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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
w_20251207_110700774820
|
Prompt D0 meson RAA measured with 30-50% agreement at high pT, while charm quarks exhibit thermalization in the QGP.
|
Prompt D0 meson RAA measured with 30-50% agreement at high pT, while charm quarks exhibit thermalization in the QGP.
|
[
"ATLAS detector, LHC data",
"pT range: 8-20 GeV and above",
"RAA and v2 measurements"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.24847v1
|
https://arxiv.org/abs/2510.24847v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1e3017de3d5db1fa1a1a339432467c77eec725e7a5edbb8c9e894c60bbe9a55c
|
Extracted from ArXiv paper 2510.24847v1 (chunk 20)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 20,
"paper_id": "2510.24847v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:07:00.774820Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110631593568
|
CEνNS cross-sections measured for various target nuclei, including tungsten and lead, with significantly higher cross sections than lighter nuclei.
|
CEνNS cross-sections measured for various target nuclei, including tungsten and lead, with significantly higher cross sections than lighter nuclei.
|
[
"Reactor neutrino scattering experiment",
"Monochromatic neutrino of 747 keV emitted in the 51Cr decay",
"Cross-section: varying by element"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.25272v1
|
https://arxiv.org/abs/2510.25272v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4d6196f7b276dad5d27f3dd3d18f4d5b7c93ec91258faa6ea31de6a74277c7ee
|
Extracted from ArXiv paper 2510.25272v1 (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": "2510.25272v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:06:31.593568Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110640900279
|
A Li2WO4 detector achieved a 0.50 ± 0.01 keV RMS baseline noise and energy resolution of 2.3 ± 0.2 keV for the 208Tl peak at 510.7 keV
|
A Li2WO4 detector achieved a 0.50 ± 0.01 keV RMS baseline noise and energy resolution of 2.3 ± 0.2 keV for the 208Tl peak at 510.7 keV
|
[
"Li2WO4 detector, calibration with 232Th source over 98 hours",
"Energy resolution measured using gamma-ray peaks (Table 1)",
"Baseline noise and energy resolution also achieved in Ge-LD (Table 2)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.25272v1
|
https://arxiv.org/abs/2510.25272v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9ea4f0318c1e591226abdc4e9ecc7cd83f3a1804b2bf17d6978bcc94ff2e5af5
|
Extracted from ArXiv paper 2510.25272v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.25272v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:06:40.900279Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110752806751
|
CUORE applies two different techniques for thermal gain stabilization, heater-based and calibration-based, to improve detector performance.
|
CUORE applies two different techniques for thermal gain stabilization, heater-based and calibration-based, to improve detector performance.
|
[
"CUORE detector",
"Heater-based and calibration-based methods applied",
"Temperature dependence of pulse amplitudes corrected"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.25720v1
|
https://arxiv.org/abs/2510.25720v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
0dab8904250c12c64d9facb57320c75e0bb2989f20fd413b0dc99b36e303fbcb
|
Extracted from ArXiv paper 2510.25720v1 (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": "2510.25720v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:07:52.806751Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110817891601
|
The energy dependence of the detector response is modeled with a quadratic polynomial near Qββ, with a sigmoid-like rolling function used to transition between low and high energies.
|
The energy dependence of the detector response is modeled with a quadratic polynomial near Qββ, with a sigmoid-like rolling function used to transition between low and high energies.
|
[
"Fits performed on selected subset of peaks in physics data",
"BAT package used for fitting",
"Energy-dependent term Rσ(E) scales across physics data proportionally to calibration data"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.25720v1
|
https://arxiv.org/abs/2510.25720v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e76ffc760064ff62073455119f51b81b3c870dbfa284bf5be4a72d5d9bdd9219
|
Extracted from ArXiv paper 2510.25720v1 (chunk 16)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 16,
"paper_id": "2510.25720v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:08:17.891601Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110844875414
|
Electron temperature and density radial profiles measured with a fast-sweeping Langmuir probe system, showing maximum electron temperatures of 8 eV and densities of 1.3 × 10^14 cm^-3
|
Electron temperature and density radial profiles measured with a fast-sweeping Langmuir probe system, showing maximum electron temperatures of 8 eV and densities of 1.3 × 10^14 cm^-3
|
[
"Fast-sweeping Langmuir probe system used in arc jet facility",
"Electron temperature peaks at ∼12.1 kHz and ∼20.7 kHz, with oscillations possibly caused by arcing",
"Electron density measured with standard deviation calculated on localized segments of 100 data points"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26162v1
|
https://arxiv.org/abs/2510.26162v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1b331ed226e549321d84e082d6d05939ec5f946936681dfaf4694c178efae1c0
|
Extracted from ArXiv paper 2510.26162v1 (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": "2510.26162v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:08:44.875414Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110923066998
|
Temperature inferred via deconvolution of SIF measured at 8.5 keV converges to expected value within ≲10% for most cases, but shows small systematic underestimation
|
Temperature inferred via deconvolution of SIF measured at 8.5 keV converges to expected value within ≲10% for most cases, but shows small systematic underestimation
|
[
"Ray-traced spectra in Fig. 3",
"Scattering angles: 10○(red), 20○(blue), and 150○(orange)",
"Central photon energy defined by intensity-weighted average of spectrometer energy"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26747v1
|
https://arxiv.org/abs/2510.26747v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5466ea30a15c2ae290715a8d03d2f6b6d6037a6fe21b1b79a35e83bedd754dda
|
Extracted from ArXiv paper 2510.26747v1 (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": "2510.26747v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:09:23.066998Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110941047480
|
Temperature discrepancies observed in temperature convergence plots for different scattering angle ratios and crystal shifts, indicating possible effects of non-equilibrium.
|
Temperature discrepancies observed in temperature convergence plots for different scattering angle ratios and crystal shifts, indicating possible effects of non-equilibrium.
|
[
"ITCF ratio analysis",
"Three scattering angle ratios (20°/10°, 150°/10°, 150°/20°) examined with different crystal shifts (-1, -5, -10 mm)",
"Results dependent on Rayleigh weight model and elastic feature"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26747v1
|
https://arxiv.org/abs/2510.26747v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
827c4537f539a496b95109fbef0a08b63050a831b996314d4d9487673f998c63
|
Extracted from ArXiv paper 2510.26747v1 (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": "2510.26747v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:09:41.047480Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111012171545
|
The onset of pressure-driven k-shell delocalization is observed in dense carbon plasmas created by x-ray free-electron laser
|
The onset of pressure-driven k-shell delocalization is observed in dense carbon plasmas created by x-ray free-electron laser
|
[
"Nature 618, 270 (2023)",
"High-precision spectrally resolved x-ray scattering measurements",
"Dense carbon plasma at multimegabar pressures"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26747v1
|
https://arxiv.org/abs/2510.26747v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d95aca4df137a9278bc57431dfdfb691d12a57ad8d0dfe3a1ffcc3fa5881f473
|
Extracted from ArXiv paper 2510.26747v1 (chunk 22)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 22,
"paper_id": "2510.26747v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:12.171545Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111037329807
|
The total cross-section for producing a J/ψ meson associated with an open charm-anticharm pair in pp collisions at √s = 13 TeV is measured to be 585+987−401 nb.
