{"id":"W3107117957","doi":"10.1103/physrevb.88.144516","title":"Electron doping evolution of the magnetic excitations in BaFe<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mrow/><mml:mrow><mml:mn>2</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math>Ni<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mrow/><mml:mi>x</mml:mi></mml:msub></mml:math>As<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub></mml:math>","year":2013,"lang":"lv","type":"article","venue":"Physical Review B","topic":"Iron-based superconductors research","field":"Materials Science","cited_by":48,"is_retracted":false,"has_abstract":true,"ca_institutions":"Atomic Energy (Canada)","funders":"","keywords":"Antiferromagnetism; Condensed matter physics; Physics; Doping; Resonance (particle physics); Inelastic neutron scattering; Superconductivity; Order (exchange); Electron; Spin wave; Materials science; Neutron scattering; Neutron; Atomic physics; Nuclear physics; Ferromagnetism","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":[0.0001194825,0.0001802233,0.00017233,0.0002409831,0.0004582758,0.0004982501,0.0003740603,0.0003186782,0.006029943],"category_scores_gemma":[0.0003269849,0.000160782,0.0001074909,0.0002347299,0.0004048331,0.0003583888,0.0002576922,0.0004526724,0.0005122803],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0007388667,"about_ca_system_score_gemma":0.0002222779,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.004530218,"about_ca_topic_score_gemma":0.005710408,"domain_scores_codex":[0.999928,0.000008468905,0.000003198862,0.00001295935,0.00001921107,0.0000281306],"domain_scores_gemma":[0.9998537,0.00005721413,0.0000309973,0.00001104874,0.00002946516,0.00001753032],"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":[0.001642505,0.0003562003,0.009282771,0.0003236127,0.000060343,0.0006541334,0.00108905,0.01565257,0.9255016,0.02185445,0.006513446,0.01706928],"study_design_scores_gemma":[0.0000823323,0.0003649986,0.02955195,0.00009239759,0.00004175774,0.0001691593,0.0006718098,0.08636375,0.8721839,0.002449549,0.007960333,0.00006807892],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9907501,0.000273762,0.0008775449,0.0002175672,0.00002249803,0.000004864263,0.000264967,0.00007283773,0.007515838],"genre_scores_gemma":[0.9939426,0.0002412353,0.0008368329,0.00004176024,0.000003542738,0.00001285207,0.0002910997,0.00004794726,0.004582096],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.006029943,"threshold_uncertainty_score":0.02017212,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01993028078985278,"score_gpt":0.2655383433227089,"score_spread":0.2456080625328561,"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."}}