{"meta":{"query_hash":"f88067592290","filters":{"venue":"High Energy Density Physics"},"cohort_total":12,"direct_labels_cover":0,"predictions_cover":12,"exported":12,"export_cap":100000,"truncated":false,"label_status":"direct model label, unvalidated","prediction_status":"machine_predicted_unvalidated (Codex and Gemma teacher distillation)","score_status":"score_only:v0-immature-baseline","snapshot":{"source":"OpenAlex, pinned release, all 482 partitions","release":"2026-06-24","frame_built":"2026-07-12"},"permalink":"https://metacan.xera.ac/q/f88067592290","api":"https://metacan.xera.ac/api/v1/cohort?venue=High+Energy+Density+Physics"},"results":[{"id":"W2005423858","doi":"10.1016/j.hedp.2007.02.035","title":"X-ray absorption of a warm dense aluminum plasma created by an ultra-short laser pulse","year":2007,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-induced spectroscopy and plasma","field":"Engineering","cited_by":14,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":true,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Institut National de la Recherche Scientifique","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Opacity; Materials science; Laser; Plasma; Absorption (acoustics); Spectral line; Absorption spectroscopy; Spectroscopy; Ionization; Atomic physics; Hohlraum; Optics; Physics; Ion","score_opus":0.008109181409681481,"score_gpt":0.20534884107571383,"score_spread":0.19723965966603235,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2005423858","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.97920626,0.000011151386,0.018032188,0.000007063028,0.00038547948,0.000070987364,0.000063739935,0.00031186463,0.0019112483],"genre_scores_gemma":[0.99840575,0.00004957639,0.0004624041,0.000064597465,0.00026674403,0.0000053464983,0.00040612312,0.00006637701,0.00027307495],"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.9985456,0.000038267182,0.000333575,0.00030810913,0.00030892214,0.00046554315],"domain_scores_gemma":[0.99911267,0.00009094661,0.000056488934,0.000423991,0.000111025816,0.0002048762],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00016097308,0.00031065868,0.00035692748,0.00006768322,0.00008691932,0.000027018961,0.00017022704,0.00023864036,0.000038431535],"category_scores_gemma":[0.000008939871,0.00033121975,0.00009880343,0.00031824855,0.00006294524,0.00027531807,0.000013547032,0.00023137087,0.00003130498],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00013102042,0.00026178197,0.00054760464,0.000035179062,0.0001190211,0.000051181534,0.00017802007,0.019876419,0.97180134,0.003148413,0.0015226364,0.0023273875],"study_design_scores_gemma":[0.00038333982,0.00011299864,0.0017049366,0.00002089434,0.00006318697,0.000010460205,0.000027052916,0.0060225315,0.99000376,0.0005600499,0.00072839676,0.00036239505],"about_ca_topic_score_codex":0.0005620163,"about_ca_topic_score_gemma":0.00066691404,"teacher_disagreement_score":0.019199478,"about_ca_system_score_codex":0.00010389798,"about_ca_system_score_gemma":0.00002024372,"threshold_uncertainty_score":0.999914},"labels":[],"label_agreement":null},{"id":"W2017596469","doi":"10.1016/j.hedp.2011.09.002","title":"Ab initio calculations of the equation of state of hydrogen in a regime relevant for inertial fusion applications","year":2011,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":23,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Dalhousie University","funders":"Lawrence Livermore National Laboratory; U.S. Department of Energy","keywords":"National Ignition Facility; Implosion; Physics; Equation of state; Inertial confinement fusion; Ab initio; Hydrogen; Quantum Monte Carlo; Phase (matter); Monte Carlo method; Statistical physics; Atomic physics; Thermodynamics; Plasma; Quantum