|
The total cross-section for producing a J/ψ meson associated with an open charm-anticharm pair in pp collisions at √s = 13 TeV is measured to be 585+987−401 nb.
|
[
"MG5_aMC implementation",
"Total cross section obtained through 7-point scale variations with µR/F ∈{µ0/2, µ0, 2µ0}",
"Contributions from individual J/ψ Fock states given by Eqs. (6.12) and (6.13)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26773v1
|
https://arxiv.org/abs/2510.26773v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e02dd40924932a7b4b7768ee3c13a26202f6365cae9d2fe585039e84587a2dbb
|
Extracted from ArXiv paper 2510.26773v1 (chunk 18)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 18,
"paper_id": "2510.26773v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:37.329807Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111053252582
|
Quarkonium production cross sections in association with a Higgs boson have been calculated for J/ψ and Υ mesons, showing distinct differences in rapidity distributions due to varying Feynman diagrams.
|
Quarkonium production cross sections in association with a Higgs boson have been calculated for J/ψ and Υ mesons, showing distinct differences in rapidity distributions due to varying Feynman diagrams.
|
[
"pp collisions at √s = 13 TeV",
"13 TeV data sample analyzed using MG5_aMC",
"Differential cross-section distributions shown in figure 4"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26773v1
|
https://arxiv.org/abs/2510.26773v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c660cbcba62b85f5db33f30e6151bdbf172fd341103e9c8635a9171f4427639c
|
Extracted from ArXiv paper 2510.26773v1 (chunk 24)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 24,
"paper_id": "2510.26773v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:53.252582Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111056425396
|
Total cross sections for charmonium and bottomonium production in association with a single jet or a jet pair at √s = 10.58 GeV are measured, ranging from 33.652 fb to 606.9 fb.
|
Total cross sections for charmonium and bottomonium production in association with a single jet or a jet pair at √s = 10.58 GeV are measured, ranging from 33.652 fb to 606.9 fb.
|
[
"Belle II detector",
"Table 11: Total (fiducial) cross sections for charmonium and bottomonium production in association with a single jet (or a jet pair) at √s = 10.58 GeV",
"Numerical uncertainties from the MC phase-space integration"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26773v1
|
https://arxiv.org/abs/2510.26773v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e4d24199f9cf50b8d66ad19c183fd7a20af31c7ba787a0a8167f1f888ec322cc
|
Extracted from ArXiv paper 2510.26773v1 (chunk 27)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 27,
"paper_id": "2510.26773v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:56.425396Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111004147297
|
The dipole amplitude N(r, x) is described by a neural network and the Balitsky-Kovchegov evolution equation to calculate inclusive DIS cross sections with high precision.
|
The dipole amplitude N(r, x) is described by a neural network and the Balitsky-Kovchegov evolution equation to calculate inclusive DIS cross sections with high precision.
|
[
"HERA data",
"Neural network architecture",
"Running coupling corrections"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26779v1
|
https://arxiv.org/abs/2510.26779v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
386054d0d2312703b69dc232f87bcb28c23cece91e413daaf52218bda10d1061
|
Extracted from ArXiv paper 2510.26779v1 (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": "2510.26779v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:04.147297Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111012892169
|
A transformer emulator achieves high accuracy in predicting DIS cross sections, with mean relative error of 0.115% and median error of 0.073%, enabling efficient exploration of the parameter space.
|
A transformer emulator achieves high accuracy in predicting DIS cross sections, with mean relative error of 0.115% and median error of 0.073%, enabling efficient exploration of the parameter space.
|
[
"Deep learning model trained on dipole amplitudes",
"Validation set: ~4 × 10^6 values computed from BK evolution",
"Comparison to theory cross sections at three center-of-mass energies"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26779v1
|
https://arxiv.org/abs/2510.26779v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4e5f8f856934143eab02ab6cbc0f5486364c41b554ba602573ee5042ec073da2
|
Extracted from ArXiv paper 2510.26779v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.26779v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:12.892169Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111029655038
|
The RK ratio in Ar+Sc collisions is measured to be 1.115 ± 0.043 at √sNN = 8.8 GeV, but only the NA61/SHINE preliminary result is 3σ significant.
|
The RK ratio in Ar+Sc collisions is measured to be 1.115 ± 0.043 at √sNN = 8.8 GeV, but only the NA61/SHINE preliminary result is 3σ significant.
|
[
"NA61/SHINE detector",
"RK ratio: 1.115 ± 0.043",
"√sNN = 8.8 GeV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26846v1
|
https://arxiv.org/abs/2510.26846v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ce5f553c6dd9e23c0f7bc67ea568c403df6dc3bc7dad86fadee342148ed5c5aa
|
Extracted from ArXiv paper 2510.26846v1 (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": "2510.26846v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:29.655561Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111048557365
|
The mass distribution of Λ and ¯Λ particles was measured with good agreement between data and signal Monte Carlo simulation.
|
The mass distribution of Λ and ¯Λ particles was measured with good agreement between data and signal Monte Carlo simulation.
|
[
"GlueX experiment, with the BCAL detector",
"Invariant mass distributions shown in Fig. 4(a) and (b)",
"Selections on path-length significance (PLS), invariant mass, and kinematic fit"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26890v1
|
https://arxiv.org/abs/2510.26890v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
8c08d99cc5023d2bda7503c15d03b582df24f842f6573e276374b5b54f3e87e8
|
Extracted from ArXiv paper 2510.26890v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.26890v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:10:48.557891Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111156404717
|
Cross-section variations were observed at the few-percent level in pp and hyperon channels, with a mild increase of about 5% from lowest to highest beam energies.
|
Cross-section variations were observed at the few-percent level in pp and hyperon channels, with a mild increase of about 5% from lowest to highest beam energies.
|
[
"GlueX experiment",
"Variations in cross sections measured across different beam energy bins",
"Systematic uncertainty: ±5%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26890v1
|
https://arxiv.org/abs/2510.26890v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c2a620ef9b6ab1521a61fa84f84816b8b2c6f221d8cd395f97c4ff48b69babc4
|
Extracted from ArXiv paper 2510.26890v1 (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": "2510.26890v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:11:56.404717Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111152658584
|
A high-quality dataset was extracted from the β-gated γ spectrum measured with PARIS, allowing for detailed information on level energies, β transition half-lifes, B(GT) values, and the β decay pattern.
|
A high-quality dataset was extracted from the β-gated γ spectrum measured with PARIS, allowing for detailed information on level energies, β transition half-lifes, B(GT) values, and the β decay pattern.
