{"id":"W1593060474","doi":"10.1103/physrevlett.100.097001","title":"Observation of a 500 meV Collective Mode in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>La</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>Sr</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mi>CuO</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>Nd</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>CuO</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:math>Using Resonant Inelastic X-Ray Scattering","year":2008,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Physics of Superconductivity and Magnetism","field":"Physics and Astronomy","cited_by":111,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Toronto","funders":"","keywords":"Polarization (electrochemistry); Inelastic scattering; Excitation; Reciprocal lattice; Mode (computer interface); Scattering; Resonant inelastic X-ray scattering; Formalism (music)","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":[0.0001755702,0.0003246599,0.0001682705,0.00052493,0.0006800023,0.0003935919,0.0004544502,0.0007895086,0.01921184],"category_scores_gemma":[0.000220069,0.0001982184,0.000215559,0.0006738218,0.000384161,0.0003904507,0.0003952757,0.0008681047,0.001580539],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0005181666,"about_ca_system_score_gemma":0.0002462,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.003713242,"about_ca_topic_score_gemma":0.006923092,"domain_scores_codex":[0.9998899,0.000006575104,0.000002572099,0.00003543049,0.00003219993,0.00003331479],"domain_scores_gemma":[0.9998347,0.00004649733,0.00003712142,0.00002823187,0.00002630877,0.00002719617],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"observational","study_design_scores_codex":[0.001346452,0.0001527195,0.009205882,0.0004542623,0.00009487529,0.00165048,0.0009336872,0.001007817,0.9113982,0.006456204,0.04907347,0.01822605],"study_design_scores_gemma":[0.0002150163,0.0008062218,0.162912,0.0001729528,0.0001146527,0.001459335,0.00206687,0.01447153,0.7358583,0.002869223,0.07890601,0.0001480236],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9187807,0.0009891146,0.005822862,0.001578839,0.0002996534,0.00003078275,0.0041389,0.0009202104,0.06743887],"genre_scores_gemma":[0.9788142,0.0002345215,0.003006113,0.0002980766,0.00002260323,0.00004438337,0.002221911,0.0001614475,0.0151968],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.01921184,"threshold_uncertainty_score":0.06426996,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.0241574119734833,"score_gpt":0.2512603875432777,"score_spread":0.2271029755697944,"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."}}