mechanics","score_opus":0.02167304329574865,"score_gpt":0.229136537173458,"score_spread":0.20746349387770935,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2017596469","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.79120123,0.0000015471384,0.20771688,0.000027289954,0.000054213113,0.0001841206,0.00017516936,0.0000047367043,0.00063478725],"genre_scores_gemma":[0.99827784,0.000004265713,0.0014077128,0.000008329308,0.000051827632,0.0000640974,0.0001044525,0.000009485109,0.000071962095],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.9993685,0.00002691073,0.00030810884,0.00010854039,0.00010175159,0.00008617894],"domain_scores_gemma":[0.9990649,0.00014135781,0.00031711126,0.00025322966,0.00020346187,0.000019933697],"candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.000044028115,0.000077723875,0.00016131297,0.00003758977,0.000050337767,0.0000025684035,0.000092575385,0.00002358674,0.000019002626],"category_scores_gemma":[0.000008059939,0.00006550706,0.00009950599,0.00021259593,0.00006097978,0.00007378696,0.000045950736,0.000047148773,0.000001719972],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00006275127,0.0009089646,0.009010712,0.00003401709,0.000064485386,1.1145311e-7,0.00046910753,0.013508529,0.027884671,0.9446672,0.00009388432,0.0032955448],"study_design_scores_gemma":[0.00067870924,0.00006638287,0.015969668,0.00007016354,0.00009096531,2.1479015e-7,0.000057793102,0.007862327,0.7478684,0.22679201,0.00041508902,0.00012823708],"about_ca_topic_score_codex":0.0046919,"about_ca_topic_score_gemma":0.00020778106,"teacher_disagreement_score":0.71998376,"about_ca_system_score_codex":0.000014690683,"about_ca_system_score_gemma":0.000057640438,"threshold_uncertainty_score":0.7092781},"labels":[],"label_agreement":null},{"id":"W2036310447","doi":"10.1016/j.hedp.2009.12.009","title":"Warm dense matter created by isochoric laser heating","year":2010,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-induced spectroscopy and plasma","field":"Engineering","cited_by":36,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"University of British Columbia","funders":"Lawrence Livermore National Laboratory; U.S. Department of Energy","keywords":"Isochoric process; Warm dense matter; Plasma; Physics; Electron; Laser; Condensed matter physics; State of matter; Atomic physics; Dielectric; Thermodynamic equilibrium; Optics; Quantum mechanics; Thermodynamics","score_opus":0.0034867855942406906,"score_gpt":0.17578596608274702,"score_spread":0.17229918048850634,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2036310447","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.98837787,0.00001077622,0.0064366194,0.000059978283,0.0009040691,0.00003999208,0.000027365162,0.0003930248,0.0037503352],"genre_scores_gemma":[0.99696714,0.000014833537,0.00076536735,0.00036218233,0.00052925514,0.000009760755,0.00012379166,0.000067558925,0.0011601013],"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.9989739,0.000023311974,0.00017584735,0.00025348124,0.00017670915,0.00039671652],"domain_scores_gemma":[0.99934006,0.00007038754,0.00003387194,0.00036822134,0.000052680065,0.00013480963],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00004775203,0.0002630151,0.0002441424,0.00003076773,0.00014404596,0.000063340914,0.00014703353,0.00018302027,0.00021665009],"category_scores_gemma":[0.0000064356036,0.00026893703,0.00007584073,0.00021582235,0.000034827903,0.00016814261,0.00003780971,0.00042285677,0.00040404755],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00002107604,0.00011340415,0.002154449,0.000036364494,0.00011768698,0.000037672467,0.00013593974,0.0051002186,0.9328248,0.009012942,0.049334966,0.0011104633],"study_design_scores_gemma":[0.00028316907,0.000019233794,0.0011074304,0.000010662689,0.00003444424,0.000012584626,0.0000057611956,0.006012166,0.9855412,0.0029962873,0.0035985576,0.00037845355],"about_ca_topic_score_codex":0.000548663,"about_ca_topic_score_gemma":0.00023854617,"teacher_disagreement_score":0.052716434,"about_ca_system_score_codex":0.00004408823,"about_ca_system_score_gemma":0.000012872978,"threshold_uncertainty_score":0.9999763},"labels":[],"label_agreement":null},{"id":"W2053015700","doi":"10.1016/j.hedp.2011.03.005","title":"Radiative