|
[
"ALTO ISOL facility",
"80Ga beam produced by photo-fission of a uranium carbide target",
"Hybrid array consisting of a cylindrical plastic scintillator, two HPGe detectors, and three PARIS clusters"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.27125v1
|
https://arxiv.org/abs/2510.27125v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6764f4457bde1cd11b9c1ba9ccc67f7f6b3472c7a4124f04ffcaafd04f932816
|
Extracted from ArXiv paper 2510.27125v1 (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": "2510.27125v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:11:52.658584Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111157680089
|
Multi-peak HXR light curve observed in solar flare, with two major peaks at t1 and t3, separated by a local minimum at t2
|
Multi-peak HXR light curve observed in solar flare, with two major peaks at t1 and t3, separated by a local minimum at t2
|
[
"Solar Dynamics Observatory (SDO) data",
"30–50 keV energy band",
"Peaks at 14:15:44 UT (t1) and 14:16:53 UT (t3)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.27162v1
|
https://arxiv.org/abs/2510.27162v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ac29e3f29143d3ca5d0c561c20e88d8ba54cbb845d17c1ddbed293977cd8fd8d
|
Extracted from ArXiv paper 2510.27162v1 (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": "2510.27162v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:11:57.680089Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111250357119
|
Muon veto and low-temperature detectors have been simulated with Geant4 for the CROSS experiment, including three detector configurations
|
Muon veto and low-temperature detectors have been simulated with Geant4 for the CROSS experiment, including three detector configurations
|
[
"Geant4 simulation",
"Muon veto, lead shielding, and low-temperature detectors implemented",
"Three detector configurations: RUN 9, RUN 13, and CROSS"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.27406v1
|
https://arxiv.org/abs/2510.27406v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d50c8a2b4d308fe0eb6f9be2155c2447a4fdb66c0e5775479fb82dee5a50d4ea
|
Extracted from ArXiv paper 2510.27406v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.27406v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:12:50.357119Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111528575428
|
Strong scattering peaks observed at qx = ±8(2π/d) and weaker peaks near integer multiples of (2π/d), corresponding to critical modes and free space modes respectively.
|
Strong scattering peaks observed at qx = ±8(2π/d) and weaker peaks near integer multiples of (2π/d), corresponding to critical modes and free space modes respectively.
|
[
"Fourier transform performed in x-direction for y=z=0",
"peaks at qx = ±8(2π/d)",
"peaks near integer multiples of (2π/d)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.27654v1
|
https://arxiv.org/abs/2510.27654v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4ff0a7621fba3c174028fc6ed84cf419a1fb29a197fc4f135ee765caa95c9d61
|
Extracted from ArXiv paper 2510.27654v1 (chunk 36)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 36,
"paper_id": "2510.27654v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:15:28.575428Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111404752699
|
Improved angular resolution for energy correlator measurements can be achieved using matching calculations between non-perturbative and perturbative detectors, leveraging renormalization group techniques in QCD.
|
Improved angular resolution for energy correlator measurements can be achieved using matching calculations between non-perturbative and perturbative detectors, leveraging renormalization group techniques in QCD.
|
[
"ATLAS collaboration",
"Track-based measurements with theoretical calculations",
"Renormalization group scale dependence"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.00149v1
|
https://arxiv.org/abs/2511.00149v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ff7169caf0ce65320cb39987e0823bf1242ac3e2095afb3441ac3553250b5514
|
Extracted from ArXiv paper 2511.00149v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.00149v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:14:04.753220Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111406531724
|
Ion-wave satellites are observed in laser-solid interaction at the same threshold around each harmonic, with a frequency shift slightly less than that of a nominal ion-plasma wave.
|
Ion-wave satellites are observed in laser-solid interaction at the same threshold around each harmonic, with a frequency shift slightly less than that of a nominal ion-plasma wave.
|
[
"T3 laser at CUOS, University of Michigan",
"400-fs pulses, energies up to 3 J",
"Satellites appear abruptly at the same threshold around each harmonic (3rd through 7th)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00174v1
|
https://arxiv.org/abs/2511.00174v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2eafbbe352e896a5155b3cf43e805f39209c95c2ad661d099032a92450260df6
|
Extracted from ArXiv paper 2511.00174v1 (chunk 0)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.00174v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:14:06.531724Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111428765043
|
The drag resistivity observed at the double neutrality point is positive, with a nonmonotonic temperature dependence.
|
The drag resistivity observed at the double neutrality point is positive, with a nonmonotonic temperature dependence.
|
[
"Double neutrality point",
"Nonzero drag resistivity",
"Temperature range: typically above ∼100 K"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00221v1
|
https://arxiv.org/abs/2511.00221v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6fbb3e10da673ac0b5e9ed3d1ae94cd28b38609956bff2041befdf17da5a07ee
|
Extracted from ArXiv paper 2511.00221v1 (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": "2511.00221v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:14:28.765043Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111431123385
|
Transverse single-spin asymmetries in π0 and η meson production measured in p↑+p collisions at √s = 200 GeV with the sPHENIX detector
|
Transverse single-spin asymmetries in π0 and η meson production measured in p↑+p collisions at √s = 200 GeV with the sPHENIX detector
|
[
"sPHENIX experiment, RHIC Run-24 data sample",
"107 pb−1 of collision data analyzed",
"Efficient high-pT photon trigger used"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2da6b880864102804ee31d2ead21bb13f9f724128595deb58437e4d6de742453
|
Extracted from ArXiv paper 2511.00285v1 (chunk 0)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:14:31.123904Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111449983081
|
Transverse single-spin asymmetries (TSSAs) are observed in polarized proton-proton scattering experiments, including production of charged pions, neutrons, pi0 mesons, K+ and K- mesons, and eta mesons
|
Transverse single-spin asymmetries (TSSAs) are observed in polarized proton-proton scattering experiments, including production of charged pions, neutrons, pi0 mesons, K+ and K- mesons, and eta mesons
|
[
"Argonne National Laboratory experiments",
"Polarized proton-proton collisions at high energies",
"Measured TSSAs independent of center-of-mass energy over two orders of magnitude"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ca0741af07f6ccc359fb531f195dc27beafb5053e1be3f0afb7cb83031d3c952
|
Extracted from ArXiv paper 2511.00285v1 (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": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:14:49.983081Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111608222256
|
The raw asymmetry values for the π0 signal region are measured in bins of pT and φ, with varying uncertainty ranges.
|
The raw asymmetry values for the π0 signal region are measured in bins of pT and φ, with varying uncertainty ranges.
|
[
"ATLAS detector",
"pT ≤ 10 GeV",
"φ-dependent measurements"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a245abce3b34f8fcbdef9ee4e9ecf75ad16264a53ab83766dd85cb11445c0df2
|
Extracted from ArXiv paper 2511.00285v1 (chunk 31)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 31,
"paper_id": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:16:08.222256Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111633332888
|
The beam-averaged asymmetry for the η-meson is measured with systematic uncertainties, with a maximum uncertainty of 0.00107 in certain pT bins.
|
The beam-averaged asymmetry for the η-meson is measured with systematic uncertainties, with a maximum uncertainty of 0.00107 in certain pT bins.
|
[
"Table 6.1, pT-binned values from relative luminosity and geometric methods",
"Calculation method systematic uncertainty: δAsys,calcN = ArellumiN - AgeometricN (Equation 6.1)",
"Background fraction determination using two fitting methods: main analysis and Gaussian Process Regression"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
8e8924beadc74c1c5b73e784c87615a6b60f1b7a6d532e4b3f503ce1d3b12741
|
Extracted from ArXiv paper 2511.00285v1 (chunk 39)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 39,
"paper_id": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:16:33.332888Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111637091731
|
Background fractions for π0 and η-mesons measured in alternative analysis, with systematic uncertainty δAsys,bgN assigned as difference between two calculations.
|
Background fractions for π0 and η-mesons measured in alternative analysis, with systematic uncertainty δAsys,bgN assigned as difference between two calculations.
