{"id":"W2614952272","doi":"10.1103/physrevlett.118.152502","title":"Scattering of the Halo Nucleus <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>Be</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>11</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math> on <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>Au</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>197</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math> at Energies around the Coulomb Barrier","year":2017,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Nuclear physics research studies","field":"Physics and Astronomy","cited_by":65,"is_retracted":false,"has_abstract":true,"ca_institutions":"TRIUMF; University of Guelph; Simon Fraser University","funders":"Seventh Framework Programme; Horizon 2020 Framework Programme; Ministerio de Economía y Competitividad; British Columbia Knowledge Development Fund; Natural Sciences and Engineering Research Council of Canada; European Commission; Università degli Studi di Padova; Canada Foundation for Innovation; TRIUMF; Villum Fonden","keywords":"Physics; Halo; Atomic physics; Breakup; Excited state; Halo nucleus; Nuclear reaction; Semiclassical physics; Scattering; Nuclear physics; Quantum mechanics","routes":{"ca_aff":true,"ca_fund":true,"ca_venue":false,"about_ca":true,"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":[0.0009646133,0.001086854,0.001215458,0.001247152,0.002046882,0.002094004,0.001157693,0.001153313,0.08103643],"category_scores_gemma":[0.001768875,0.0005976178,0.001672756,0.001661673,0.0005711319,0.0009976774,0.001581054,0.001945441,0.01349927],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.002626622,"about_ca_system_score_gemma":0.001711092,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0152272,"about_ca_topic_score_gemma":0.01589258,"domain_scores_codex":[0.9991577,0.0000920618,0.00001376993,0.0001393321,0.0003219327,0.0002751166],"domain_scores_gemma":[0.9990103,0.000228058,0.00004423899,0.0001894809,0.0002696052,0.0002583411],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"not_applicable","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.00297093,0.0003918873,0.02321322,0.001283198,0.000565822,0.004553372,0.003064795,0.05535115,0.1449593,0.247665,0.4000376,0.1159438],"study_design_scores_gemma":[0.000930375,0.001074494,0.06727825,0.0004854672,0.0004153108,0.002220814,0.002731769,0.2990596,0.2504474,0.1625525,0.2118894,0.0009145495],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"other","genre_gemma":"empirical","genre_scores_codex":[0.2542747,0.001982732,0.08542631,0.003655195,0.00227582,0.0002347427,0.0138614,0.01077647,0.6275126],"genre_scores_gemma":[0.7900744,0.001191313,0.01251167,0.001665427,0.0002354312,0.0002108927,0.02049425,0.009679131,0.1639374],"genre_candidate":"empirical","genre_consensus":null,"teacher_disagreement_score":0.08103643,"threshold_uncertainty_score":0.2710939,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02651849913174939,"score_gpt":0.2696827905241199,"score_spread":0.2431642913923705,"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."}}