effects in radiative shocks in shock tubes","year":2011,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":46,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Simon Fraser University","funders":"","keywords":"Radiative transfer; Shock wave; Shock (circulatory); Radiant energy; Physics; Mechanics; Shock tube; Shock front; Energy transfer; Radiation; Computational physics; Optics; Atomic physics","score_opus":0.009329446825063963,"score_gpt":0.21033616206735267,"score_spread":0.20100671524228872,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2053015700","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.9573523,0.00000943771,0.02441361,0.000020072519,0.0005052168,0.00014468293,0.00003361655,0.00003263502,0.017488474],"genre_scores_gemma":[0.99867874,0.000007318434,0.0005571628,0.00010192624,0.00027382496,0.00005808084,0.00006616573,0.000026064992,0.0002306874],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"observational","domain_scores_codex":[0.9988263,0.00010821236,0.0002473847,0.00033666755,0.00013233922,0.0003490758],"domain_scores_gemma":[0.99910545,0.000400883,0.00007272703,0.00025730816,0.000069028894,0.00009458051],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0000539565,0.00025086582,0.00035463524,0.000104274746,0.00007145854,0.000027944543,0.00014534607,0.00006668834,0.00020789246],"category_scores_gemma":[0.000017556347,0.00025294238,0.00010061282,0.00035410668,0.00006031431,0.00028476893,0.00007783292,0.00025408503,0.00012459279],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"about_ca_topic_candidate":true,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000079193254,0.0012769299,0.30157715,0.0000148151,0.000098383505,0.00006729691,0.0022108806,0.004761548,0.00016260843,0.684916,0.00076573604,0.0040694387],"study_design_scores_gemma":[0.0030785059,0.00025423485,0.57307637,0.00019088243,0.00007796765,0.0000017733886,0.00067762024,0.0073724613,0.16265455,0.2511512,0.000498486,0.0009659543],"about_ca_topic_score_codex":0.017244302,"about_ca_topic_score_gemma":0.0009275023,"teacher_disagreement_score":0.43376485,"about_ca_system_score_codex":0.00010043583,"about_ca_system_score_gemma":0.00006165183,"threshold_uncertainty_score":0.99999225},"labels":[],"label_agreement":null},{"id":"W2058471735","doi":"10.1016/j.hedp.2014.11.007","title":"A novel platform to study magnetized high-velocity collisionless shocks","year":2014,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":17,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Institut National de la Recherche Scientifique","funders":"Grand Équipement National De Calcul Intensif; Labex; Agence Nationale de la Recherche; Lawrence Livermore National Laboratory; U.S. Department of Energy","keywords":"Physics; Plasma; Magnetic field; Acceleration; Computational physics; Electron; Atomic physics; Particle-in-cell; Nuclear physics; Classical mechanics; Quantum mechanics","score_opus":0.011554897070021223,"score_gpt":0.22908351376674496,"score_spread":0.21752861669672374,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2058471735","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.7071264,3.0271443e-7,0.2896334,0.0000681033,0.0005517826,0.00016450747,0.000079798054,0.000062018604,0.002313733],"genre_scores_gemma":[0.99316025,5.8862815e-7,0.0042597847,0.00030130564,0.00091649394,0.000069215734,0.00014700175,0.000040911968,0.0011044777],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"observational","domain_scores_codex":[0.9984031,0.00004332653,0.00032409382,0.00048900774,0.00035068023,0.00038