{"id":"W2331177922","doi":"10.1103/physreva.89.043403","title":"Shifts due to quantum-mechanical interference from distant neighboring resonances for saturated fluorescence spectroscopy of the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mn>2</mml:mn><mml:msup><mml:mspace width=\"0.16em\"/><mml:mn>3</mml:mn></mml:msup><mml:mi>S</mml:mi></mml:mrow></mml:math>to<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mn>2</mml:mn><mml:msup><mml:mspace width=\"0.16em\"/><mml:mn>3</mml:mn></mml:msup><mml:mi>P</mml:mi></mml:mrow></mml:math>intervals of helium","year":2014,"lang":"lv","type":"article","venue":"Physical Review A","topic":"Cold Atom Physics and Bose-Einstein Condensates","field":"Physics and Astronomy","cited_by":24,"is_retracted":false,"has_abstract":true,"ca_institutions":"York University","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Physics; Spectroscopy; Imaging phantom; Helium; Fluorescence spectroscopy; Atomic physics; Interference (communication); Quantum; Fluorescence; Optics; Quantum mechanics","routes":{"ca_aff":true,"ca_fund":true,"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":[0.0008140656,0.0004631052,0.0002603207,0.0004600094,0.0007607348,0.000406639,0.0008560132,0.0006700018,0.0253813],"category_scores_gemma":[0.001923141,0.0004264306,0.0003649355,0.0005086688,0.000578739,0.0009194481,0.0006305138,0.001372263,0.002545614],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0009840919,"about_ca_system_score_gemma":0.0005491826,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001556593,"about_ca_topic_score_gemma":0.005073854,"domain_scores_codex":[0.9993254,0.0001397073,0.00002343622,0.0001475222,0.0002728424,0.00009108622],"domain_scores_gemma":[0.9990193,0.0005679107,0.0001037426,0.0001767236,0.00009175351,0.00004064488],"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":[0.0004849968,0.00005861361,0.001143957,0.0002230686,0.00003719126,0.0002384352,0.0002255313,0.001493176,0.9672586,0.005906784,0.003506514,0.01942314],"study_design_scores_gemma":[0.00002471313,0.0001162236,0.003383942,0.00001563802,0.00002105244,0.0002036667,0.00007168654,0.005735843,0.9828976,0.001018026,0.006488909,0.0000227794],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.7801712,0.001376478,0.1607644,0.001301695,0.0002999869,0.00008874605,0.00139954,0.004012948,0.05058499],"genre_scores_gemma":[0.9228451,0.00101408,0.05304074,0.0003988669,0.00002164908,0.0001115723,0.001447026,0.0009939577,0.02012695],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.0253813,"threshold_uncertainty_score":0.0849089,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01928344887047619,"score_gpt":0.2589649656703838,"score_spread":0.2396815167999076,"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."}}