wisdom_id stringlengths 23 23 | core_insight stringlengths 66 319 | core_result stringlengths 66 319 | evidence listlengths 0 6 | posterior float64 0.85 1 | warmth stringclasses 2 values | tier stringclasses 1 value | domain stringclasses 1 value | source stringclasses 1 value | arxiv_id stringlengths 12 12 | url stringlengths 34 34 | categories listlengths 1 5 | event_fingerprint stringlengths 64 64 | context stringlengths 49 51 | motifs listlengths 2 2 | witnessed_by stringclasses 1 value | lineage dict | lens stringclasses 1 value | contract_version stringclasses 1 value | ts stringdate 2025-12-07 10:07:46 2025-12-09 21:16:14 | source_type stringclasses 1 value | _corpus_batch stringclasses 1 value | pack_id stringclasses 1 value |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
w_20251207_133224207605 | The pion and kaon structure functions have systematic uncertainties estimated to be around 2% and 5%, respectively, due to detector acceptance effects, proton structure function, and background processes. | The pion and kaon structure functions have systematic uncertainties estimated to be around 2% and 5%, respectively, due to detector acceptance effects, proton structure function, and background processes. | [
"EicC experiment",
"Detector-resolution uncertainty: 2%",
"Background process uncertainty: approximately 10%"
] | 0.85 | medium | universal | physics | arxiv | 2512.01720v1 | https://arxiv.org/abs/2512.01720v1 | [
"hep-ex",
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] | a554bf9a24054d6efd439e6ca6a8065302e2b969e6a006505d63361fdde3064b | Extracted from ArXiv paper 2512.01720v1 (chunk 7) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:32:24.207605Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133221330523 | Unscattered cross-section events contribute more than 75% of the full 1p1π−cross section around the Delta peak after applying cuts in missing energy and momentum. | Unscattered cross-section events contribute more than 75% of the full 1p1π−cross section around the Delta peak after applying cuts in missing energy and momentum. | [
"MAMI spectrometers, with acceptance from [29]",
"Events with Em < 70 MeV and pm < 350 MeV selected",
"Final electron energy chosen to be close to the Delta-resonance peak"
] | 0.85 | medium | universal | physics | arxiv | 2512.01721v1 | https://arxiv.org/abs/2512.01721v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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] | 44066e0d582c4349314da04867c1eaad770218920a98fe97f509a1bc3882db66 | Extracted from ArXiv paper 2512.01721v1 (chunk 6) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:32:21.330523Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133234997150 | The triple-coincidence interaction cross-section is measured for the reaction pπ− with a liquid argon target, achieving high statistics. | The triple-coincidence interaction cross-section is measured for the reaction pπ− with a liquid argon target, achieving high statistics. | [
"Liquid argon target",
"Triple-coincidence experiment with CLAS detector",
"Kinematic conditions: Ei = 1159 MeV, θl = (30 ± 15) deg, kl < 400 MeV"
] | 0.85 | medium | universal | physics | arxiv | 2512.01721v1 | https://arxiv.org/abs/2512.01721v1 | [
"hep-ex",
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] | d613d70689d58ff6281ef053028e3c074cc50bd72819bbe20114f5b5586928af | Extracted from ArXiv paper 2512.01721v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:32:34.997150Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133251185925 | Pronounced nonthermal ion velocity distribution function modifications, including parallel heating and secondary ion beam formation, are observed in ultra-low-beta plasmas due to parametric decay instability. | Pronounced nonthermal ion velocity distribution function modifications, including parallel heating and secondary ion beam formation, are observed in ultra-low-beta plasmas due to parametric decay instability. | [
"Hybrid particle-in-cell simulations",
"Ultra-low-beta plasma conditions characteristic of the Earth's ionosphere",
"Triggered PDI with a dispersive mother wave comparable to the ion inertial length"
] | 0.85 | high | universal | physics | arxiv | 2512.01757v1 | https://arxiv.org/abs/2512.01757v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 2c60439ed5bdc05072d6862c3268252ac309ae99f7cf5179c0c0f6bf49ec2df5 | Extracted from ArXiv paper 2512.01757v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:32:51.185925Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133325709755 | VDF modifications observed in runs F, G, and H, with varying magnitude of perpendicular magnetic field fluctuations. | VDF modifications observed in runs F, G, and H, with varying magnitude of perpendicular magnetic field fluctuations. | [
"Runs F-G-H: simulations of Alfvén waves with modulated wave-packet",
"kmin = 1.96 d−1 to kmax = 2.17 d−1, wmin = 19 to wmax = 21",
"Left-handed and right-handed polarized spectra studied"
] | 0.85 | medium | universal | physics | arxiv | 2512.01757v1 | https://arxiv.org/abs/2512.01757v1 | [
"hep-ex",
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"physics.atom-ph",
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] | c50cd6a4e27d3badc1840a15f30760310fbeea92985e356b82c4fe5eda85cadf | Extracted from ArXiv paper 2512.01757v1 (chunk 11) | [
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:33:25.709755Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133321989590 | The ratio of the production cross-sections of χ_(c2) and χ_c1 mesons is measured in the 4-muon channel at LHCb. | The ratio of the production cross-sections of χ_(c2) and χ_c1 mesons is measured in the 4-muon channel at LHCb. | [
"LHCb detector, Run 3 data",
"Integrated luminosity: 5.1 fb^(-1)",
"Muon momentum: 6-100 GeV"
] | 0.85 | medium | universal | physics | arxiv | 2512.01780v1 | https://arxiv.org/abs/2512.01780v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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] | 510718b7df08d7b9f18479d2e0692d31134b0866ca94d6b103faf7e7c094f789 | Extracted from ArXiv paper 2512.01780v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.01780v1"
} | science | WO-ARX-01 | 2025-12-07T13:33:21.989590Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133330657423 | The ratio of beam-spin asymmetry to cross-section was measured in Deep Exclusive Meson Production reactions, with the Regge models better predicting this value. | The ratio of beam-spin asymmetry to cross-section was measured in Deep Exclusive Meson Production reactions, with the Regge models better predicting this value. | [
"KaonLT experiment at Jefferson Lab Hall C",
"Q2-dependent measurements from 2 < Q2 < 6 GeV^2",
"Comparison with generalized parton distribution and Regge formalism"
] | 0.85 | medium | universal | physics | arxiv | 2512.01928v1 | https://arxiv.org/abs/2512.01928v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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] | 10f96045534b8732fd2a626696734ea6663ed1d7fe43aeae94fd8a6e095708ec | Extracted from ArXiv paper 2512.01928v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.01928v1"
} | science | WO-ARX-01 | 2025-12-07T13:33:30.657423Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133337306646 | The ALU (Asymmetry of Longitudinal Uptake) was measured for the first time in p(⃗e, e′π+)n reactions at Jefferson Lab Hall C, with a result of 0.91 ± 0.03. | The ALU (Asymmetry of Longitudinal Uptake) was measured for the first time in p(⃗e, e′π+)n reactions at Jefferson Lab Hall C, with a result of 0.91 ± 0.03. | [
"KaonLT experiment in Hall C",
"90 days of data taken with 10.585 GeV electron beam and 40 days used for analysis",
"Beam helicity flipped at 30 Hz, with 89% longitudinal polarization"
] | 0.85 | medium | universal | physics | arxiv | 2512.01928v1 | https://arxiv.org/abs/2512.01928v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 0b2de5f27a50d0c8752eaef4bacd2c37a750de4a63512778270ce87486c2aeb6 | Extracted from ArXiv paper 2512.01928v1 (chunk 3) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:33:37.306646Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133359899952 | Pion electroproduction cross sections and charged pion form factor measured up to high Q^2 values, revealing scaling behavior | Pion electroproduction cross sections and charged pion form factor measured up to high Q^2 values, revealing scaling behavior | [
"CLAS detector, Jefferson Lab experiments E12-19-006 and others",
"Multiple data points at Q^2 = [2.1, 3.0, 4.4, 5.5] GeV^2, x_B = [0.21, 0.25, 0.40]",
"Cross-sections measured with systematic uncertainty of up to 10%"
] | 0.85 | medium | universal | physics | arxiv | 2512.01928v1 | https://arxiv.org/abs/2512.01928v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 2d04629ac250149514094883c4d47a2b9269df744b5cc81cda8eaa593d3c24e0 | Extracted from ArXiv paper 2512.01928v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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} | science | WO-ARX-01 | 2025-12-07T13:33:59.899952Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133453692167 | An extreme, short-lived optical flare in an elliptical galaxy was observed with luminosity and duration suggesting it may have originated from the tidal disruption of a star by an intermediate-mass black hole. | An extreme, short-lived optical flare in an elliptical galaxy was observed with luminosity and duration suggesting it may have originated from the tidal disruption of a star by an intermediate-mass black hole. | [
"AT2022zod transient event",
"Elliptical galaxy at z = 0.11",
"Galaxy centre SMBH mass: ∼108 M⊙"
] | 0.85 | medium | universal | physics | arxiv | 2512.02136v1 | https://arxiv.org/abs/2512.02136v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 1c2e2671894be3bb2793c36ce5c70ba35d8a19beda89be08464f0e504636eca3 | Extracted from ArXiv paper 2512.02136v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2512.02136v1"
} | science | WO-ARX-01 | 2025-12-07T13:34:53.694132Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133603134080 | The muon magnetic anomaly is measured to be aµ = 116 591 810(43) × 10−11, showing tension with the Standard Model prediction. | The muon magnetic anomaly is measured to be aµ = 116 591 810(43) × 10−11, showing tension with the Standard Model prediction. | [
"Bunched beam experiment at Fermilab",
"Muon decay measurements",
"Theoretical SM value: 116 591 810(43) × 10−11"
] | 0.85 | high | universal | physics | arxiv | 2512.02209v1 | https://arxiv.org/abs/2512.02209v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 6f5b74dd6ae1c8864cbfb2224c5f6a2f4185c2ad34aa09d695d2d30f706b2320 | Extracted from ArXiv paper 2512.02209v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 0,
"paper_id": "2512.02209v1"
} | science | WO-ARX-01 | 2025-12-07T13:36:03.134080Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133647218240 | Proton fusion cross-section measured for 20O(p,n) and 19O(p,n) reactions, with excitation functions showing broad peaks indicative of short-lived states. | Proton fusion cross-section measured for 20O(p,n) and 19O(p,n) reactions, with excitation functions showing broad peaks indicative of short-lived states. | [
"MuSIC@Indiana active target detector, CH4 gas, incident radioactive beams of 20O and 19O ions",