981045],"domain_scores_gemma":[0.9984105,0.0003243068,0.00013902609,0.0005973601,0.0002841537,0.00024464735],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00011284133,0.00032990007,0.00044252357,0.00005928829,0.00037573322,0.00014636706,0.00028404483,0.00006258167,0.00039319316],"category_scores_gemma":[0.000021700971,0.00031333434,0.00012829737,0.00034636416,0.00003750199,0.0001790188,0.00025604968,0.0001952241,0.0003028888],"study_design_candidate":"theoretical_or_conceptual","study_design_consensus":null,"about_ca_topic_candidate":true,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00018232959,0.004958603,0.012525418,0.000009246423,0.0002736368,0.000008396387,0.00036970133,0.009870906,0.001830814,0.9418904,0.004990389,0.02309013],"study_design_scores_gemma":[0.02455731,0.0038757036,0.38335755,0.00024217468,0.0013041872,0.000016210268,0.0027075442,0.023488892,0.2456027,0.25552356,0.053557042,0.0057671266],"about_ca_topic_score_codex":0.013729147,"about_ca_topic_score_gemma":0.00050819694,"teacher_disagreement_score":0.68636686,"about_ca_system_score_codex":0.000055786375,"about_ca_system_score_gemma":0.00005981667,"threshold_uncertainty_score":0.9999319},"labels":[],"label_agreement":null},{"id":"W2073396044","doi":"10.1016/j.hedp.2008.03.001","title":"Evolution of photoionization two-stream instability in collisional plasma","year":2008,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":9,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"University of Alberta","funders":"Deutsches Elektronen-Synchrotron","keywords":"Instability; Physics; Photoionization; Atomic physics; Plasma; Electron; Two-stream instability; Ionization; Ion; Nuclear physics; Quantum mechanics","score_opus":0.008443579630965906,"score_gpt":0.2122355740554735,"score_spread":0.2037919944245076,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2073396044","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.9606623,0.0000016412291,0.036373287,0.0000122931615,0.00023942893,0.00006211906,0.00007979168,0.000018420304,0.0025507128],"genre_scores_gemma":[0.9986946,0.0000042916963,0.0006864586,0.000011155666,0.00018352241,0.0000131888655,0.00020879706,0.000012072654,0.00018594257],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"observational","domain_scores_codex":[0.9990835,0.00004804947,0.000280407,0.00022390971,0.00020120534,0.0001629327],"domain_scores_gemma":[0.9991736,0.00016382277,0.00014501667,0.00023168694,0.00023273879,0.000053128795],"candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.000042704265,0.00013935276,0.00021702623,0.000056582732,0.00012785429,0.0000098430455,0.000084362124,0.00004189023,0.00016619505],"category_scores_gemma":[0.000015723883,0.00014470145,0.00008016987,0.0003682787,0.00009303494,0.00021744551,0.000052662414,0.00010536905,0.000028462786],"study_design_candidate":"observational","study_design_consensus":null,"about_ca_topic_candidate":true,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00007209124,0.0014018794,0.3525249,0.000008838372,0.000030248048,0.0000055779515,0.00011876335,0.059696775,0.0015908054,0.58322746,0.0004955179,0.00082715496],"study_design_scores_gemma":[0.0046386067,0.00020901382,0.46260032,0.00013701226,0.00007700271,0.0000128064485,0.0003210088,0.05280267,0.3481229,0.12875289,0.0014905109,0.0008352467],"about_ca_topic_score_codex":0.011871538,"about_ca_topic_score_gemma":0.00043631234,"teacher_disagreement_score":0.45447457,"about_ca_system_score_codex":0.00011678475,"about_ca_system_score_gemma":0.00014335367,"threshold_uncertainty_score":0.9947085},"labels":[],"label_agreement":null},{"id":"W2086112854","doi":"10.1016/j.hedp.2006.04.001","title":"Bremsstrahlung vs. Thomson scattering in VUV-FEL plasma experiments","year":2006,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-induced spectroscopy and