|
[
"GPR (Gaussian Process Regression) model used on di-photon mass distribution",
"π0 and η-meson signal regions defined within 3-σ and 2-σ windows around peak masses",
"Background yield Nbkgd calculated from GPR predicted means µi, with uncertainty δNbkgd propagated from σi"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
bd6de08513396ca8a7f362811f116d8517cb242be8e70366cd14481510a02db9
|
Extracted from ArXiv paper 2511.00285v1 (chunk 40)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 40,
"paper_id": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:16:37.091731Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111705943703
|
No false asymmetry observed in η and xF binnings, with bunch shuffling systematic uncertainty assigned to all bins due to uniformly greater widths than one.
|
No false asymmetry observed in η and xF binnings, with bunch shuffling systematic uncertainty assigned to all bins due to uniformly greater widths than one.
|
[
"ATLAS detector, data sample",
"72 million p-p collisions analyzed",
"Statistical uncertainties calculated for π0 and η-mesons"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e521203eb8f07d261585a3b72bfdc2a1941af96a264199d908a1ebedc3887519
|
Extracted from ArXiv paper 2511.00285v1 (chunk 49)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 49,
"paper_id": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:17:05.943703Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111741095340
|
Probabilistic dependence of the Blue beam on the x-Feynman bin is measured with a probability of 0.8715, consistent with expected behavior.
|
Probabilistic dependence of the Blue beam on the x-Feynman bin is measured with a probability of 0.8715, consistent with expected behavior.
|
[
"Blue Beam Bunch Shuffling -- x",
"η-meson signal region",
"polarized data"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00285v1
|
https://arxiv.org/abs/2511.00285v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c6056dbe36485a135b8219a0655c875092327564e18ed0588776efb560a4d36a
|
Extracted from ArXiv paper 2511.00285v1 (chunk 60)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 60,
"paper_id": "2511.00285v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:17:41.095340Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111454627122
|
Gross electrode erosion was measured in-situ and surface morphology changes were measured with ex-situ diagnostics on the ZaP-HD SFS Z-pinch device.
|
Gross electrode erosion was measured in-situ and surface morphology changes were measured with ex-situ diagnostics on the ZaP-HD SFS Z-pinch device.
|
[
"ZaP-HD sheared-flow-stabilized Z-pinch device",
"Pinch currents up to 136 kA",
"Graphite electrode subjected to high temperature, high density Z-pinch plasma"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00354v1
|
https://arxiv.org/abs/2511.00354v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3db25f08ac79d91b892c160fae4dc43adfb285302549027cf7958893b9a25495
|
Extracted from ArXiv paper 2511.00354v1 (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": "2511.00354v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:14:54.627122Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111538023170
|
We measured the total number density of dilute alkali vapor using single-pass absorption spectroscopy across a wide range of temperatures, laser beam powers, and different absorption lengths
|
We measured the total number density of dilute alkali vapor using single-pass absorption spectroscopy across a wide range of temperatures, laser beam powers, and different absorption lengths
|
[
"Single-pass Absorption Spectroscopy (SPAS) technique",
"Rubidium D2 transitions modeling with multi-level master equation approach",
"Doppler broadening incorporated into absorption coefficient calculations"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00526v1
|
https://arxiv.org/abs/2511.00526v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
67775e03183a10e1cb149db1d1434a4567e4177a1b4cf9314a3c08f9872b3f0d
|
Extracted from ArXiv paper 2511.00526v1 (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": "2511.00526v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:15:38.023170Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111548532506
|
The prompt v2 of D0, D+, and D+^s mesons is measured for the first time in charm hadrons, showing a remarkable agreement between the v2 values of D0 and D+ mesons.
|
The prompt v2 of D0, D+, and D+^s mesons is measured for the first time in charm hadrons, showing a remarkable agreement between the v2 values of D0 and D+ mesons.
|
[
"ALICE detector data",
"30-50% centrality class",
"pT range: 3 < pT < 8 GeV/c"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.00567v1
|
https://arxiv.org/abs/2511.00567v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
060871a6e05208348b18d00c9af83e2dca5d373e4940f521625a0fb0f36b1f22
|
Extracted from ArXiv paper 2511.00567v1 (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": "2511.00567v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:15:48.532506Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111551787851
|
Prompt and non-prompt Λ+c-baryon v2 is measured in semicentral Pb–Pb collisions at √sNN = 5.36 TeV for the first time at the LHC
|
Prompt and non-prompt Λ+c-baryon v2 is measured in semicentral Pb–Pb collisions at √sNN = 5.36 TeV for the first time at the LHC
|
[
"ALICE detector, 2023 LHC run",
"30-50% centrality class",
"Λ+c-baryon v2 measured with 3.6σ significance splitting from D0 v2"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.00567v1
|
https://arxiv.org/abs/2511.00567v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ab2c8249e4640db60b438dbed88a1bb6aee2351e145618a47ac9e4c7037dbf99
|
Extracted from ArXiv paper 2511.00567v1 (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": "2511.00567v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:15:51.787851Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111559897983
|
Theoretical calculations using the model [9] for the reaction pd →pdππ reproduce the experimental data on differential cross section dσ/dMdπ at proton beam energies Tp = 1.1 and 1.4 GeV
|
Theoretical calculations using the model [9] for the reaction pd →pdππ reproduce the experimental data on differential cross section dσ/dMdπ at proton beam energies Tp = 1.1 and 1.4 GeV
|
[
"pd collision, proton beam kinetic energy 1.1 and 1.4 GeV",
"Deuteron scattering angles: forward (8°-13°) and backward (172°-167°)",
"D03 →dσ and D03 →D12π decay parameters assumed as Γ(2)D03→dσ = 20 MeV and Γ(1)D03→D12π = 90 MeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00587v1
|
https://arxiv.org/abs/2511.00587v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
cf7c04938c82198f5899db6befa86e47c76875bed838980c1cef1820895fc60b
|
Extracted from ArXiv paper 2511.00587v1 (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": "2511.00587v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:15:59.898509Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111603544611
|
Theoretical calculations of differential cross sections for reactions pd →pdππ and dd →ddππ are consistent with experimental data, except at high energies where the theoretical curve overestimates the data by a factor of 1.7.
|
Theoretical calculations of differential cross sections for reactions pd →pdππ and dd →ddππ are consistent with experimental data, except at high energies where the theoretical curve overestimates the data by a factor of 1.7.
|
[
"Calculations using the model [9] and isospin factor CT = 2.8",
"Comparison with experimental data from Ref. [11]",
"Proton beam energies Tp = 1.1 and 1.4 GeV, and deuteron beam energy Td = 4-20 GeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00587v1
|
https://arxiv.org/abs/2511.00587v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f7924731f0d69fd8e312ac25745ca72a88691caec94fdb6b0895f34510402149
|
Extracted from ArXiv paper 2511.00587v1 (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": "2511.00587v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:16:03.544611Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111558165091
|
The sPHENIX detector tracks approximately constant efficiency across streamed data, with 100 billion events collected and 2.9 pb^-1 integrated luminosity.
|
The sPHENIX detector tracks approximately constant efficiency across streamed data, with 100 billion events collected and 2.9 pb^-1 integrated luminosity.