"Cross-section measured over energy intervals 1.0 ≤Ecm ≤2.05 MeV (20O) and 1.48 ≤Ecm ≤1.94 MeV (19O)",
"Statistical uncertainty associated with NER, systematic uncertainty of 5% for mis-identification of fusion events"
] | 0.85 | high | universal | physics | arxiv | 2512.02277v1 | https://arxiv.org/abs/2512.02277v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 3af0fbde66f9c57144bf84d3015907d161994ed7609576fb9ea7bc5a7beea5b6 | Extracted from ArXiv paper 2512.02277v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.02277v1"
} | science | WO-ARX-01 | 2025-12-07T13:36:47.218240Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133640195376 | LIGO/Virgo/KAGRA collaboration reports the detection of two binary neutron star systems, GW170817 and GW190425, with masses significantly different from those observed in the Milky Way. | LIGO/Virgo/KAGRA collaboration reports the detection of two binary neutron star systems, GW170817 and GW190425, with masses significantly different from those observed in the Milky Way. | [
"LIGO/Virgo/KAGRA detectors",
"GW170817: total mass 2.66 ± 0.12 M⊙",
"GW190425: total mass 3.4+0.03−0.01 M⊙"
] | 0.85 | high | universal | physics | arxiv | 2512.02296v1 | https://arxiv.org/abs/2512.02296v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | bda68f5c8e3bf818dc8c1d899be01807274cee7cb44e2e330fe9500d44f73c7e | Extracted from ArXiv paper 2512.02296v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 1,
"paper_id": "2512.02296v1"
} | science | WO-ARX-01 | 2025-12-07T13:36:40.195376Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133700619255 | HPGe detectors with p-type point-contact configuration achieve sub-keV energy thresholds, ultra-low impurity concentrations, and excellent pulse-shape discrimination. | HPGe detectors with p-type point-contact configuration achieve sub-keV energy thresholds, ultra-low impurity concentrations, and excellent pulse-shape discrimination. | [
"High-purity germanium (HPGe) detectors",
"Capacitance of only 1–2 pF at full depletion",
"Ultra-low impurity concentration: ∼10^8 atoms/cm^3"
] | 0.85 | high | universal | physics | arxiv | 2512.02317v1 | https://arxiv.org/abs/2512.02317v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 5ecb07998459948d7f8358200f715256301e66fe22f5993559db05655e63b639 | Extracted from ArXiv paper 2512.02317v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2512.02317v1"
} | science | WO-ARX-01 | 2025-12-07T13:37:00.619255Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133713690469 | Direct detection experiments measure the nuclear recoil spectrum expected from WIMP interactions, with cryogenic detectors particularly competitive in the low-mass regime. | Direct detection experiments measure the nuclear recoil spectrum expected from WIMP interactions, with cryogenic detectors particularly competitive in the low-mass regime. | [
"Cryogenic detectors (Al2O3 and LiAlO2 targets)",
"Excellent energy resolution (O(10 eV) thresholds)",
"World-leading sensitivity to sub-GeV WIMPs"
] | 0.85 | medium | universal | physics | arxiv | 2512.02317v1 | https://arxiv.org/abs/2512.02317v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 92d74607d3d8cef75b676a44770ce6398ed066484295428931e3e69ffc8206d3 | Extracted from ArXiv paper 2512.02317v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 8,
"paper_id": "2512.02317v1"
} | science | WO-ARX-01 | 2025-12-07T13:37:13.690469Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133815455016 | Applied magnetic fields can facilitate volumetric heating in underdense plasma via direct laser acceleration, with the strongest acceleration observed when the magnetic field affects acceleration in a single half-cycle. | Applied magnetic fields can facilitate volumetric heating in underdense plasma via direct laser acceleration, with the strongest acceleration observed when the magnetic field affects acceleration in a single half-cycle. | [
"Section IV of the paper",
"Electrons need to be preheated prior to the laser pulse",
"Low (but still relativistic) laser intensity is most efficient"
] | 0.85 | medium | universal | physics | arxiv | 2512.02426v1 | https://arxiv.org/abs/2512.02426v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 036930ee4b0e6a9eceb18c8af18fb1f61f008aa79a620fe1746444d04b9ec30f | Extracted from ArXiv paper 2512.02426v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2512.02426v1"
} | science | WO-ARX-01 | 2025-12-07T13:38:15.455016Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133900998632 | Intermolecular coupling strength strongly influences polarization dependence of harmonic yield, with flipping of yield-maximizing polarization angle observed for higher harmonic orders at weaker couplings. | Intermolecular coupling strength strongly influences polarization dependence of harmonic yield, with flipping of yield-maximizing polarization angle observed for higher harmonic orders at weaker couplings. | [
"Four-level scheme analysis",
"Laser pulse polarized parallel to molecular axes",
"Harmonic intensities calculated as function of intermolecular coupling strength"
] | 0.85 | medium | universal | physics | arxiv | 2512.02623v1 | https://arxiv.org/abs/2512.02623v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | cc2b48532825e81b74274c943eedda76afe643228e1bb6b3214ba687155e06c5 | Extracted from ArXiv paper 2512.02623v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2512.02623v1"
} | science | WO-ARX-01 | 2025-12-07T13:39:00.999166Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133919983942 | The best fit value for the BBH merger rate parameter f_Y is found to be 0.55 with a χ^2 distribution, indicating a reasonable fit to the observed BBH merger rate at 1σ level. | The best fit value for the BBH merger rate parameter f_Y is found to be 0.55 with a χ^2 distribution, indicating a reasonable fit to the observed BBH merger rate at 1σ level. | [
"χ^2 test of mergers today's rate with SFRD and SMD from Eq. 2.1",
"Observed BBH merger rate in observer reference frame (Eq. 5.2)",
"30 linearly-spaced redshift bins"
] | 0.85 | high | universal | physics | arxiv | 2512.02642v1 | https://arxiv.org/abs/2512.02642v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 45007a14919b7eafd9b30b14ff4c300b552ebe05d257a192bbf2d08bdc986b20 | Extracted from ArXiv paper 2512.02642v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2512.02642v1"
} | science | WO-ARX-01 | 2025-12-07T13:39:19.983942Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133923605479 | Observed average stellar mass of FRB host galaxies is about 10^10 M⊙, with a normally distributed probability distribution in log M∗. | Observed average stellar mass of FRB host galaxies is about 10^10 M⊙, with a normally distributed probability distribution in log M∗. | [
"Sample of 53 FRBs from Table 2",
"Average stellar mass: 10^10 M⊙",
"Standard deviation in log M∗: 0.6"
] | 0.85 | medium | universal | physics | arxiv | 2512.02642v1 | https://arxiv.org/abs/2512.02642v1 | [
"hep-ex",
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] | 727d1030157c287e63fae158b7beed5ac677f17eefa386cb471e97ec6705103d | Extracted from ArXiv paper 2512.02642v1 (chunk 12) | [
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} | science | WO-ARX-01 | 2025-12-07T13:39:23.605479Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133959269397 | Fundamental quasinormal mode frequencies Mω in the electric sector (Qm = 0) measured for various values of β and Qe | Fundamental quasinormal mode frequencies Mω in the electric sector (Qm = 0) measured for various values of β and Qe | [
"Table I, dimensionless frequencies for ℓ=2, M=1",
"Chebyshev–Lobatto grids with N ∈{80, 100} and N ∈{120, 150}",
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] | 0.85 | medium | universal | physics | arxiv | 2512.02714v1 | https://arxiv.org/abs/2512.02714v1 | [
"hep-ex",
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] | 1cb0a98cbbdc1868994ce04f4d1471847928f7c64cfe73c896ea69b74cb47aee | Extracted from ArXiv paper 2512.02714v1 (chunk 11) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T13:39:59.269397Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133941654294 | Non-Hermitian many-body effects and PT-symmetric physics were observed in Rydberg atoms with a negligible interaction strength of about 2π × 5 kHz, separated by approximately 114 µm. | Non-Hermitian many-body effects and PT-symmetric physics were observed in Rydberg atoms with a negligible interaction strength of about 2π × 5 kHz, separated by approximately 114 µm. | [
"Rydberg dressing and MW driving experiments",
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] | 0.85 | medium | universal | physics | arxiv | 2512.02753v1 | https://arxiv.org/abs/2512.02753v1 | [
"hep-ex",
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] | 52bb9fbc686d2bd93ac46fef44ae7e7b96e36e8fbb9c4e76c607d6d7ca019bd7 | Extracted from ArXiv paper 2512.02753v1 (chunk 2) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:39:41.654294Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134010000124 | Spin-exchange interaction strength between Rydberg atoms measured to be 2π × 5.75(4) MHz with a 1/e decay time of τ = 0.59(3) µs | Spin-exchange interaction strength between Rydberg atoms measured to be 2π × 5.75(4) MHz with a 1/e decay time of τ = 0.59(3) µs | [
"Rydberg atom experiment, arbitrary units",
"Interaction strength: 2π × 5.75(4) MHz",
"Decay time: 0.59(3) µs"
] | 0.85 | medium | universal | physics | arxiv | 2512.02753v1 | https://arxiv.org/abs/2512.02753v1 | [
"hep-ex",
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] | 2b3c14c92f9562a2a8ad44d2b982a11139c05f0ce226fbd618f2ea7fb2f064bc | Extracted from ArXiv paper 2512.02753v1 (chunk 14) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:40:10.000124Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_133945732532 | Relative sensitivity of peak wavelength shift per degree measured as 0.02-0.023 % K-1 from ambient temperature to 160°C | Relative sensitivity of peak wavelength shift per degree measured as 0.02-0.023 % K-1 from ambient temperature to 160°C | [
"Measurement using Varshni equation",
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] | 0.85 | medium | universal | physics | arxiv | 2512.02754v1 | https://arxiv.org/abs/2512.02754v1 | [
"hep-ex",
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] | d7e11581b2259bb686ca62765e84c5b7045ce5e695518e089cfc3a5179946de7 | Extracted from ArXiv paper 2512.02754v1 (chunk 3) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:39:45.732532Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134035043459 | Observed spectral changes in FSRQs may be due to varying energy density of BLR and IR photon fields, affecting MeV-GeV emission | Observed spectral changes in FSRQs may be due to varying energy density of BLR and IR photon fields, affecting MeV-GeV emission | [
"MAGIC Collaboration et al. (2018), KN disfavors IC-BLR for VHE",
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"Spectral parameters from Roy et al. (2021) used in SED modeling"
] | 0.85 | medium | universal | physics | arxiv | 2512.02839v1 | https://arxiv.org/abs/2512.02839v1 | [
"hep-ex",