plasma","field":"Engineering","cited_by":24,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"University of Alberta","funders":"","keywords":"Bremsstrahlung; Thomson scattering; Physics; Photon; Plasma; Atomic physics; Scattering; Radiation; Computational physics; Nuclear physics; Optics","score_opus":0.006966081333940832,"score_gpt":0.193036697564156,"score_spread":0.18607061623021517,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2086112854","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.99035925,0.00002924249,0.004491613,0.00002523899,0.0006007243,0.000051806383,0.000010123911,0.00030854106,0.0041234596],"genre_scores_gemma":[0.9981594,0.00002160256,0.0008549108,0.00006320134,0.0005105657,0.000014403797,0.00006778326,0.00005855303,0.00024958455],"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.99874496,0.000027142414,0.00024904782,0.0002911972,0.00021899627,0.00046862572],"domain_scores_gemma":[0.9995353,0.00003787493,0.00003811283,0.00029672586,0.000020512143,0.00007143075],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.0000483949,0.00028749695,0.00029628663,0.00006955488,0.000083881,0.000059362228,0.00016799543,0.00014168407,0.00002050368],"category_scores_gemma":[0.0000018039547,0.00032858664,0.000071109396,0.00024845477,0.00003291793,0.0002424415,0.000049069313,0.00022319538,0.000055382658],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000065866254,0.00025719352,0.004711722,0.000081323444,0.00007045445,0.00018631566,0.00025317556,0.17307192,0.7500734,0.06649777,0.0024921484,0.002238747],"study_design_scores_gemma":[0.0005481285,0.000023942068,0.012024154,0.000047922495,0.000012289982,0.000010490567,0.000011632759,0.018446553,0.9641205,0.0035852073,0.00075079093,0.0004183899],"about_ca_topic_score_codex":0.0016139117,"about_ca_topic_score_gemma":0.0008219391,"teacher_disagreement_score":0.21404713,"about_ca_system_score_codex":0.00017386761,"about_ca_system_score_gemma":0.000015376054,"threshold_uncertainty_score":0.9999166},"labels":[],"label_agreement":null},{"id":"W2589755935","doi":"10.1016/j.hedp.2017.02.003","title":"Detailed characterization of laser-produced astrophysically-relevant jets formed via a poloidal magnetic nozzle","year":2017,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-induced spectroscopy and plasma","field":"Engineering","cited_by":40,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Institut National de la Recherche Scientifique","funders":"Lawrence Livermore National Laboratory; High Magnetic Field Laboratory, Chinese Academy of Sciences; Engineering and Physical Sciences Research Council; Helmholtz-Zentrum Dresden-Rossendorf; National Research Nuclear University MEPhI; Ministry of Education and Science of the Russian Federation; Russian Foundation for Basic Research; Agence Nationale de la Recherche; Deutsche Forschungsgemeinschaft; U.S. Department of Energy","keywords":"Physics; Magnetic field; Plasma; Jet (fluid); Magnetic pressure; Nozzle; Ejecta; Atomic physics; Laser; Optics; Astrophysics; Nuclear physics; Magnetization; Mechanics","score_opus":0.006694936303179534,"score_gpt":0.19090554634191317,"score_spread":0.18421061003873365,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2589755935","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.975435,0.0000033806564,0.023323284,0.000058110763,0.0005908984,0.00009622643,0.000042549804,0.0001620105,0.00028852987],"genre_scores_gemma":[0.9984481,0.00002912701,0.00060698536,0.00003399192,0.0004744054,0.000014466444,0.00014374137,0.00005435938,0.0001948473],"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.99877226,0.000029214936,0.000270166,0.00029535932,0.0002560592,0.00037691614],"domain_scores_gemma":[0.99877775,0.000031385283,0.00016986932,0.0007942696,0.00011312816,0.00011357704],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.000048762886,0.00028