|
[
"sPHENIX tracking detectors",
"Streaming readout mode at O(200) kHz rate",
"Figure 1: Number of reconstructed tracks vs beam crossing number"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00596v1
|
https://arxiv.org/abs/2511.00596v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
109b603ac5cf042308870d999d418388edb808bfffc3cbffaf431ec90f4a02da
|
Extracted from ArXiv paper 2511.00596v1 (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": "2511.00596v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:15:58.165091Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111642422820
|
Fusion excitation function measured for the reaction 20O + p with broad peaks at Ecm ≈1.35, 1.55, and 1.85 MeV, indicating a barrier-governed process.
|
Fusion excitation function measured for the reaction 20O + p with broad peaks at Ecm ≈1.35, 1.55, and 1.85 MeV, indicating a barrier-governed process.
|
[
"MuSIC@Indiana detector, various pressures and incident energies utilized",
"Statistical uncertainty: NER",
"Systematic uncertainty: 5% mis-identification of fusion events"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.01076v1
|
https://arxiv.org/abs/2511.01076v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a3fc935dee1fac78725c49d1d1bfb2e983428eea953ba71ae0c9fb2b3aa7ca48
|
Extracted from ArXiv paper 2511.01076v1 (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": "2511.01076v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:16:42.422820Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111714798438
|
Ground-state Larmor frequency of 3He measured as ωg = 2π × 7.821 Hz, unaffected by metastability exchange collisions and light shift
|
Ground-state Larmor frequency of 3He measured as ωg = 2π × 7.821 Hz, unaffected by metastability exchange collisions and light shift
|
[
"Resonant RF pulse excitation",
"Free induction decay (FID) signal analysis",
"Optical pumping enabled/disabled measurements"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.01313v1
|
https://arxiv.org/abs/2511.01313v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c7dcd43678d8b455ad18e5cc677da4f6a868bfc3b1cbb47230441c481fa3eb8c
|
Extracted from ArXiv paper 2511.01313v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.01313v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:17:14.798438Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111828190482
|
Predicted cross sections for coherent and incoherent electron pair production show a 2-5% variation when switching from proton to lead PDFs, with additional uncertainty of ~20% due to experimental exclusivity requirement
|
Predicted cross sections for coherent and incoherent electron pair production show a 2-5% variation when switching from proton to lead PDFs, with additional uncertainty of ~20% due to experimental exclusivity requirement
|
[
"ATLAS detector data",
"dielectron invariant mass: 10 < mee < 80 GeV",
"nuclear modifications to proton PDF accounted for using nNNPDF3.0 NLO PDF sets"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.01980v1
|
https://arxiv.org/abs/2511.01980v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5908165a0dfef03e747f3836b01612e52c164bc2bd98c757233bed487f7f4e66
|
Extracted from ArXiv paper 2511.01980v1 (chunk 9)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2511.01980v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:18:28.190482Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111856020274
|
A new analytic model for bremsstrahlung cross sections is introduced, combining a multi-Yukawa form factor with Coulomb corrections, to accurately interpolate across charge states.
|
A new analytic model for bremsstrahlung cross sections is introduced, combining a multi-Yukawa form factor with Coulomb corrections, to accurately interpolate across charge states.
|
[
"Multi-Yukawa potential representation",
"Fitted to high-quality atomic data (DHFS fits and Hubbell tabulations)",
"Rapidly evaluable expression for the doubly differential cross section"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02098v1
|
https://arxiv.org/abs/2511.02098v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
16b1b218448a62dc913fbbaf436e21ceda7b1008ea66267d8774720f957756da
|
Extracted from ArXiv paper 2511.02098v1 (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": "2511.02098v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:18:56.020791Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111917562684
|
Fully analytical expression for screened doubly differential cross section (DDCS) derived for arbitrary ionized states described by a multi-Yukawa potential
|
Fully analytical expression for screened doubly differential cross section (DDCS) derived for arbitrary ionized states described by a multi-Yukawa potential
|
[
"Matlab program implemented Eqs. (5), (7), and (16)",
"Comparison with numerical integration of Eq. (13) showed excellent agreement for various ionization degrees of aluminum",
"Doubly differential cross section (DDCS) results depend on the multi-Yukawa potential representation"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02098v1
|
https://arxiv.org/abs/2511.02098v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
823cc173e223ace5422e177689fad1c516ccdf2c0789f762cfab908c02e5fb68
|
Extracted from ArXiv paper 2511.02098v1 (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": "2511.02098v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:19:17.562684Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111938531691
|
The kinematic reach of the CLAS detector up to Q2 < 5.0 GeV2 has enabled mapping of the momentum dependence of the dressed–quark mass over a limited distance range where ≈30% of the hadron mass is generated.
|
The kinematic reach of the CLAS detector up to Q2 < 5.0 GeV2 has enabled mapping of the momentum dependence of the dressed–quark mass over a limited distance range where ≈30% of the hadron mass is generated.
|
[
"CLAS12 facility",
"Q2 up to 5.0 GeV2",
"Hadron mass generated: ≈30%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02124v1
|
https://arxiv.org/abs/2511.02124v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a7ec49cc7760da3c459655a1e02ea4db1162e11d2c2e2503eba1e5fa64087a3c
|
Extracted from ArXiv paper 2511.02124v1 (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": "2511.02124v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:19:38.531691Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111951468932
|
The quantum of circulation κ in annular atomic Fermi superfluids is measured to equal h/2m within experimental uncertainties, both in the BEC regime and in the strongly interacting unitary Fermi gas.
|
The quantum of circulation κ in annular atomic Fermi superfluids is measured to equal h/2m within experimental uncertainties, both in the BEC regime and in the strongly interacting unitary Fermi gas.
|
[
"Sagnac-like phonon interferometer",
"Rotation-induced phononic phase shift",
"Angular momentum per particle"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02664v2
|
https://arxiv.org/abs/2511.02664v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
394edcee3529715ecf46393102bcb34214eb160bb4b7831de7bb4c4a97e3be23
|
Extracted from ArXiv paper 2511.02664v2 (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": "2511.02664v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:19:51.468932Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_111957361944
|
Phonon velocity measured across the BEC-BCS crossover, with quality factor Q = ω0/Γ reaching up to 10 across the unitary regime
|
Phonon velocity measured across the BEC-BCS crossover, with quality factor Q = ω0/Γ reaching up to 10 across the unitary regime
|
[
" Phonon interferometry using atomic density measurements in an annular-shaped hard-wall potential",
" Phonon frequency extracted from fits of density modulations δn(θ, t) using Eq. (2)",
" Fitting error < 1%"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02664v2
|
https://arxiv.org/abs/2511.02664v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
43531719ff7368cb4f869d8578cc5e9449c9a28b4d4769772419ba4c2691959b
|
Extracted from ArXiv paper 2511.02664v2 (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": "2511.02664v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:19:57.361944Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112005992894
|
We measured the superfluid fraction of fermionic gases at unitarity as a function of temperature, finding a decrease in the superfluid fraction with increasing temperature.
|
We measured the superfluid fraction of fermionic gases at unitarity as a function of temperature, finding a decrease in the superfluid fraction with increasing temperature.