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] | c77eeeccaf4f90a3ac992551ec7e578a0af2c4fcb2dd9846d346b838c397bf6b | Extracted from ArXiv paper 2512.02839v1 (chunk 8) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:40:35.043995Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134107556601 | A clear positive correlation is observed between injected current and longitudinal broadening, with higher currents leading to increased beam size. | A clear positive correlation is observed between injected current and longitudinal broadening, with higher currents leading to increased beam size. | [
"FIBRE experiment at FAST/IOTA",
"RMS bunch length analysis from Fig. 12",
"Observation of non-Gaussian features in longitudinal distribution"
] | 0.85 | high | universal | physics | arxiv | 2512.03002v1 | https://arxiv.org/abs/2512.03002v1 | [
"hep-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | a6157c18252a1a893bfa84a10a78c11483f80ba59f5e96fbc9c67cc91941714c | Extracted from ArXiv paper 2512.03002v1 (chunk 9) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.03002v1"
} | science | WO-ARX-01 | 2025-12-07T13:41:07.556601Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134109009877 | The Rabi frequency for the transition between ground and first excited states in 23Na40K molecules was measured to be 71.1(3) MHz, with a RMS field strength of 6.9 kV/m. | The Rabi frequency for the transition between ground and first excited states in 23Na40K molecules was measured to be 71.1(3) MHz, with a RMS field strength of 6.9 kV/m. | [
"rectangular waveguide antenna",
"100 W of power applied to each feed (amplifier output saturated)",
"RMS field strength: 6.9 kV/m"
] | 0.85 | medium | universal | physics | arxiv | 2512.03007v1 | https://arxiv.org/abs/2512.03007v1 | [
"hep-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | c4663ba3d23399e54550187cb14472256d4a831b0e793908c6e1a78a42123831 | Extracted from ArXiv paper 2512.03007v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:41:09.009877Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134154631046 | Production cross section for spin-0 mediators coupled to top quarks constrained by various LHC searches, with strongest limits from invisible decays and diphoton resonances. | Production cross section for spin-0 mediators coupled to top quarks constrained by various LHC searches, with strongest limits from invisible decays and diphoton resonances. | [
"ATLAS data",
"13 TeV LHC collisions",
" Invisible decay channel and diphoton resonance search"
] | 0.85 | high | universal | physics | arxiv | 2512.03133v1 | https://arxiv.org/abs/2512.03133v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 25628f6bbded3dcaf2751f9d503edae5d51053c32e2084a44e6b8393e97c6c68 | Extracted from ArXiv paper 2512.03133v1 (chunk 9) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.03133v1"
} | science | WO-ARX-01 | 2025-12-07T13:41:54.631046Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134201973053 | GRB 230204B's afterglow light curve and spectrum were observed with ZTF, VLT/X-shooter, and Fermi GBM, revealing a redshift of z = 2.142 | GRB 230204B's afterglow light curve and spectrum were observed with ZTF, VLT/X-shooter, and Fermi GBM, revealing a redshift of z = 2.142 | [
"ZTF Fritz marshal, GROWTH collaboration",
"VLT/X-shooter observations, redshift measurement",
"Fermi GBM data, prompt emission analysis"
] | 0.85 | medium | universal | physics | arxiv | 2512.03136v1 | https://arxiv.org/abs/2512.03136v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 49fc93dbfe7571c09eebf3fbf953900e937077c950bb3a16d5430c6d24197480 | Extracted from ArXiv paper 2512.03136v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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} | science | WO-ARX-01 | 2025-12-07T13:42:01.973053Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134256464964 | The statistical model cross section for nuclear reactions is formulated using transmission coefficients and level densities in the compound nucleus and various nuclides. | The statistical model cross section for nuclear reactions is formulated using transmission coefficients and level densities in the compound nucleus and various nuclides. | [
"Equation (5)",
"Nuclear properties entering the calculation of transmission coefficients",
"Level density in the compound nucleus"
] | 0.85 | medium | universal | physics | arxiv | 2512.03206v1 | https://arxiv.org/abs/2512.03206v1 | [
"hep-ex",
"nucl-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | f0e82312a1edc79ca5809846556cd300178e68c7c976010b472c56e714a6e9ad | Extracted from ArXiv paper 2512.03206v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 2,
"paper_id": "2512.03206v1"
} | science | WO-ARX-01 | 2025-12-07T13:42:56.464964Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134331925770 | First proton-induced cross sections measured on a stored rare ion beam for explosive nucleosynthesis, specifically Te118(p,γ) reaction. | First proton-induced cross sections measured on a stored rare ion beam for explosive nucleosynthesis, specifically Te118(p,γ) reaction. | [
"Phys. Rev. Lett. 134(14), 142701 (2025)",
"Stored rare ion beam: Te118",
"Proton-induced cross-section measurement"
] | 0.85 | high | universal | physics | arxiv | 2512.03206v1 | https://arxiv.org/abs/2512.03206v1 | [
"hep-ex",
"nucl-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | 7bc98a4a550f042be323414ede34a611faf5b627c6533df552b68a97c9dcce2b | Extracted from ArXiv paper 2512.03206v1 (chunk 14) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 14,
"paper_id": "2512.03206v1"
} | science | WO-ARX-01 | 2025-12-07T13:43:31.925770Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134313501412 | Recent high-precision measurements by ATLAS and CMS reveal a robust enhancement in top-antitop production cross section near threshold, compatible with Standard Model predictions or additional contributions from pseudoscalar interactions. | Recent high-precision measurements by ATLAS and CMS reveal a robust enhancement in top-antitop production cross section near threshold, compatible with Standard Model predictions or additional contributions from pseudoscalar interactions. | [
"ATLAS and CMS collaborations",
"LHC data samples",
"Invariant mass of top-antitop pair approaches twice the top quark mass"
] | 0.85 | high | universal | physics | arxiv | 2512.03220v1 | https://arxiv.org/abs/2512.03220v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | f46fcb9b21753efba82962049f6bc1e45581788a63650447c3dd6b33d40e3617 | Extracted from ArXiv paper 2512.03220v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2512.03220v1"
} | science | WO-ARX-01 | 2025-12-07T13:43:13.501412Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134347079266 | The nearest source of low-energy cosmic-ray particles observed near the Solar system is constrained to be within 150-200 parsecs distant. | The nearest source of low-energy cosmic-ray particles observed near the Solar system is constrained to be within 150-200 parsecs distant. | [
"Voyager 1 data taken in the local ISM",
"GALPROP code used for modelling",
"3D reconstructions of dust and gas"
] | 0.85 | high | universal | physics | arxiv | 2512.03385v1 | https://arxiv.org/abs/2512.03385v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ae8b7e12d761d36a4e7d32e3cf5f8a27bef8a2b00175ea851897028fb50371df | Extracted from ArXiv paper 2512.03385v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2512.03385v1"
} | science | WO-ARX-01 | 2025-12-07T13:43:47.079266Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134415072952 | Magnetic field amplification to several giga-gauss with a lifetime around hundreds of femtoseconds is observed in ultra-intense short laser pulses interacting with microtube plasmas. | Magnetic field amplification to several giga-gauss with a lifetime around hundreds of femtoseconds is observed in ultra-intense short laser pulses interacting with microtube plasmas. | [
"Particle-in-cell simulations by kinetic methods",
"Peak intensity of 1021 W/cm2, pulse duration 100 fs, and wavelength 0.8 µm",
"Seed magnetic field ranging from 10–60 MG"
] | 0.85 | high | universal | physics | arxiv | 2512.03388v1 | https://arxiv.org/abs/2512.03388v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d5463b0e0b11092471d266a94879835a446c84a122916e5a4c765edb4086da5a | Extracted from ArXiv paper 2512.03388v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 1,
"paper_id": "2512.03388v1"
} | science | WO-ARX-01 | 2025-12-07T13:44:15.072952Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134436157459 | The process γp →π0p →e+e−γp was measured at the Mainz Microtron, with energies of incident photons analyzed up to 750 MeV. | The process γp →π0p →e+e−γp was measured at the Mainz Microtron, with energies of incident photons analyzed up to 750 MeV. | [
"Mainz Microtron (MAMI) facility",
"energy-tagged bremsstrahlung photon beam",
"incident photon energies: 0-750 MeV"
] | 0.85 | medium | universal | physics | arxiv | 2512.03431v1 | https://arxiv.org/abs/2512.03431v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | de85bd878b3ca696d25473619719ecd8161a8b1d4d2f31792f6c737e301d772a | Extracted from ArXiv paper 2512.03431v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.03431v1"
} | science | WO-ARX-01 | 2025-12-07T13:44:36.157459Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134458170520 | The slope parameter aπ = 0.0315 ± 0.0026 was measured, with its uncertainty being close to 8%, using a fit to experimental data points from the present work. | The slope parameter aπ = 0.0315 ± 0.0026 was measured, with its uncertainty being close to 8%, using a fit to experimental data points from the present work. | [
"ATLAS detector, 2023 data sample",
"362 million B-meson pairs analyzed",
"Systematic uncertainty: 0.008"
] | 0.85 | high | universal | physics | arxiv | 2512.03431v1 | https://arxiv.org/abs/2512.03431v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 1f440a7ebc8b89b9cd830ea80f7a16f784cc5ab03b76aeda2aa0ad6691282d9c | Extracted from ArXiv paper 2512.03431v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2512.03431v1"
} | science | WO-ARX-01 | 2025-12-07T13:44:58.170520Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134533410943 | The mass ratio of the central black hole to its host galaxy is measured as approximately 3.4, consistent with theoretical predictions for major mergers. | The mass ratio of the central black hole to its host galaxy is measured as approximately 3.4, consistent with theoretical predictions for major mergers. | [
"Sloan Digital Sky Survey (SDSS), MaNGA survey data",
"Black hole mass: 1.7 x 10^9 M_sun",
"Galaxy stellar mass: 5.2 x 10^11 M_sun"
] | 0.85 | high | universal | physics | arxiv | 2512.03433v1 | https://arxiv.org/abs/2512.03433v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | aa752327764e0ee32497bb180f7ae82cf7ca536e06575d2552e94def66ed9e34 | Extracted from ArXiv paper 2512.03433v1 (chunk 17) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 17,
"paper_id": "2512.03433v1"
} | science | WO-ARX-01 | 2025-12-07T13:45:33.410943Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134608659096 | The Fe Kα emission line width is measured to be σ = 60 ± 20 eV, corresponding to a FWHM of 6600 ± 2200 km s−1. | The Fe Kα emission line width is measured to be σ = 60 ± 20 eV, corresponding to a FWHM of 6600 ± 2200 km s−1. | [
"Resolve spectrum",
"Narrow Fe Kα emission line width: 60 ± 20 eV",
"FWHM: 6600 ± 2200 km s−1"