185887,0.0004234759,0.00004069088,0.00023759996,0.00007183691,0.00032641206,0.00012798056,0.000025468775],"category_scores_gemma":[0.00002128134,0.00028775382,0.00011760951,0.00009535295,0.00008880411,0.00035300362,0.00008761242,0.00017844136,0.00005269872],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000055215474,0.00009785136,0.00035608525,0.00004961055,0.000051883395,0.000012326787,0.000052388732,0.0007715071,0.98897225,0.0051064044,0.00002308517,0.0044513824],"study_design_scores_gemma":[0.0005429289,0.00013184914,0.042896807,0.000030278388,0.00005591784,0.0000035598534,0.000001879836,0.0107876025,0.9419159,0.0032744047,0.00007014184,0.00028869006],"about_ca_topic_score_codex":0.00013727126,"about_ca_topic_score_gemma":0.00018078568,"teacher_disagreement_score":0.04705632,"about_ca_system_score_codex":0.0000559805,"about_ca_system_score_gemma":0.00003147428,"threshold_uncertainty_score":0.99995744},"labels":[],"label_agreement":null},{"id":"W2886460943","doi":"10.1016/j.hedp.2018.08.001","title":"A Review of Equation-of-State Models for Inertial Confinement Fusion Materials","year":2018,"lang":"en","type":"review","venue":"High Energy Density Physics","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":93,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Université de Montréal; National Research Council Canada","funders":"Lawrence Livermore National Laboratory; NSAF Joint Fund; Los Alamos National Laboratory; National Nuclear Security Administration; Agence Nationale de la Recherche; University of Rochester; Deutsche Forschungsgemeinschaft; Iowa State University; U.S. Department of Energy","keywords":"Inertial confinement fusion; Equation of state; Warm dense matter; Physics; Deuterium; Nuclear physics; Thermodynamics; Plasma","score_opus":0.04522418556236136,"score_gpt":0.2980271471830495,"score_spread":0.25280296162068816,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W2886460943","genre_codex":"review","genre_gemma":"review","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"review","genre_consensus":"review","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.00010513554,0.65884465,0.33221078,0.000019908857,0.0018511728,0.0014450757,0.0043741483,0.00003239559,0.0011167588],"genre_scores_gemma":[0.0010283316,0.99325883,0.0010290318,0.00005193666,0.0007629963,0.00020756383,0.0032991832,0.000049839866,0.0003122828],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"not_applicable","domain_scores_codex":[0.9981906,0.00009198342,0.0010033336,0.00031781258,0.00019424898,0.00020204397],"domain_scores_gemma":[0.9972318,0.00032536057,0.0012840992,0.0004650079,0.00063606707,0.000057671758],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00014766716,0.00036442417,0.0016655434,0.000053860796,0.000070072514,0.000021332804,0.000203261,0.00007995357,0.00036757172],"category_scores_gemma":[0.000018896477,0.00030477473,0.00050965976,0.00016442647,0.000063856765,0.000091787326,0.00012315183,0.00007163383,0.000024527004],"study_design_candidate":"not_applicable","study_design_consensus":null,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.00003756973,0.00077318255,6.6295246e-7,0.09708446,0.00084952125,8.532047e-7,0.000032968383,0.0002629236,0.000081999875,0.51406735,0.020079598,0.3667289],"study_design_scores_gemma":[0.00043777216,0.0001723719,2.2072109e-7,0.08878445,0.002043622,9.0182635e-7,0.0000035580397,0.0002693998,0.011764427,0.027630595,0.8683353,0.00055738],"about_ca_topic_score_codex":0.001401996,"about_ca_topic_score_gemma":0.000009900783,"teacher_disagreement_score":0.8482557,"about_ca_system_score_codex":0.000032099626,"about_ca_system_score_gemma":0.00023030341,"threshold_uncertainty_score":0.99994045},"labels":[],"label_agreement":null},{"id":"W3011668892","doi":"10.1016/j.hedp.2020.100772","title":"Suppressing cross-beam energy transfer