|
[
"Our experiment",
"Temperature range: 0.4 - 0.6 Tc",
"Angular momentum per particle measurements"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02664v2
|
https://arxiv.org/abs/2511.02664v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e788c8121252af8f063ea3bcfedda1d14ee0e6f99ca73935deb398489488ee6e
|
Extracted from ArXiv paper 2511.02664v2 (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": "2511.02664v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:20:05.993416Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112018615458
|
Phonon frequencies and decay rates measured in superfluids via interferometric data, with results from two fitting methods providing compatible results
|
Phonon frequencies and decay rates measured in superfluids via interferometric data, with results from two fitting methods providing compatible results
|
[
"Interferograms of rotating superfluids in BEC, UFG, and BCS regimes",
"Density-weighted angular moments ⟨cos θ⟩(t) and ⟨sin θ⟩(t)",
"Fitting procedure using Eqs. (8) and (10)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02664v2
|
https://arxiv.org/abs/2511.02664v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
123815166856ba2282f9f37fa82874811c9ec312e833c8c4e8e824d4e58f005b
|
Extracted from ArXiv paper 2511.02664v2 (chunk 13)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2511.02664v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:20:18.615458Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112231115358
|
The atomic polarizability of Erbium in its ground state was calculated and measured, showing a broad red-detuned region for long wavelengths without many resonances.
|
The atomic polarizability of Erbium in its ground state was calculated and measured, showing a broad red-detuned region for long wavelengths without many resonances.
|
[
"Semi-empirical electronic-structure calculation",
"Calculated static polarizability: 149 a.u.",
"Measured data shown in Fig. 1"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
72c66c2d9c202cc9fb027cf2034e57dc532f2f72bcdca777089c5235fdd8dd54
|
Extracted from ArXiv paper 2511.02890v2 (chunk 43)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 43,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:22:31.115358Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112238227798
|
The ground-state polarizability of Er is measured with an uncertainty of up to 35% at three different wavelengths, with values summarized in Table I.
|
The ground-state polarizability of Er is measured with an uncertainty of up to 35% at three different wavelengths, with values summarized in Table I.
|
[
"Single-beam optical dipole trap generated by a focused beam operating at the desired wavelength λ",
"Beam waists measured with an uncertainty of the order of 1% using the knife-edge method",
"Trap frequencies measured as a function of laser powers P"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
595cfc83ddad7acbcccd17debcadd2aaa6f29c668e902f7b103785b9566afb74
|
Extracted from ArXiv paper 2511.02890v2 (chunk 45)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 45,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:22:38.227798Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112245462738
|
The tensor polarizability of Er atoms in the ground state was measured to be αt = -15 ± 3 a.u., contributing only a few percent to the total atomic polarizability.
|
The tensor polarizability of Er atoms in the ground state was measured to be αt = -15 ± 3 a.u., contributing only a few percent to the total atomic polarizability.
|
[
"Er atoms trapped at θp = 90°, using 532.26 nm and 1064.5 nm laser wavelengths",
"Relative change of the light shift κ(θp) measured with Eq. (7)",
"αt extracted from fitting Eq. (7) to data in Fig. 3"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3d284d4c7cb4e873aba320f2e6639196a49a06bfbd2af1e3ff35a441c7219597
|
Extracted from ArXiv paper 2511.02890v2 (chunk 47)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 47,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:22:45.462738Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112444833910
|
A modified version of the Judd-Ofelt theory is proposed to describe transition intensities of lanthanide-ion-doped solids, allowing for characterizing forbidden transitions and predicting unobserved properties.
|
A modified version of the Judd-Ofelt theory is proposed to describe transition intensities of lanthanide-ion-doped solids, allowing for characterizing forbidden transitions and predicting unobserved properties.
|
[
"least-squares fit of experimental oscillator strengths or transition probabilities with three adjustable parameters",
"crystal field dependence of fitted parameters",
"accurate free-ion eigenvectors calculated using Cowan codes"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e22853103c24a9af5ccdbcafaaca24d03f568646af0d200aa32fdeb7631c6ac7
|
Extracted from ArXiv paper 2511.02890v2 (chunk 89)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 89,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:44.834426Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112734710368
|
Photoassociation resonances in ultracold atom-molecule collisions observed with a binding energy of 0.5 MHz.
|
Photoassociation resonances in ultracold atom-molecule collisions observed with a binding energy of 0.5 MHz.
|
[
"J. Cao, B.-Y. Wang, H. Yang, Z.-J. Fan, Z. Su, J. Rui, B. Zhao, and J.-W. Pan",
"Phys. Rev. Lett. 132, 093403 (2024)",
"0.5 MHz binding energy"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
87e76fe42a206d5fd7fd36a9033a2ac3174d257f2bc6be5be93191379bdbeb4f
|
Extracted from ArXiv paper 2511.02890v2 (chunk 147)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 147,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:27:34.710892Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112034068101
|
Proton beam drift and relative core-to-beam density ratio are reproduced in simulations, supporting the theory that kinetic instabilities determine the observed evolution of proton beam drift.
|
Proton beam drift and relative core-to-beam density ratio are reproduced in simulations, supporting the theory that kinetic instabilities determine the observed evolution of proton beam drift.
|
[
"Hybrid expanding box simulations",
"Comparison with solar wind data out to 1.5 AU",
"Initial conditions representing plasma states at 0.3 AU"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02940v1
|
https://arxiv.org/abs/2511.02940v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c5ba289308cdbe1c0b5c293eb3f343792e4d0e3068fa48f1ea78de5c9982c637
|
Extracted from ArXiv paper 2511.02940v1 (chunk 0)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.02940v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:20:34.068101Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112112692372
|
The Alfvenic fluctuations are observed in the solar wind with a mean velocity of 32 km/s, and a significant correlation between magnetic field and plasma flow is found.
|
The Alfvenic fluctuations are observed in the solar wind with a mean velocity of 32 km/s, and a significant correlation between magnetic field and plasma flow is found.
|
[
"Parker Solar Probe, spacecraft data",
"Velocity: 32 ± 5 km/s",
"Magnetic field-plasma flow correlation"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02940v1
|
https://arxiv.org/abs/2511.02940v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9b9f329deed0948891e81e0fc3ff8a38a31c585043e4e138b1b1b8b32b711684
|
Extracted from ArXiv paper 2511.02940v1 (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": "2511.02940v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:21:12.692372Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112120434924
|
Magnetic field morphology deviates from Gaussianity in turbulent dynamo simulations, with non-Gaussian structures observed at various scales.
|
Magnetic field morphology deviates from Gaussianity in turbulent dynamo simulations, with non-Gaussian structures observed at various scales.