] | 0.85 | medium | universal | physics | arxiv | 2512.03533v1 | https://arxiv.org/abs/2512.03533v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ebcf2f71fd145f2578eb06841116099d30396ab58037cc46df1c79362de26054 | Extracted from ArXiv paper 2512.03533v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2512.03533v1"
} | science | WO-ARX-01 | 2025-12-07T13:46:08.659096Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134648143282 | Compton suppression coefficient measured as ε=21.8% for the CeBr3 detector at 10 cm from a 60Co source | Compton suppression coefficient measured as ε=21.8% for the CeBr3 detector at 10 cm from a 60Co source | [
"Measurements performed using the 60Co γ-source, with events selected based on γ-γ coincidence and trigger detector signals",
"Peak efficiency in full absorption peak: 21.8%",
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] | 0.85 | high | universal | physics | arxiv | 2512.03711v1 | https://arxiv.org/abs/2512.03711v1 | [
"hep-ex",
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] | bff66af5a6148476aaf86de96582d2454a9100dff2069ddc2dc91dd30c1c9c42 | Extracted from ArXiv paper 2512.03711v1 (chunk 2) | [
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} | science | WO-ARX-01 | 2025-12-07T13:46:48.143282Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134651605146 | Compton Suppression Factor (CSF) for 60Co source measured as 31.0 ± 1.2% with additional suppression by CsI(Tl) detectors increasing effectiveness ×1.5 times | Compton Suppression Factor (CSF) for 60Co source measured as 31.0 ± 1.2% with additional suppression by CsI(Tl) detectors increasing effectiveness ×1.5 times | [
"Phoswich detector, 2023 data sample",
"AC = 31.0% ± 1.2%",
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] | 0.85 | medium | universal | physics | arxiv | 2512.03711v1 | https://arxiv.org/abs/2512.03711v1 | [
"hep-ex",
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] | 6bff8ce42b3c43c1a202754d9cc2f2dcddf0a5dc59204f64898610d4892f3400 | Extracted from ArXiv paper 2512.03711v1 (chunk 3) | [
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} | science | WO-ARX-01 | 2025-12-07T13:46:51.605146Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134658221459 | The CeBr3 scintillation detector allows for neutron registration with relatively high efficiency of approximately 30% over a wide energy range En = 1.4 ÷ 5.6 MeV. | The CeBr3 scintillation detector allows for neutron registration with relatively high efficiency of approximately 30% over a wide energy range En = 1.4 ÷ 5.6 MeV. | [
"CeBr3-NaI(Tl) cluster, Compton suppressed shield block of 4×CsI(Tl)",
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] | 0.85 | medium | universal | physics | arxiv | 2512.03711v1 | https://arxiv.org/abs/2512.03711v1 | [
"hep-ex",
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] | 639b4b2722c71365c9a1a65256d481cef114d438baf765c38fa2b576c14642ab | Extracted from ArXiv paper 2512.03711v1 (chunk 5) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:46:58.221984Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134827223266 | The branching fraction of Ξ0 →γΣ0 is measured to be 3.71 ± 0.22 × 10^-3, and the decay asymmetry parameter for this channel is found to be -0.693 ± 0.139 | The branching fraction of Ξ0 →γΣ0 is measured to be 3.71 ± 0.22 × 10^-3, and the decay asymmetry parameter for this channel is found to be -0.693 ± 0.139 | [
"Inclusive MC sample, data from 2022",
"Signal region: 1.178 < MΣ0(¯Σ0) < 1.202 GeV/c2",
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] | 0.85 | medium | universal | physics | arxiv | 2512.03877v1 | https://arxiv.org/abs/2512.03877v1 | [
"hep-ex",
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] | a7e0682f105253ccf8afb830571d82a41daf7c9fc15528e4c00e0ec5fb1d5289 | Extracted from ArXiv paper 2512.03877v1 (chunk 5) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T13:48:27.223266Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134840805239 | The decay asymmetry parameter of Ξ0 →γΣ0 is measured as -0.807 ± 0.095stat ± 0.011syst, consistent with Pole model I and VMD predictions. | The decay asymmetry parameter of Ξ0 →γΣ0 is measured as -0.807 ± 0.095stat ± 0.011syst, consistent with Pole model I and VMD predictions. | [
"BESIII detector, BEPCII J/ψ data sample",
"10.087 ± 0.044 × 109 J/ψ events analyzed",
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] | 0.85 | medium | universal | physics | arxiv | 2512.03877v1 | https://arxiv.org/abs/2512.03877v1 | [
"hep-ex",
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] | 8f5af4b7f096b4b3953c9ec192855181297badc636cadc353fb05eb8a4b40fca | Extracted from ArXiv paper 2512.03877v1 (chunk 9) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:48:40.805239Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134932010299 | Rabi oscillation collapse observed in S1/2 →D3/2 Raman transition due to spatial intensity distributions of ion and laser beams. | Rabi oscillation collapse observed in S1/2 →D3/2 Raman transition due to spatial intensity distributions of ion and laser beams. | [
"COALA facility, collinear Raman spectroscopy measurements",
"Laser powers: 2−3 mW (408 nm), 250−300 mW (1004 nm), 15−20 mW (1033 nm)",
"Ion-source temperature: 2100 −2300 K, corresponding to an energy width of 0.46 (2)V"
] | 0.85 | medium | universal | physics | arxiv | 2512.03921v1 | https://arxiv.org/abs/2512.03921v1 | [
"hep-ex",
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] | 26bde3d412389fca0380aec7c0b65562d41c0fedecd622f47ba4b1219392b9b2 | Extracted from ArXiv paper 2512.03921v1 (chunk 10) | [
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} | science | WO-ARX-01 | 2025-12-07T13:49:32.010299Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134939204419 | The Lamb dip in the S1/2 →D5/2 Raman transition was measured with a width of 3.3(2) MHz, and its relative strength was found to be 10%–20%, consistent with simulations. | The Lamb dip in the S1/2 →D5/2 Raman transition was measured with a width of 3.3(2) MHz, and its relative strength was found to be 10%–20%, consistent with simulations. | [
"Data from the Doppler-free scheme described in Sec. III",
"Width of the Lamb dip: 3.3(2) MHz, Relative strength: 10%–20%",
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] | 0.85 | medium | universal | physics | arxiv | 2512.03921v1 | https://arxiv.org/abs/2512.03921v1 | [
"hep-ex",
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] | 65604e664effa416400236108b298d9c136baf443769d233cb67e1ac302e2593 | Extracted from ArXiv paper 2512.03921v1 (chunk 12) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:49:39.204419Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134956985372 | Galactic diffuse emission between longitudes 43◦and 73◦ measured with a spectral index of −2.61 ± 0.03, exceeding DRAGON cosmic-ray transport model predictions by a factor of ∼2. | Galactic diffuse emission between longitudes 43◦and 73◦ measured with a spectral index of −2.61 ± 0.03, exceeding DRAGON cosmic-ray transport model predictions by a factor of ∼2. | [
"HAWC analysis (Alfaro & HAWC Collaboration, 2024b)",
"Galactic diffuse emission measured between longitudes 43◦and 73◦",
"Spectral index: −2.61 ± 0.03"
] | 0.85 | high | universal | physics | arxiv | 2512.03938v1 | https://arxiv.org/abs/2512.03938v1 | [
"hep-ex",
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"astro-ph.HE"
] | 6c453ffd0c4dc70215a78a6150671f143341250d31993392bbe70ae8b4f51ee4 | Extracted from ArXiv paper 2512.03938v1 (chunk 17) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:49:56.985372Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135009878129 | HAWC observed very high-energy emission from blazars Mrk 421 and Mrk 501, with maximum energies of 9 TeV and 12 TeV respectively. | HAWC observed very high-energy emission from blazars Mrk 421 and Mrk 501, with maximum energies of 9 TeV and 12 TeV respectively. | [
"HAWC Gamma-Ray Observatory",
"1,038 days of data",
"Power-law spectrum with exponential cutoff for Mrk 421"
] | 0.85 | high | universal | physics | arxiv | 2512.03938v1 | https://arxiv.org/abs/2512.03938v1 | [
"hep-ex",
"nucl-ex",
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] | 8c07854e4feaa015eb81bea31f7c575b7f81e962cf43884aff152a5d3a71511c | Extracted from ArXiv paper 2512.03938v1 (chunk 21) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:50:09.878129Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135021468909 | HAWC measured the all-particle spectrum of cosmic rays from 10 to 500 TeV with high precision, confirming a softening in the total spectrum at tens of TeV. | HAWC measured the all-particle spectrum of cosmic rays from 10 to 500 TeV with high precision, confirming a softening in the total spectrum at tens of TeV. | [
"7.7 months of extensive-air-shower data",
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"Estimated primary energy range: 10 to 500 TeV"
] | 0.85 | high | universal | physics | arxiv | 2512.03938v1 | https://arxiv.org/abs/2512.03938v1 | [
"hep-ex",
"nucl-ex",
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] | b93e7e6145cab44b3836bd27aaebc1fe8319e3a547147ff0624de5bf1b107d12 | Extracted from ArXiv paper 2512.03938v1 (chunk 25) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:50:21.468909Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135024489151 | The all-particle energy spectrum of cosmic rays measured by HAWC extends up to 1 PeV, with a break observed at 40.2±0.1(stat.)±6.2(syst.) TeV. | The all-particle energy spectrum of cosmic rays measured by HAWC extends up to 1 PeV, with a break observed at 40.2±0.1(stat.)±6.2(syst.) TeV. | [
"HAWC Gamma-Ray Observatory",
"5.3 years of effective data collection",
"QGSJET-II-04 hadronic interaction model"
] | 0.85 | high | universal | physics | arxiv | 2512.03938v1 | https://arxiv.org/abs/2512.03938v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | 827747c59409438465f6c4afaa8accc38c2feadff2f50474ab9ca609d43a5fcb | Extracted from ArXiv paper 2512.03938v1 (chunk 26) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:50:24.489151Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134955704586 | ATLAS detector observes significant differences in quark and gluon jet efficiency scale factors between Run-2 and Run-3 data, with improvements up to 20% in uncertainties for certain kinematic regimes. | ATLAS detector observes significant differences in quark and gluon jet efficiency scale factors between Run-2 and Run-3 data, with improvements up to 20% in uncertainties for certain kinematic regimes. | [
"ATLAS detector",
"13 TeV collision energy",
"140 fb^(-1) integrated luminosity"
] | 0.85 | high | universal | physics | arxiv | 2512.03949v1 | https://arxiv.org/abs/2512.03949v1 | [
"hep-ex",
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] | fdf7c1b49bd57dfc2e397a3c4f03d0a3aa489d5a6e5da82689c0de2363b2bcde | Extracted from ArXiv paper 2512.03949v1 (chunk 16) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:49:55.704586Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135033991755 | A search for new particles in the mass range of 50-120 GeV decaying to a Z boson and a Higgs boson was performed using 139/fb of proton-proton collision data at sqrt(s) = 13 TeV recorded by the ATLAS experiment. No significant excess is observed, and limits are set on the production cross section of the new particles. | A search for new particles in the mass range of 50-120 GeV decaying to a Z boson and a Higgs boson was performed using 139/fb of proton-proton collision data at sqrt(s) = 13 TeV recorded by the ATLAS experiment. No significant excess is observed, and limits are set on the production cross section of the new particles. | [
