spread":0.2199008688352286,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). Scores rank; they never assert a category."}}