|
[
"Numerical simulations of small-scale turbulent dynamo",
"Excursion set analysis for magnetic fields",
"Minkowski functionals (MFs) computed for each magnetic field component and threshold"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03072v1
|
https://arxiv.org/abs/2511.03072v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9fc9a4ae405fabd5a778e298cceb5f31c6903e1959d41abb453c263bdf4a5516
|
Extracted from ArXiv paper 2511.03072v1 (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": "2511.03072v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:21:20.435449Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112121934511
|
Seed laser intensity envelope along x direction changes due to CBET process in magnetized plasma, with noticeable spontaneous backscattering observed at doubled seed laser intensity
|
Seed laser intensity envelope along x direction changes due to CBET process in magnetized plasma, with noticeable spontaneous backscattering observed at doubled seed laser intensity
|
[
"2D-3V PIC simulations",
"Pump and seed laser intensities: Ip = Is = 0.5 × 10^15 W/cm^2 at entering boundaries",
"Notable effects on CBET process observed at halved or doubled intensities"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03090v1
|
https://arxiv.org/abs/2511.03090v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d79435778fa0733605a9a4c930ab8bb25044cc5152293b899224e3f201ab9926
|
Extracted from ArXiv paper 2511.03090v1 (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": "2511.03090v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:21:21.934511Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112145501463
|
Increased ion temperature and neutron yield observed in magnetized indirectly driven d2-filled capsule implosions on the National Ignition Facility
|
Increased ion temperature and neutron yield observed in magnetized indirectly driven d2-filled capsule implosions on the National Ignition Facility
|
[
"National Ignition Facility, 2022 data sample",
"Ion temperature: 150 million °C",
"Neutron yield enhancement"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03090v1
|
https://arxiv.org/abs/2511.03090v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
331129acc29ac596abeb313fc42d1eebd51ce42bb0896ec2b4362d53d28ff27c
|
Extracted from ArXiv paper 2511.03090v1 (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": "2511.03090v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:21:45.501463Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112118377970
|
α/γ discrimination method developed using three methods to identify and distinguish α particles and γ rays in bulky BaF2 detector for γ total absorption facility.
|
α/γ discrimination method developed using three methods to identify and distinguish α particles and γ rays in bulky BaF2 detector for γ total absorption facility.
|
[
"BaF2 detection unit, GTAF data acquisition system",
"3 radioactive sources (22Na, 137C, 60Co) used for verification",
"Quality factor FOM: 1.19-1.41, 0.94-1.04, and 0.93-1.07 from three methods"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03139v1
|
https://arxiv.org/abs/2511.03139v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
acd7cd9c4589b06085d4b7fd4445c40774f52de5865943a113fbecfb00d79680
|
Extracted from ArXiv paper 2511.03139v1 (chunk 0)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.03139v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:21:18.377970Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112216601973
|
Ratios R(D) = 0.467±0.101 and R(D∗) = 0.304±0.019 measured, showing deviations from directly measured averages
|
Ratios R(D) = 0.467±0.101 and R(D∗) = 0.304±0.019 measured, showing deviations from directly measured averages
|
[
"Belle II detector, future data sample",
"Comparison with PQCD-based SM predictions",
"Hadronic form factor uncertainties"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03414v1
|
https://arxiv.org/abs/2511.03414v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
0b5bc2ec0347b798f79c67eaf59d32fbe01ec20bb6b6f404c5cc3ccc461a7fcd
|
Extracted from ArXiv paper 2511.03414v1 (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": "2511.03414v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:22:16.601973Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112321755154
|
Thermal scattering cross-section for n+239Pu evaluated in ENDF/B-VIII.1 library, showing deviations within 1% for fission and capture cross sections.
|
Thermal scattering cross-section for n+239Pu evaluated in ENDF/B-VIII.1 library, showing deviations within 1% for fission and capture cross sections.
|
[
"ENDF/B-VIII.1 library",
"thermal cross sections compared with Thermal Neutron Constants derived by the Standard group [1] and Duran et al.",
"deviations up to -6% with JEFF-3.3 library"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
93f7dfe0133883da8be0291c0f416884c08c7ef094451184df2e267da0e66c9e
|
Extracted from ArXiv paper 2511.03564v1 (chunk 13)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:23:21.755154Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112328221551
|
The evaluated 239Pu(n,f) cross section uncertainty was updated to have energy-dependent correlations rather than being fully correlated, reducing the estimated uncertainty from 1.2% to an unspecified value.
|
The evaluated 239Pu(n,f) cross section uncertainty was updated to have energy-dependent correlations rather than being fully correlated, reducing the estimated uncertainty from 1.2% to an unspecified value.
|
[
"ENDF/B-VIII.0",
"USU component of fission cross-section uncertainties",
"Energy-dependent bias functions for each dataset"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
505f55b5ff3d647923355b8ce104f5bb6bc84fa5e862f6c2e0767fb2fb3f8051
|
Extracted from ArXiv paper 2511.03564v1 (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": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:23:28.221551Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112338304119
|
The evaluated uncertainty of the ENDF/B-VIII.1 capture cross sections is about 4% from 5 keV up to 100 keV, reduced by a factor of about 2 compared to ENDF/B-VIII.0 and ENDF/B-VII.1 uncertainties.
|
The evaluated uncertainty of the ENDF/B-VIII.1 capture cross sections is about 4% from 5 keV up to 100 keV, reduced by a factor of about 2 compared to ENDF/B-VIII.0 and ENDF/B-VII.1 uncertainties.
|
[
"EXFOR database",
"GANDR system with vetted experimental data",
"Evaluated correlation matrix shows negative and positive correlations due to the experimental data constrains"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
345b284edab30df7d2001d1b8d67678a13b43697eb6211cb216616659dc281ee
|
Extracted from ArXiv paper 2511.03564v1 (chunk 19)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 19,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:23:38.304119Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112351313189
|
Simulated effective delayed neutron fraction for Jezebel and Flattop plutonium systems agree better with measured values than ENDF/B-VIII.0
|
Simulated effective delayed neutron fraction for Jezebel and Flattop plutonium systems agree better with measured values than ENDF/B-VIII.0
|
[
"Table VIII: Calculated vs. experimental values of effective delayed neutron fraction",
"Two assemblies considered: Jezebel (PU-MET-FAST-001-001) and Flattop with plutonium core (PU-MET-FAST-006-001)",
"Uncertainties added to experimental ones in quadrature following IRPhEP"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
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5edcd22b733972b277cb13a8962f7a5f5f0607f234689fb38684550e85661144
|
Extracted from ArXiv paper 2511.03564v1 (chunk 23)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
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"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:23:51.313189Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112408620903
|
New ENDF/B-VIII.1 evaluation of neutron capture cross sections shows improved agreement with experimental data for forward angles, but underestimates scattered neutron yield at backward angles.
|
New ENDF/B-VIII.1 evaluation of neutron capture cross sections shows improved agreement with experimental data for forward angles, but underestimates scattered neutron yield at backward angles.
|
[
"ENDF/B-VIII.1 evaluation",
"Experimental data from scattering measurements between 1.3 MeV and 2 MeV",
"Underestimation of scattered neutron yield observed at backward angles"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2d4fb8abc48fe98c59fe751140470b6976041ac8c19bad66a418229c5a4d6f59
|
Extracted from ArXiv paper 2511.03564v1 (chunk 28)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 28,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:08.621416Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112411866973
|
Capture cross sections for chromium isotopes were updated to improve description of experimental data and criticality benchmarks.
|
Capture cross sections for chromium isotopes were updated to improve description of experimental data and criticality benchmarks.
|
[
"ENDF/B-VIII.1 evaluated files for 50,52,53,54Cr",
"Recent evaluation by Nobre et al. [155]",
"Careful investigation of previous data from Refs. [156–158]"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
0a750b16c270107f2bdae0bfcb698e710a65e43d9a13a11c0b7d4c847c9db872
|
Extracted from ArXiv paper 2511.03564v1 (chunk 29)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 29,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:11.866973Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112415616873
|
Evaluated files for chromium isotopes in ENDF/B-VIII.1 show improved description of experimental data, including angle-integrated cross sections and neutron double-differential spectra.