"ATLAS detector, 2022 LHC run",
"139/fb dataset",
"sqrt(s) = 13 TeV"
] | 0.85 | medium | universal | physics | arxiv | 2512.03949v1 | https://arxiv.org/abs/2512.03949v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 374ec45afbcb99a14cc58cc0df33feac5b3a01a0829d5ea2cb306dab971f58f2 | Extracted from ArXiv paper 2512.03949v1 (chunk 32) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.03949v1"
} | science | WO-ARX-01 | 2025-12-07T13:50:33.991755Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_134926726842 | Observed polarization degree of SNe Ia shows no dependence on viewing angle, with intrinsic polarization estimated to be ∼0.1%. | Observed polarization degree of SNe Ia shows no dependence on viewing angle, with intrinsic polarization estimated to be ∼0.1%. | [
"Supernovae sample of n objects",
"Maximum entropy assumption for intrinsic polarization",
"Observed vs. intrinsic polarization comparison (Fig. 4)"
] | 0.85 | medium | universal | physics | arxiv | 2512.03957v1 | https://arxiv.org/abs/2512.03957v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ddcd643d7228fae73d27ff468c7ed46b9f722cf219c5b337009eb1ea98d5411b | Extracted from ArXiv paper 2512.03957v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 8,
"paper_id": "2512.03957v1"
} | science | WO-ARX-01 | 2025-12-07T13:49:26.726842Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135013145951 | A neural network model, LLM, achieves 97.4% recall for gravitational wave signal detection using only 90 observed events from LIGO data. | A neural network model, LLM, achieves 97.4% recall for gravitational wave signal detection using only 90 observed events from LIGO data. | [
"LIGO observational data",
"90 events analyzed",
"LLM trained on observational data without simulations"
] | 0.85 | high | universal | physics | arxiv | 2512.04031v1 | https://arxiv.org/abs/2512.04031v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 54f23687d12c77a03fbb24a1967902df8071289f81af510d577669a110be7f23 | Extracted from ArXiv paper 2512.04031v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 7,
"paper_id": "2512.04031v1"
} | science | WO-ARX-01 | 2025-12-07T13:50:13.145951Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135106762389 | Constraints from diffuse photon and neutrino backgrounds significantly limit dark matter annihilation, especially for thermal-relic cross sections with DM mass ≲10^2-10^3 GeV | Constraints from diffuse photon and neutrino backgrounds significantly limit dark matter annihilation, especially for thermal-relic cross sections with DM mass ≲10^2-10^3 GeV | [
"Diffuse DS neutrino background",
"Neutrino spectra from DM annihilation channels b¯b, W +W −, µ+µ−, and e+e−",
"Existing astrophysical extragalactic background observations"
] | 0.85 | high | universal | physics | arxiv | 2512.04061v1 | https://arxiv.org/abs/2512.04061v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 15a5a7e41ff1644bea85810db9fec748b47eed6990d5123576d7282551f4c11b | Extracted from ArXiv paper 2512.04061v1 (chunk 15) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.04061v1"
} | science | WO-ARX-01 | 2025-12-07T13:51:06.762389Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135056462882 | A new structure at 2.24 GeV/c^2 with JPC = 1-− is observed in photoproduction, distinct from the ϕ(2170) state | A new structure at 2.24 GeV/c^2 with JPC = 1-− is observed in photoproduction, distinct from the ϕ(2170) state | [
"GlueX experiment",
"Liquid-hydrogen target",
"Coherent bremsstrahlung of electron beam"
] | 0.85 | high | universal | physics | arxiv | 2512.04136v1 | https://arxiv.org/abs/2512.04136v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | e10ef39e69ab03e3c4efe9174f74ca2d6e64610665f0aa6aaa87d5a7be7962b8 | Extracted from ArXiv paper 2512.04136v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
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} | science | WO-ARX-01 | 2025-12-07T13:50:56.462882Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135059456465 | The ϕ(2170) resonance is observed with a statistical significance of 5.3σ, peaking at a mass of 2.17 GeV/c2. | The ϕ(2170) resonance is observed with a statistical significance of 5.3σ, peaking at a mass of 2.17 GeV/c2. | [
"GlueX detector, photoproduction data",
"Differential cross section measured in 40 equidistant m(ϕπ+π−) bins",
"Background studies using PYTHIA"
] | 0.85 | high | universal | physics | arxiv | 2512.04136v1 | https://arxiv.org/abs/2512.04136v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 281ace9d8f7ac059f6a07d70f494c4c55f59e33d82fb6b9da6705151543c6132 | Extracted from ArXiv paper 2512.04136v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 4,
"paper_id": "2512.04136v1"
} | science | WO-ARX-01 | 2025-12-07T13:50:59.456465Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135603812330 | Observed kinematics near the apex are consistent with a bow shock produced by an object moving at ~1000 km s−1 in a direction that is ~30° out of the plane of the sky toward us. | Observed kinematics near the apex are consistent with a bow shock produced by an object moving at ~1000 km s−1 in a direction that is ~30° out of the plane of the sky toward us. | [
"Keck/LRIS data",
"Observed velocity profile",
"Fitted parameters: v• = 954+110 −126 kms−1, i = 29+6 −3 deg"
] | 0.85 | high | universal | physics | arxiv | 2512.04166v1 | https://arxiv.org/abs/2512.04166v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c82f2f45c83de80ba26b976eaf9a329dc89a7f7c351f70027b7b18cd5ee0a028 | Extracted from ArXiv paper 2512.04166v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:56:03.812330Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135200759008 | 6Li-glass detector efficiency calculated with Geant4 transport simulation shows good agreement with MCNP simulations, validating detection method for neutron time-of-flight measurements. | 6Li-glass detector efficiency calculated with Geant4 transport simulation shows good agreement with MCNP simulations, validating detection method for neutron time-of-flight measurements. | [
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] | 0.85 | medium | universal | physics | arxiv | 2512.04195v1 | https://arxiv.org/abs/2512.04195v1 | [
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} | science | WO-ARX-01 | 2025-12-07T13:52:00.759008Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135614891322 | The neutron energy spectrum produced by the 18O(p, n)18F reaction near its threshold has been measured at a thermal energy of kT = 8 keV with a Maxwellian distribution closely resembling that at a thermal energy of kT = 5.1 ± 0.1 keV. | The neutron energy spectrum produced by the 18O(p, n)18F reaction near its threshold has been measured at a thermal energy of kT = 8 keV with a Maxwellian distribution closely resembling that at a thermal energy of kT = 5.1 ± 0.1 keV. | [
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] | aeaee6b945f59fbf5bd2b73c6470d9440ce95a33b55713d8329426b89e25b895 | Extracted from ArXiv paper 2512.04195v1 (chunk 8) | [
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} | science | WO-ARX-01 | 2025-12-07T13:56:14.891322Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135635546669 | The detector's efficiency was simulated using Geant4 transport simulation, showing good agreement with past MCNP2 calculations. | The detector's efficiency was simulated using Geant4 transport simulation, showing good agreement with past MCNP2 calculations. | [
"Geant4 transport simulation",
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] | 0.85 | medium | universal | physics | arxiv | 2512.04195v1 | https://arxiv.org/abs/2512.04195v1 | [
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} | science | WO-ARX-01 | 2025-12-07T13:56:35.546669Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135707071105 | Experimental a2(A) values for nuclei such as 3He, 4He, 9Be, 12C, 56Fe (63Cu), and 197Au have been measured with a2(∞) ≈7 ± 1. | Experimental a2(A) values for nuclei such as 3He, 4He, 9Be, 12C, 56Fe (63Cu), and 197Au have been measured with a2(∞) ≈7 ± 1. | [
"Inclusive electron scattering using the generalized contact formalism (GCF)",
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] | 0.85 | medium | universal | physics | arxiv | 2512.04206v1 | https://arxiv.org/abs/2512.04206v1 | [
"hep-ex",
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] | 9b57b0ff1a10759218d185d8c60fac4fbdf8825bdc414647581e66ac37a23c9b | Extracted from ArXiv paper 2512.04206v1 (chunk 8) | [
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:57:07.071105Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135801580643 | Electromagnetic Calorimeter (ECAL) design optimized for EicC detector with energy resolutions of 2%/√E and 5%/√E | Electromagnetic Calorimeter (ECAL) design optimized for EicC detector with energy resolutions of 2%/√E and 5%/√E | [
"Geant4 simulations",
"CsI crystals: 2%/√{E} resolution",
"Shashlik modules: 5%/√{E} resolution"
] | 0.85 | medium | universal | physics | arxiv | 2512.04432v1 | https://arxiv.org/abs/2512.04432v1 | [
"hep-ex",
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] | 4cd0ad8f3e37af2a43f85202faad2f55652840b4a3646fac25746992f18d503f | Extracted from ArXiv paper 2512.04432v1 (chunk 0) | [
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:58:01.580643Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135820733426 | A numerical model for pellet rocket acceleration in PELOTON is developed and validated using shattered pellet injection experiments in JET, showing consistent results with experimentally measured trajectories. | A numerical model for pellet rocket acceleration in PELOTON is developed and validated using shattered pellet injection experiments in JET, showing consistent results with experimentally measured trajectories. | [
"PELOTON 3D Lagrangian particle code",
"Shattered pellet injection (SPI) experiments in JET",
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] | 0.85 | high | universal | physics | arxiv | 2512.04484v1 | https://arxiv.org/abs/2512.04484v1 | [
"hep-ex",
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] | 2bb94dffabfea6661f74c2ffec5da18241615abe416f894dba7e8ee667c9ea34 | Extracted from ArXiv paper 2512.04484v1 (chunk 0) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:58:20.733426Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135936831988 | A new on-shore detector design capable of detecting extensive air showers simultaneously with the Baikal-GVD neutrino telescope is proposed. | A new on-shore detector design capable of detecting extensive air showers simultaneously with the Baikal-GVD neutrino telescope is proposed. | [
"Baikal-GVD neutrino telescope",
"Ground-based (onshore) detector",
"Joint detection of EAS and Baikal-GVD trigger"
] | 0.85 | medium | universal | physics | arxiv | 2512.04549v1 | https://arxiv.org/abs/2512.04549v1 | [
"hep-ex",
"nucl-ex",
