{"id":"W2978221711","doi":"10.1139/p11-101","title":"The Einstein–Maxwell-particle system in the York canonical basis of ADM tetrad gravity. Part 2. The weak field approximation in the 3-orthogonal gauges and Hamiltonian post-minkowskian gravity: the <i>N</i>-body problem and gravitational waves with asymptotic background <sup>1</sup>This paper is one of three companion papers published in the same issue of <i>Can. J. Phys.</i>","year":2012,"lang":"en","type":"article","venue":"Canadian Journal of Physics","topic":"Pulsars and Gravitational Waves Research","field":"Physics and Astronomy","cited_by":27,"is_retracted":false,"has_abstract":true,"ca_institutions":"","funders":"","keywords":"Physics; Tetrad; General relativity; Gravitational field; Mathematical physics; Hamiltonian (control theory); Gravitational wave; Classical mechanics; Hamiltonian constraint; Gravitation; Quantum mechanics; Quantum gravity","routes":{"ca_aff":false,"ca_fund":false,"ca_venue":true,"about_ca":false,"invisible_to_affiliation_only":true},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"codex-gemma-dda1882f352a","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.002350737,0.0002104558,0.0003556522,0.00007732842,0.0003501646,0.0001996438,0.0006760748,0.00005446705,0.00002541891],"category_scores_gemma":[0.0000443192,0.00009297785,0.0001221883,0.0006524614,0.000638788,0.0003451147,0.00003194932,0.0006302214,4.100631e-7],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00005155204,"about_ca_system_score_gemma":0.0006063582,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.006295364,"about_ca_topic_score_gemma":0.01385815,"domain_scores_codex":[0.9973013,0.0007204214,0.0006586873,0.0001679105,0.0007171792,0.000434547],"domain_scores_gemma":[0.9971375,0.001690792,0.0004298147,0.0003708038,0.0002450773,0.0001259687],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"observational","study_design_scores_codex":[0.0002812623,0.0007921835,0.2985295,0.000314371,0.0004711233,0.00000717267,0.0654647,0.0009784236,0.002073328,0.6183152,0.001896737,0.010876],"study_design_scores_gemma":[0.002293256,0.0008485385,0.8178404,0.0007081999,0.0002726245,0.00006986206,0.1108078,0.001408728,0.0008309084,0.06034921,0.004159935,0.000410544],"study_design_candidate":"observational","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9759054,0.00065675,0.00001637332,0.02136212,0.00003934052,0.0007874259,0.0003176791,8.061974e-7,0.0009141304],"genre_scores_gemma":[0.999024,0.00001557083,0.00006925746,0.0005765974,0.0001835001,0.00003649199,0.00005046368,0.00001403454,0.00003012407],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.557966,"threshold_uncertainty_score":0.9516749,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01420017320234486,"score_gpt":0.24281059781756,"score_spread":0.2286104246152152,"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."}}