with broadband lasers","year":2020,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Laser-Plasma Interactions and Diagnostics","field":"Physics and Astronomy","cited_by":29,"is_retracted":false,"has_abstract":true,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"University of Alberta","funders":"U.S. Department of Energy","keywords":"Laser; Optics; Inertial confinement fusion; Physics; Materials science; Plasma; Filamentation","score_opus":0.00933361441500702,"score_gpt":0.21632676284346555,"score_spread":0.20699314842845853,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W3011668892","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.58015704,0.0000052542164,0.4122359,0.00023528743,0.00024440698,0.000042777123,0.00011924031,0.000101984566,0.0068581295],"genre_scores_gemma":[0.99685127,0.000004666402,0.00032127436,0.0007387563,0.0009516929,0.000014993382,0.000256481,0.000050049563,0.00081079255],"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.99876463,0.000030005496,0.00021000081,0.0004134913,0.000236952,0.00034493647],"domain_scores_gemma":[0.99915665,0.000118251046,0.00006082713,0.00026940965,0.0001563138,0.00023852165],"candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.000017863415,0.00029141438,0.00030164781,0.000021498116,0.00027658342,0.00021661351,0.00016507145,0.000057700814,0.00048618708],"category_scores_gemma":[0.000003274963,0.0002595026,0.00013452527,0.00022875136,0.00011770517,0.0003543812,0.00005016694,0.00017238042,0.000061387385],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.0007546162,0.0013539374,0.0389408,0.000059663987,0.0008838096,0.00013910006,0.00081514136,0.0725247,0.012918288,0.8408061,0.01687554,0.013928281],"study_design_scores_gemma":[0.002207227,0.00025581915,0.0022049798,0.0000649847,0.00019527398,0.0000050157264,0.0001326805,0.0029606416,0.9490737,0.005601496,0.036458567,0.00083966745],"about_ca_topic_score_codex":0.0025749002,"about_ca_topic_score_gemma":0.00008298026,"teacher_disagreement_score":0.9361554,"about_ca_system_score_codex":0.000021720976,"about_ca_system_score_gemma":0.000072067334,"threshold_uncertainty_score":0.9999857},"labels":[],"label_agreement":null},{"id":"W3038898299","doi":"10.1016/j.hedp.2020.100905","title":"Review of the first charged-particle transport coefficient comparison workshop","year":2020,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Nuclear reactor physics and engineering","field":"Engineering","cited_by":86,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"National Research Council Canada","funders":"Sandia National Laboratories; U.S. Department of Energy; Fusion Energy Sciences; Los Alamos National Laboratory; National Nuclear Security Administration; Office of Science; Lawrence Livermore National Laboratory","keywords":"Particle (ecology); Physics; Nuclear physics; Geology","score_opus":0.014872728035201503,"score_gpt":0.1907977014168412,"score_spread":0.17592497338163968,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W3038898299","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.82546455,0.012744334,0.15258747,0.0023149434,0.0014996666,0.00046701,0.00005073571,0.0011842621,0.00368704],"genre_scores_gemma":[0.9982202,0.0008629419,0.000040806746,0.0006684494,0.00015077104,0.0000033415865,0.000009457778,0.00003767492,0.000006340408],"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","domain_scores_codex":[0.9993138,0.0000068788604,0.00020866959,0.00012438418,0.00017372936,0.00017254238],"domain_scores_gemma":[0.9995779,0.000016598991,0.00003997039,0.0002514896,0.000039173374,0.00007486328],"candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.000028757735,0.00014119649,0.0002833096,0.0000043786335,0.00004551353,0.000006510539,0.00018166016,0.00003131766,0.000011223749],"category_scores_gemma":[0.0000047762273,0.00012008318,0.00011581807,0.00035