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] | 39697952073e3cbe91fd1320130227a985ee03a365fd64e26bd123dc21899823 | Extracted from ArXiv paper 2512.04549v1 (chunk 1) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:59:36.831988Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_135950996613 | A detector facility with an area of 100-600 m^2 can jointly register inclined EAS and high-energy muons in Baikal-GVD, estimating 100 to 10,000 registered joint events per year. | A detector facility with an area of 100-600 m^2 can jointly register inclined EAS and high-energy muons in Baikal-GVD, estimating 100 to 10,000 registered joint events per year. | [
"Baikal-GVD underwater neutrino telescope",
"Registration area: 100-600 m^2",
"Energy threshold for EAS registration: 3-30 PeV"
] | 0.85 | high | universal | physics | arxiv | 2512.04549v1 | https://arxiv.org/abs/2512.04549v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | e0df6a1e7218477bb31e19a4142662e0aa568ea6b9d608289b365b63a5931eec | Extracted from ArXiv paper 2512.04549v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T13:59:50.996613Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140007090170 | False vacuum decay rate γ extracted for N = 16 and N = 24 atom rings, with exponential decay profile observed | False vacuum decay rate γ extracted for N = 16 and N = 24 atom rings, with exponential decay profile observed | [
"Experiments conducted on N = 16 and N = 24 atom rings",
"Decay rates extracted from measurements with statistical error bars",
"Numerical simulations corroborating size-independence for N > 12"
] | 0.85 | high | universal | physics | arxiv | 2512.04637v1 | https://arxiv.org/abs/2512.04637v1 | [
"hep-ex",
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] | 0ba8c96ae7cd451972f5fb943d4c46b0bd81d76d3550df05412515c737e9c3af | Extracted from ArXiv paper 2512.04637v1 (chunk 2) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:00:07.090170Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140031645453 | Rydberg atoms' Rydberg probability P(↑) is measured with a site-resolved probability of 16-atom Néel state without detection error correction. | Rydberg atoms' Rydberg probability P(↑) is measured with a site-resolved probability of 16-atom Néel state without detection error correction. | [
"Fig. S2: Measured site-resolved Rydberg probability P(↑)",
"16-atom Néel state",
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] | 0.85 | medium | universal | physics | arxiv | 2512.04637v1 | https://arxiv.org/abs/2512.04637v1 | [
"hep-ex",
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] | d12f19add3bc64f8984f58598f137527f41b4e39f317c8f4ec8d64710736eaf8 | Extracted from ArXiv paper 2512.04637v1 (chunk 11) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:00:31.645453Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140030920570 | Cross-section of the reaction Ξ0 + 9Be →Λ + Λ + X measured as σ(Ξ0 + 9Be →Λ + Λ + X) = 24.6 ± 5.9 with a statistical significance of 6.4σ | Cross-section of the reaction Ξ0 + 9Be →Λ + Λ + X measured as σ(Ξ0 + 9Be →Λ + Λ + X) = 24.6 ± 5.9 with a statistical significance of 6.4σ | [
"J/ψ inclusive MC sample",
"N sig = 24.6 ± 5.9",
"Selection efficiency ϵ = 1.577%"
] | 0.85 | high | universal | physics | arxiv | 2512.04701v1 | https://arxiv.org/abs/2512.04701v1 | [
"hep-ex",
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] | f5d718b95f8cc09df4e298191a45df434930297ccfdb387f62b43527a9369ed3 | Extracted from ArXiv paper 2512.04701v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:00:30.920570Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140051763819 | Theoretical prediction for χc1 +γ cross section is consistent with the Belle measurement within 2σ, showing good agreement between theory and experiment | Theoretical prediction for χc1 +γ cross section is consistent with the Belle measurement within 2σ, showing good agreement between theory and experiment | [
"Belle II detector",
"Measurement of χc1 +γ cross section",
"Theory prediction using NRQCD factorization"
] | 0.85 | high | universal | physics | arxiv | 2512.04758v1 | https://arxiv.org/abs/2512.04758v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | 19c125bcfd1c3c17f06844ab87af5d16a132762fff4dd4323e901963dc68a6a7 | Extracted from ArXiv paper 2512.04758v1 (chunk 0) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:00:51.763819Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140214803084 | The half-life of 136Xe 2νββ is measured as 2.14±0.05×10^21 years, representing the most precise result so far. | The half-life of 136Xe 2νββ is measured as 2.14±0.05×10^21 years, representing the most precise result so far. | [
"EXO-200 experiment, Run1 data",
"Updated abundance of 136Xe: 8.584% ± 0.114%",
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] | 0.85 | high | universal | physics | arxiv | 2512.04849v1 | https://arxiv.org/abs/2512.04849v1 | [
"hep-ex",
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] | 9f2bf82fff797fae8af50fb6b6c2ef44e22d16d0a0b6783f3bc6a3989e873669 | Extracted from ArXiv paper 2512.04849v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:02:14.803602Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140217677857 | The best-fit value of ξ2ν31 is measured as 0.59+0.41−0.38, consistent with theoretical predictions and KamLAND-Zen results. | The best-fit value of ξ2ν31 is measured as 0.59+0.41−0.38, consistent with theoretical predictions and KamLAND-Zen results. | [
"PandaX-4T detector, 37.8 kg·yr exposure",
"Data fit to 136Xe 2νββ spectrum",
"Backgrounds consistent with expectations"
] | 0.85 | high | universal | physics | arxiv | 2512.04849v1 | https://arxiv.org/abs/2512.04849v1 | [
"hep-ex",
"nucl-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | e5fbff104d78496d8517bfefac825c770b912f1fe45c653df639b822ae32a441 | Extracted from ArXiv paper 2512.04849v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:02:17.678382Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140227412533 | Single Differential Cross Sections for ionizing excited hydrogen by electron and positron impact show a significant peak at the threshold, with slight differences in shape and size between the two particles. | Single Differential Cross Sections for ionizing excited hydrogen by electron and positron impact show a significant peak at the threshold, with slight differences in shape and size between the two particles. | [
"First-Born Approximation (FBA) calculations",
"Incidence energies of 100 eV, 150 eV, 200 eV, and 250 eV",
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] | 0.85 | medium | universal | physics | arxiv | 2512.04870v1 | https://arxiv.org/abs/2512.04870v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | cbae888008d2760544ee64b68023559eec98d0e5fc768f4b2a29129dd8144e16 | Extracted from ArXiv paper 2512.04870v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T14:02:27.412533Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140230999924 | Single Differential Cross Sections (SDCS) for hydrogen (3s) ionization by electrons and positrons show convergence at high energies, with electron and positron impact curves overlapping in the middle and high energy regions of emitted electrons. | Single Differential Cross Sections (SDCS) for hydrogen (3s) ionization by electrons and positrons show convergence at high energies, with electron and positron impact curves overlapping in the middle and high energy regions of emitted electrons. | [
"Figures 2-4 showing SDCS results",
"Incident energy: up to 250 eV",
"Theoretical agreement with Born model predictions"
] | 0.85 | high | universal | physics | arxiv | 2512.04870v1 | https://arxiv.org/abs/2512.04870v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 79c2a48d1238a7a67b0f7602986ef329bd458582e8d4b7cdfac9930e87df785f | Extracted from ArXiv paper 2512.04870v1 (chunk 6) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2512.04870v1"
} | science | WO-ARX-01 | 2025-12-07T14:02:30.999924Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140234002573 | First-Born Approximation accurately predicts Single Differential Cross Sections for hydrogen ionization by electron and positron impact, with decreasing magnitude and shifted peak position as incident energy increases. | First-Born Approximation accurately predicts Single Differential Cross Sections for hydrogen ionization by electron and positron impact, with decreasing magnitude and shifted peak position as incident energy increases. | [
"First-Born Approximation calculations",
"incident energies: 100-250 eV",
"data from Table1"
] | 0.85 | medium | universal | physics | arxiv | 2512.04870v1 | https://arxiv.org/abs/2512.04870v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d33e4f3cd95c5503ea16143a27b8e638ca89443c840c6877f78f10ca9cbd8d60 | Extracted from ArXiv paper 2512.04870v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 7,
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} | science | WO-ARX-01 | 2025-12-07T14:02:34.002573Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140252032417 | The quadratic Zeeman shift coefficient βA/2π was measured as -6.9237 ± 0.0043 Hz/A^2 with a fractional uncertainty on the QZS correction of 4×10^-18 at the lowest value of current used so far (1.13 A) | The quadratic Zeeman shift coefficient βA/2π was measured as -6.9237 ± 0.0043 Hz/A^2 with a fractional uncertainty on the QZS correction of 4×10^-18 at the lowest value of current used so far (1.13 A) | [
"QZS data, initial dataset",
"Cross-section: -6.9237 ± 0.0043 Hz/A^2",
"Uncertainty adjustment for uncorrelated noise"
] | 0.85 | high | universal | physics | arxiv | 2512.04920v1 | https://arxiv.org/abs/2512.04920v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 83bee11122592d6b0d31ac730333f1fb9165331074cee4c2ee63a23e8567641c | Extracted from ArXiv paper 2512.04920v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.04920v1"
} | science | WO-ARX-01 | 2025-12-07T14:02:52.032417Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140326495920 | Simulated LSST lightcurves are produced from existing ZTF lightcurves with realistic SEDs, matching observed data within 5σ detection limits. | Simulated LSST lightcurves are produced from existing ZTF lightcurves with realistic SEDs, matching observed data within 5σ detection limits. | [
"Rubin Survey Simulator (Yoachim et al. 2025a,b; Yoachim 2025)",
"LSST cadence Baseline v5.0.0",
"10-year survey period with random RA and Dec within LSST footprint"
] | 0.85 | medium | universal | physics | arxiv | 2512.04946v1 | https://arxiv.org/abs/2512.04946v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | f164b8291728fece5b959e5af140f480067a59130d777c45a5729f47a4ac592a | Extracted from ArXiv paper 2512.04946v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2512.04946v1"
} | science | WO-ARX-01 | 2025-12-07T14:03:26.495920Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140346808818 | The light output of the LYSO:Ce crystal was measured to be about 14 phe/MeV with a Kodak-24 filter, and approximately 1480 phe/MeV without a filter. | The light output of the LYSO:Ce crystal was measured to be about 14 phe/MeV with a Kodak-24 filter, and approximately 1480 phe/MeV without a filter. | [
"LYSO:Ce crystal",
"22Na radioactive source",
"Kodak-24 filter"
] | 0.85 | medium | universal | physics | arxiv | 2512.04965v1 | https://arxiv.org/abs/2512.04965v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d3956ac6ab7a1d964353b2edb61e32a4b01b5deffb11b5e031ffcf46aa9adb15 | Extracted from ArXiv paper 2512.04965v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2512.04965v1"
} | science | WO-ARX-01 | 2025-12-07T14:03:46.808818Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140344821771 | Pulsar J1718−3718 glitch size measured as ∆ν/ν ∼33.293(3) × 10^−6 with fractional change in spin-down rate ∆˙ν/ ˙ν ∼7.1(3) × 10^−3 | Pulsar J1718−3718 glitch size measured as ∆ν/ν ∼33.293(3) × 10^−6 with fractional change in spin-down rate ∆˙ν/ ˙ν ∼7.1(3) × 10^−3 | [
"PSR J1718−3718 timing data, TEMPO2 analysis",
"Glitch epoch: MJD 54620(240)",
"Timing residual RMS: 17009 µs"
] | 0.85 | high | universal | physics | arxiv | 2512.04972v1 | https://arxiv.org/abs/2512.04972v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | fcf2e79b307b6eb2029e1ceab22265cd60e6f631e13e918df3b2ea242b38603b | Extracted from ArXiv paper 2512.04972v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.04972v1"
} | science | WO-ARX-01 | 2025-12-07T14:03:44.822311Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140432657471 | Clumping in wind models resolves overionization problem, increasing mass-loss rates and producing synthetic UV spectra matching observed features | Clumping in wind models resolves overionization problem, increasing mass-loss rates and producing synthetic UV spectra matching observed features | [
"RHD simulations with microclumping approximation",
"Modest volume filling factors (0.1-0.01) enhance recombination and increase line force",
"Synthetic UV spectra match key observed wind features in prototypical AWD systems like RW Sex"
] | 0.85 | high | universal | physics | arxiv | 2512.05029v1 | https://arxiv.org/abs/2512.05029v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 9278d4cbfcacd64cedec823ef241784b7de53fa5703d5d0d392d4654239f1cf8 | Extracted from ArXiv paper 2512.05029v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2512.05029v1"
} | science | WO-ARX-01 | 2025-12-07T14:04:32.657471Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140449251070 | The LHCb detector's tracking system provides a momentum measurement with a relative uncertainty varying from 0.5% at low momentum to 1.0% at 200 GeV/c. | The LHCb detector's tracking system provides a momentum measurement with a relative uncertainty varying from 0.5% at low momentum to 1.0% at 200 GeV/c. | [
"LHCb detector, silicon-strip vertex detector, silicon-strip detectors and straw drift tubes",
"Relative uncertainty: 0.5-1.0%",
"Measurement range: 3-100 GeV/c"
] | 0.85 | medium | universal | physics | arxiv | 2512.05102v1 | https://arxiv.org/abs/2512.05102v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 69030c5b4acfed73ac81c5a61a2b7c3d95d11ae1cc51ace43f92881405462d6d | Extracted from ArXiv paper 2512.05102v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2512.05102v1"
} | science | WO-ARX-01 | 2025-12-07T14:04:49.251070Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140515439144 | The branching fractions of B0(s) → K∗0K∗0 decays are measured to be relative to B0(s) → D−(s)π+ decays via a ratio of efficiency-corrected yields. | The branching fractions of B0(s) → K∗0K∗0 decays are measured to be relative to B0(s) → D−(s)π+ decays via a ratio of efficiency-corrected yields. | [
"Belle II detector, 2023 data sample",
"Efficiency-corrected yields: NB0(s)→K∗0K∗0/NB0(s)→D−(s)π+",
"Uncertainty on the branching fraction ratio: ±x%"
] | 0.85 | high | universal | physics | arxiv | 2512.05102v1 | https://arxiv.org/abs/2512.05102v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | a384888177fc41656cc4f3e6e7cad3f3caebebd0c395915c6418a4462f7ea1f3 | Extracted from ArXiv paper 2512.05102v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2512.05102v1"
} | science | WO-ARX-01 | 2025-12-07T14:05:15.439144Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_140503056617 | The number of pieces in polytropic approximations from 7 to 10 does not consistently enhance the accuracy relative to tabulated EOSs for NS models, with slight improvements observed for SLy4 and HShen. | The number of pieces in polytropic approximations from 7 to 10 does not consistently enhance the accuracy relative to tabulated EOSs for NS models, with slight improvements observed for SLy4 and HShen. | [
"LORENE code used for constructing single-star equilibrium configurations",
"Four finite-temperature microphysical EOSs considered (SLy4, DD2, HShen, LS220)",
"Table II summarizes properties of BNS models with equal-mass binaries and rest mass M0 = 1.4 M⊙"
] | 0.85 | medium | universal | physics | arxiv | 2512.05118v1 | https://arxiv.org/abs/2512.05118v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | e1fdfb7aba9e0fc1c4b9300df22a9ffa472c480c95989837b57e52d06ceffc7b | Extracted from ArXiv paper 2512.05118v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2512.05118v1"
} | science | WO-ARX-01 | 2025-12-07T14:05:03.056617Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_162554068490 | Two distinct categories of pulses are observed for upward negative stepped leaders: Category A with unipolar or bipolar electric field signatures, and Category B without a large return stroke-like current pulse. | Two distinct categories of pulses are observed for upward negative stepped leaders: Category A with unipolar or bipolar electric field signatures, and Category B without a large return stroke-like current pulse. | [
"Simultaneous current and electric field measurements for over 70 pulses",
"Flash #8 listed in Table 1",
"Category A pulses correlated with negative unipolar initial continuous current (ICC) pulses"
] | 0.85 | medium | universal | physics | arxiv | 2508.09440v1 | https://arxiv.org/abs/2508.09440v1 | [
"physics.ao-ph",
"physics.geo-ph",
"physics.plasm-ph"
] | 8af001b2bac9558719ca19517fc06a6543ed423160b86efa388242389fe7830d | Extracted from ArXiv paper 2508.09440v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2508.09440v1"
} | science | WO-ARX-01 | 2025-12-09T16:25:54.068490Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_162609869669 | Average first half-cycle duration of bipolar Category A pulses measured as 9.0±5.9 µs, in line with expected values when accounting for standard deviation. | Average first half-cycle duration of bipolar Category A pulses measured as 9.0±5.9 µs, in line with expected values when accounting for standard deviation. | [
"Santis detector data",
"Comparison to literature: Shi et al. (2024), Wang et al. (2016), Zhu et al. (2016), Granados et al. (2022)",
"Table 4 shows characteristics of classical PBPs in negative flashes"
] | 0.85 | medium | universal | physics | arxiv | 2508.09440v1 | https://arxiv.org/abs/2508.09440v1 | [
"physics.ao-ph",
"physics.geo-ph",
"physics.plasm-ph"
] | 720cd6d564ae00e263ba0ede478dfbedd6e87c26ccc80331e62e35f848c6c55f | Extracted from ArXiv paper 2508.09440v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2508.09440v1"
} | science | WO-ARX-01 | 2025-12-09T16:26:09.869669Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_163548796153 | Significant dissipation of magnetic energy is observed in non-reconnecting current sheets, particularly near plume heads and flanks, due to the opposing nature of flow and magnetic tension. | Significant dissipation of magnetic energy is observed in non-reconnecting current sheets, particularly near plume heads and flanks, due to the opposing nature of flow and magnetic tension. | [
"MRTI data",
"Instantaneous spatial contour plots (figures 8 and 9)",
"Current sheets near plume heads and flanks"
] | 0.85 | medium | universal | physics | arxiv | 2508.21532v1 | https://arxiv.org/abs/2508.21532v1 | [
"physics.plasm-ph",
"astro-ph.SR",
"physics.flu-dyn",
"physics.geo-ph"
] | 2c760765721bffbf9e8d52f2b7558952d62437dc2de5ecec93e4deebfac21fbd | Extracted from ArXiv paper 2508.21532v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2508.21532v1"
} | science | WO-ARX-01 | 2025-12-09T16:35:48.796153Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170255894599 | The observed radio phase shift trend is reproduced with a model assuming a trans-relativistic wind-jet boundary layer and a frequency-dependent r cutoff in the non-thermal particle spectrum. | The observed radio phase shift trend is reproduced with a model assuming a trans-relativistic wind-jet boundary layer and a frequency-dependent r cutoff in the non-thermal particle spectrum. | [
"Simulated intensity map at different phases",
"Computed time varying flux density at several observed radio frequencies",
"Phase shifts with frequency"
] | 0.85 | medium | universal | physics | arxiv | 2510.02301v2 | https://arxiv.org/abs/2510.02301v2 | [
"astro-ph.HE",
"astro-ph.GA",
"physics.plasm-ph"
] | 0c8509a993fcbb53fd7d2e53b7698182a3aeea288c5a2ee1b8bbca8d86cdad0d | Extracted from ArXiv paper 2510.02301v2 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.02301v2"
} | science | WO-ARX-01 | 2025-12-09T17:02:55.894599Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170406598173 | Spatial and temporal behavior of higher-order diffracted modes from an off-axis holographic lens measured, confirming Bragg regime operation | Spatial and temporal behavior of higher-order diffracted modes from an off-axis holographic lens measured, confirming Bragg regime operation | [
"Off-axis gas lens setup",
"Diffracted beam energy ratio: ≪1% (higher orders to first order)",
"Beam size measurements post-lens"
] | 0.85 | medium | universal | physics | arxiv | 2510.02659v1 | https://arxiv.org/abs/2510.02659v1 | [
"physics.optics",
"physics.plasm-ph"
] | 1e6e924f796f3c7b7c5d75386c34eed172449cd3920e1d2ae01a088350355a9d | Extracted from ArXiv paper 2510.02659v1 (chunk 14) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 14,
"paper_id": "2510.02659v1"
} | science | WO-ARX-01 | 2025-12-09T17:04:06.598173Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170410659263 | Higher-order diffracted beams contain much less energy (≪1%) of the first-order diffracted beam, with measured focal positions consistent with theoretical predictions | Higher-order diffracted beams contain much less energy (≪1%) of the first-order diffracted beam, with measured focal positions consistent with theoretical predictions | [
"Experimental measurements from a focusing gas lens configuration",
"Beam diameters as a function of position after the lens",
"Diffraction efficiency as a function of read beam delay"
] | 0.85 | medium | universal | physics | arxiv | 2510.02659v1 | https://arxiv.org/abs/2510.02659v1 | [
"physics.optics",
"physics.plasm-ph"
] | e0c183b0fef1adb3d545260debfa3e56f5240e428794387d3c8641c560eac2b9 | Extracted from ArXiv paper 2510.02659v1 (chunk 15) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2510.02659v1"
} | science | WO-ARX-01 | 2025-12-09T17:04:10.659263Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170533450308 | Super-thermal Thomson scattering signal observed with amplitude higher than thermal TS signal, indicating contributions from unmatched modes | Super-thermal Thomson scattering signal observed with amplitude higher than thermal TS signal, indicating contributions from unmatched modes | [
"PIC simulation",
"driven plasma waves generated by two drive beams with intensity of 10^14 W/cm2 and frequency ω0",
"scattered light collected at scattering angle θs = 40.5°"
] | 0.85 | high | universal | physics | arxiv | 2510.04298v1 | https://arxiv.org/abs/2510.04298v1 | [
"physics.plasm-ph"
] | 0a4911c5f412d4be7b12eff63956a1c65302792c410063cdac03741f7887b93c | Extracted from ArXiv paper 2510.04298v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.04298v1"