205446,0.000027572154,0.000048991653,0.000033467626,0.00013260111,0.00001091426],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.000025240506,0.00035587494,0.0022905879,0.00917379,0.00034529966,0.000008805447,0.0016956849,0.654716,0.035778377,0.25070447,0.03719248,0.0077134],"study_design_scores_gemma":[0.00074283534,0.00006193252,0.009484407,0.0040915953,0.00027642137,0.0000027407077,0.000053021333,0.4998457,0.21474722,0.00042912632,0.26922074,0.0010442538],"about_ca_topic_score_codex":0.000019507273,"about_ca_topic_score_gemma":0.00000656154,"teacher_disagreement_score":0.25027534,"about_ca_system_score_codex":0.00002227361,"about_ca_system_score_gemma":0.0000071640484,"threshold_uncertainty_score":0.48968503},"labels":[],"label_agreement":null},{"id":"W4402130312","doi":"10.1016/j.hedp.2024.101154","title":"Investigating the suitability of pristine and defective C3N monolayer as supercapacitor electrodes: DFT calculations","year":2024,"lang":"en","type":"article","venue":"High Energy Density Physics","topic":"Supercapacitor Materials and Fabrication","field":"Materials Science","cited_by":4,"is_retracted":false,"has_abstract":false,"route_ca_aff":true,"route_ca_fund":false,"route_ca_venue":false,"route_about_ca":false,"ca_institutions":"Lockheed Martin (Canada)","funders":"King Saud University","keywords":"Monolayer; Electrode; Materials science; Supercapacitor; Capacitance; Charge (physics); Voltage; Vacancy defect; Density functional theory; Capacitor; Optoelectronics; Analytical Chemistry (journal); Condensed matter physics; Nanotechnology; Chemistry; Computational chemistry; Physical chemistry; Electrical engineering; Physics; Organic chemistry","score_opus":0.013464287285352707,"score_gpt":0.23200763225049142,"score_spread":0.21854334496513872,"validation_status":"score_only:v0-immature-baseline","prediction":{"id":"W4402130312","genre_codex":"empirical","genre_gemma":"empirical","domain_codex":null,"domain_gemma":null,"model_version":"codex-gemma-dda1882f352a","genre_candidate":"empirical","genre_consensus":"empirical","domain_candidate":null,"domain_consensus":null,"prediction_status":"machine_predicted_unvalidated","genre_scores_codex":[0.9924615,0.00014163512,0.006409642,0.00016003697,0.00044332832,0.000101368976,0.000023121342,0.000102277285,0.0001570955],"genre_scores_gemma":[0.99855775,0.000015825171,0.00085172965,0.00006563618,0.00042623427,0.000025462949,0.000015668082,0.000018980727,0.000022691422],"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","domain_scores_codex":[0.9987974,0.00017421474,0.00025117456,0.00034760882,0.00022865603,0.00020092372],"domain_scores_gemma":[0.99908984,0.0003037492,0.00005851761,0.00032005762,0.00016978571,0.00005804534],"candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.00032599454,0.00015642267,0.00021791985,0.000026334725,0.00020012938,0.00013179018,0.00012251873,0.00006971914,0.000036705253],"category_scores_gemma":[0.00014610711,0.00011513717,0.000058198282,0.0002391757,0.00026207799,0.00026642854,0.00007653035,0.0000894318,0.000017191045],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_system_candidate":false,"about_ca_system_consensus":false,"study_design_scores_codex":[0.0000052029395,0.000023982819,0.000994885,0.000034413228,0.00001316648,5.3464083e-7,0.0008001232,0.000035057612,0.7967402,0.20098823,0.00005088767,0.00031336158],"study_design_scores_gemma":[0.00007428357,0.000048904625,0.016470479,0.00003518939,0.00005373209,0.000008764247,0.0001194592,0.0010952032,0.9119798,0.06984453,0.00012425847,0.00014538519],"about_ca_topic_score_codex":0.003106726,"about_ca_topic_score_gemma":0.00008038096,"teacher_disagreement_score":0.13114369,"about_ca_system_score_codex":0.000062709594,"about_ca_system_score_gemma":0.00007884546,"threshold_uncertainty_score":0.46964613},"labels":[],"label_agreement":null}]}