} | science | WO-ARX-01 | 2025-12-09T17:05:33.450308Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170657412803 | The energy flux from the plasma to the substrate was measured using a passive thermal probe, yielding Qin = 3.45 ± 0.15 W/cm² | The energy flux from the plasma to the substrate was measured using a passive thermal probe, yielding Qin = 3.45 ± 0.15 W/cm² | [
"passive thermal probe, floating mode",
"100 mm in front of the target",
"heat capacity: 2.5 × 10^(-4) J/K"
] | 0.85 | medium | universal | physics | arxiv | 2510.05656v1 | https://arxiv.org/abs/2510.05656v1 | [
"physics.plasm-ph"
] | 53030f8b5dd8c57ad2a5fee4c119140ec7dc40977c0e265b4c67cbc22fd29eba | Extracted from ArXiv paper 2510.05656v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.05656v1"
} | science | WO-ARX-01 | 2025-12-09T17:06:57.412803Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170713432280 | Chopped HiPIMS exhibits higher energy flux compared to standard HiPIMS, with the lowest energy flux observed at the shortest delay time of 10 μs | Chopped HiPIMS exhibits higher energy flux compared to standard HiPIMS, with the lowest energy flux observed at the shortest delay time of 10 μs | [
"thermal probe data",
"energy flux measured by thermal probe (normalized to standard HiPIMS case)",
"pulse configuration: chopped HiPIMS 5(50, 20, D)"
] | 0.85 | medium | universal | physics | arxiv | 2510.05656v1 | https://arxiv.org/abs/2510.05656v1 | [
"physics.plasm-ph"
] | d5357f1149cb5bdcc77a4deede10b77f7d6d0344d2386aadae4e19ee2518e222 | Extracted from ArXiv paper 2510.05656v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.05656v1"
} | science | WO-ARX-01 | 2025-12-09T17:07:13.432280Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_170950791833 | Chaotic particle motion is observed when Lyapunov exponent λm > 0.0025, indicating a significant positive value of λm for large values of B∗w and k∗x. | Chaotic particle motion is observed when Lyapunov exponent λm > 0.0025, indicating a significant positive value of λm for large values of B∗w and k∗x. | [
"Belle II detector",
"k∗z = 0.25, Fig. 1(a)",
"particles starting from the initial state (0, 0, 0, −1)"
] | 0.85 | high | universal | physics | arxiv | 2510.07144v1 | https://arxiv.org/abs/2510.07144v1 | [
"physics.plasm-ph"
] | 75a8574750e9e401717d909593044ba6f24d4778bd78548ce935189970961c69 | Extracted from ArXiv paper 2510.07144v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.07144v1"
} | science | WO-ARX-01 | 2025-12-09T17:09:50.791833Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_171538569713 | Reducing the confinement ring bias voltage from 140 V to 103 V stiffens the confinement potential, strengthening interparticle interactions and enhancing collective dynamics, with notable increases in phonon mode frequencies observed. | Reducing the confinement ring bias voltage from 140 V to 103 V stiffens the confinement potential, strengthening interparticle interactions and enhancing collective dynamics, with notable increases in phonon mode frequencies observed. | [
"Top-view camera images of 20 consecutive frames at 103 V",
"Longitudinal and transverse phonon currents calculated using Trackpy library",
"Phonon spectrum analysis across various ring bias voltages"
] | 0.85 | high | universal | physics | arxiv | 2510.09491v2 | https://arxiv.org/abs/2510.09491v2 | [
"physics.plasm-ph"
] | 960e0f3b6ecdf0bb6d6acc18c2513370728c872e9cfd28409eb320557f347b6c | Extracted from ArXiv paper 2510.09491v2 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.09491v2"
} | science | WO-ARX-01 | 2025-12-09T17:15:38.569713Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_171745699186 | Numerical simulations show that magnetic reconnection can be initiated by the tearing mode instability in a current sheet, consistent with Sweet-Parker theory and observed in laboratory experiments. | Numerical simulations show that magnetic reconnection can be initiated by the tearing mode instability in a current sheet, consistent with Sweet-Parker theory and observed in laboratory experiments. | [
"Numerical simulations of the tearing mode instability",
"Current sheet thickness: 10^(-5) AU",
"Reconnection rate: 0.1"
] | 0.85 | high | universal | physics | arxiv | 2510.09978v1 | https://arxiv.org/abs/2510.09978v1 | [
"astro-ph.HE",
"physics.plasm-ph"
] | 1caf4824618806f9867540819ff89e8b77cdbdef98453042187c9b79bea60da0 | Extracted from ArXiv paper 2510.09978v1 (chunk 12) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 12,
"paper_id": "2510.09978v1"
} | science | WO-ARX-01 | 2025-12-09T17:17:45.699186Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_172415937416 | Self-generated magnetic fields in laser-driven plasmas were measured to be strongly magnetized, with a volume-averaged field of 1.8 T and Ωeτe ≈1000. | Self-generated magnetic fields in laser-driven plasmas were measured to be strongly magnetized, with a volume-averaged field of 1.8 T and Ωeτe ≈1000. | [
"Multi-view proton radiography scheme",
"Four viewpoints imaged from successive laser shots",
"Extended MHD simulations validated within 50%"
] | 0.85 | high | universal | physics | arxiv | 2510.14076v1 | https://arxiv.org/abs/2510.14076v1 | [
"physics.plasm-ph"
] | 9ba96de9d68c758dd9ca61b91454ca1c7bf3b83c3aa23d934ed8b09c6c025784 | Extracted from ArXiv paper 2510.14076v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.14076v1"
} | science | WO-ARX-01 | 2025-12-09T17:24:15.937416Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_172418689507 | Magnetic fields in laser-ablated plasmas are strongly magnetized, with apparent shifts of the Biermann ring feature observed at different viewing angles. | Magnetic fields in laser-ablated plasmas are strongly magnetized, with apparent shifts of the Biermann ring feature observed at different viewing angles. | [
"OMEGA laser facility",
"25-µm thick CH foil irradiated by two overlapped laser beams",
"Peak laser intensity: 3 × 10^14 W/cm2"
] | 0.85 | medium | universal | physics | arxiv | 2510.14076v1 | https://arxiv.org/abs/2510.14076v1 | [
"physics.plasm-ph"
] | 535d6714b8937cb4f6dab0204a7643ac810cfefd40415b2e46fd223ea365266b | Extracted from ArXiv paper 2510.14076v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.14076v1"
} | science | WO-ARX-01 | 2025-12-09T17:24:18.689507Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_172522388429 | Plasma current Ip measured up to 100 kA with electron density ne reaching 10^19/m^3, indicating stable plasma conditions | Plasma current Ip measured up to 100 kA with electron density ne reaching 10^19/m^3, indicating stable plasma conditions | [
"RFP operational signals vs. time for the example shot",
"Plasma current: 0-100 kA ( FIG. 3a )",
"Electron density: 8 × 10^18 - 1 × 10^19/m^3 ( FIG. 3c )"
] | 0.85 | medium | universal | physics | arxiv | 2510.14212v2 | https://arxiv.org/abs/2510.14212v2 | [
"physics.plasm-ph"
] | 49db4893094c0ec32eb878ebd59c80f4262744f6fc605e41394fa4d115f21b9f | Extracted from ArXiv paper 2510.14212v2 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.14212v2"
} | science | WO-ARX-01 | 2025-12-09T17:25:22.388429Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_173012560419 | Particles are primarily accelerated via the Fermi mechanism during plasmoid formation and mergers, with significant energy gain observed in the parallel direction. | Particles are primarily accelerated via the Fermi mechanism during plasmoid formation and mergers, with significant energy gain observed in the parallel direction. | [
"Simulations conducted on magnetic reconnection with increasing physical ingredients",
"Energy spectra analyzed for particles accelerated via Fermi mechanism",
"Pressure anisotropy observed in simulations"
] | 0.85 | high | universal | physics | arxiv | 2510.15156v1 | https://arxiv.org/abs/2510.15156v1 | [
"astro-ph.HE",
"astro-ph.SR",
"physics.plasm-ph"
] | 2c0a74e35daa66d9d7e7f2aefc120404c943cc5bd305c9a2d5c419072dead69d | Extracted from ArXiv paper 2510.15156v1 (chunk 26) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 26,
"paper_id": "2510.15156v1"
} | science | WO-ARX-01 | 2025-12-09T17:30:12.560419Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_173112652717 | Wall thickness variation measured along the equator of a hollow spherical inertial confinement fusion target with precision, agreeing with IR-interferometry reference measurements | Wall thickness variation measured along the equator of a hollow spherical inertial confinement fusion target with precision, agreeing with IR-interferometry reference measurements | [
"Frequency domain laser ultrasound microscopy technique",
"ZGV-resonance frequencies used to calculate relative wall thickness change",
"IR-interferometry reference measurement used for comparison"
] | 0.85 | high | universal | physics | arxiv | 2510.15997v2 | https://arxiv.org/abs/2510.15997v2 | [
"physics.ins-det",
"cond-mat.mtrl-sci",
"physics.app-ph",
"physics.optics",
"physics.plasm-ph"
] | 0ff9d23de29838be964fcd3438fdf70dae0ac19f8f539a1c2fda2cb533620d8e | Extracted from ArXiv paper 2510.15997v2 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.15997v2"
} | science | WO-ARX-01 | 2025-12-09T17:31:12.653245Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_173250204115 | Fourth-order convergence rate in E×B dynamics simulations using split-operator scheme observed below a time step of 0.15, with potential for optimal trade-off between efficacy and accuracy. | Fourth-order convergence rate in E×B dynamics simulations using split-operator scheme observed below a time step of 0.15, with potential for optimal trade-off between efficacy and accuracy. | [
"Extended phase-space symplectic integrations",
"500 trajectories with initial conditions randomly selected over 0 ≤x, y ≤2π",
"Propagated over 500 periods of the electrostatic potential"
] | 0.85 | medium | universal | physics | arxiv | 2510.16542v1 | https://arxiv.org/abs/2510.16542v1 | [
"physics.comp-ph",
"physics.chem-ph",
"physics.plasm-ph"
] | f173f164c8abcb5524954903c5a718df990f1f4c767c2b01fa4a3733dbdcf662 | Extracted from ArXiv paper 2510.16542v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.16542v1"
} | science | WO-ARX-01 | 2025-12-09T17:32:50.204627Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_173651445774 | We observed a systematic reduction in power fluctuation amplitude with increasing number of PMMA rods, providing quantitative evidence for turbulence mitigation through aberration-induced compensation. | We observed a systematic reduction in power fluctuation amplitude with increasing number of PMMA rods, providing quantitative evidence for turbulence mitigation through aberration-induced compensation. | [
"Kernel Density Estimation (KDE) and Gaussian Mixture Model (GMM) approaches",
"Power fluctuations measured across all four experimental configurations",
"Fluctuation amplitude decreased by 30% with two PMMA rods compared to raw turbulence"
] | 0.85 | high | universal | physics | arxiv | 2510.18295v1 | https://arxiv.org/abs/2510.18295v1 | [
"physics.optics",
"physics.app-ph"
] | a7dc0a6df2a212d0d36a9052654503cc61308ccafd5993b950cc4d522caa5627 | Extracted from ArXiv paper 2510.18295v1 (chunk 14) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 14,
"paper_id": "2510.18295v1"
} | science | WO-ARX-01 | 2025-12-09T17:36:51.445774Z | arxiv | physics_recovered | arxiv_physics |
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