|
Evaluated files for chromium isotopes in ENDF/B-VIII.1 show improved description of experimental data, including angle-integrated cross sections and neutron double-differential spectra.
|
[
"ENDF/B-VIII.0 and ENDF/B-VIII.1 evaluated files",
"Reaction channels: inelastic and (n,p)",
"Evaluated isotopes: 50,52,53,54Cr"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ef43ca07b53b0a5e91fe3b744500d83a38ae26b34d1eca126beee18aa0a528c4
|
Extracted from ArXiv paper 2511.03564v1 (chunk 30)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 30,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:15.616873Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112437314777
|
Updated ENDF/B-VIII.1 evaluation improves agreement between calculated and measured criticality benchmark values compared to previous libraries.
|
Updated ENDF/B-VIII.1 evaluation improves agreement between calculated and measured criticality benchmark values compared to previous libraries.
|
[
"Thermal set of benchmarks (Fig. 47)",
"Epithermal assemblies with FEPIT≈40% (HCT005) show improved performance",
"ENDF/B-VIII.0 systematically underestimated epithermal assemblies"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
51a6e40075cd11ba9afbf42a133bda7112875a8490112482e9919208bbec63c0
|
Extracted from ArXiv paper 2511.03564v1 (chunk 38)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 38,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:37.315316Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112446357595
|
Thermal and resonance region n+233U reaction cross sections evaluated up to 2.5 keV with a focus on improving performance in criticality solution benchmarks.
|
Thermal and resonance region n+233U reaction cross sections evaluated up to 2.5 keV with a focus on improving performance in criticality solution benchmarks.
|
[
"ORELA facility, early 2000s transmission data",
"Lounsbury et al.'s measurements [70-72]",
"Standard evaluations as discussed in Ref. [210]"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9ff069c630249bde07f7b9b3f6b12e8e07efa545d9d2baebc6799d84f0bb4433
|
Extracted from ArXiv paper 2511.03564v1 (chunk 41)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 41,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:46.357595Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112515146412
|
Thermal capture cross section of 240Pu increased by +4.1% to 285.6 barns compared to ENDF/B-VIII.0 value
|
Thermal capture cross section of 240Pu increased by +4.1% to 285.6 barns compared to ENDF/B-VIII.0 value
|
[
"CONRAD code analysis using EXFOR database data",
"Transmission data from Spencer (1987), Harvey (1985, 1988), Kolar (1968)",
"Capture resonance integral increased by +4.1%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ce732b5045c26ebde82fd2f162b447cd994db2fd572d7235739f0ca911c87da5
|
Extracted from ArXiv paper 2511.03564v1 (chunk 50)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 50,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:25:15.146412Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112524786938
|
6Li(n, p)6He cross section measured with an uncertainty of ±10^-3 barns at incident neutron energies between 3 and 9 MeV
|
6Li(n, p)6He cross section measured with an uncertainty of ±10^-3 barns at incident neutron energies between 3 and 9 MeV
|
[
"Experimental data from Presser et al. [257]",
"Comparison to ENDF/B-VIII.1 evaluation",
"Double-peak structure of the interfering 3/2− levels"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b402d24dfc1acb8df6358fd3ee86ce3c0d2b293c475077763e85387fd9dce7a6
|
Extracted from ArXiv paper 2511.03564v1 (chunk 53)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 53,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:25:24.786938Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112555733139
|
Total cross section for neutron-induced reactions on 181Ta measured to be consistent with RIPL-3 potential after adjustments, within a few percent of experimental data
|
Total cross section for neutron-induced reactions on 181Ta measured to be consistent with RIPL-3 potential after adjustments, within a few percent of experimental data
|
[
"Poenitz et al. total cross section measurements",
"Refined RIPL-3 CC potential using Kalman filter",
"Tsubone and Carlson's experiments agree with updated optical potential"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
10dfd47f4a3acd4d96742b1a1f489e46783d0d496fbf1564c02b0ef95cbe3805
|
Extracted from ArXiv paper 2511.03564v1 (chunk 64)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 64,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:25:55.733139Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112605445195
|
181Ta nuclear data evaluated in ENDF/B-VIII.1 library matches measured quasi-differential neutron scattering at RPI, with slight underestimation below 2 MeV
|
181Ta nuclear data evaluated in ENDF/B-VIII.1 library matches measured quasi-differential neutron scattering at RPI, with slight underestimation below 2 MeV
|
[
"Tantalum sample at RPI",
"Neutron energies: 0.55 to 20 MeV",
"Detector angles: forward and backward"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d1374c89ab0a64c212d6d0be11a7112b88ccdfd3cec53b29536a03c0a540856a
|
Extracted from ArXiv paper 2511.03564v1 (chunk 67)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 67,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:26:05.445710Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112748709443
|
Beryllium-metal thermal scattering length updated with distinct Sd effects, improving agreement with experimentally measured cross sections
|
Beryllium-metal thermal scattering length updated with distinct Sd effects, improving agreement with experimentally measured cross sections
|
[
"ENDF/B-VIII.1 database update",
"FLASSH code used for evaluation",
"Good agreement with experimental data at 300, 440, 573, and 973 K"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
efc40f8861b142a5add25a7e98ca7c8d58805e88cb140b1d2ff5168907c3c8cd
|
Extracted from ArXiv paper 2511.03564v1 (chunk 100)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 100,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:27:48.709443Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112755652832
|
Neutron thermal scattering cross sections for FLiBe molten salt and reactor-graphite with 20% porosity have been evaluated using classical MD simulations
|
Neutron thermal scattering cross sections for FLiBe molten salt and reactor-graphite with 20% porosity have been evaluated using classical MD simulations
|
[
"LAMMPS MD code",
"Classical MD models of porous graphite",
"ENDF/B-VIII.1 database"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5403e07f48ea5ca54acecc02e2aa94bcf4623f11a9b3e04f3fbb0625f3f15222
|
Extracted from ArXiv paper 2511.03564v1 (chunk 102)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 102,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:27:55.652832Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112809532954
|
Thermal neutron scattering cross sections for SiC and SiO2 materials calculated using ab initio methods
|
Thermal neutron scattering cross sections for SiC and SiO2 materials calculated using ab initio methods
|
[
"VASP code",
"PHONON code",
"FLASSH simulations"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e5f69c67d14a261f5f9d5a008e38a72f61dfd6a776e8f402ad61b605fa72d043
|
Extracted from ArXiv paper 2511.03564v1 (chunk 106)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 106,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:28:09.533485Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112838104725
|
Thermal scattering cross sections for U(UC) and C(UC) demonstrated good agreement with neutron transmission measurements, especially after accounting for neutron absorption effects.
|
Thermal scattering cross sections for U(UC) and C(UC) demonstrated good agreement with neutron transmission measurements, especially after accounting for neutron absorption effects.
|
[
"ENDF/B-VIII.1 database",
"Neutron transmission measurements [563]",
"Integrated total scattering cross sections containing incoherent inelastic (MT4) and coherent elastic (MT2) contributions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ed200068537f1a913ac3c3693a168e492dc30382e1ae907e5fa984de332e0ebc
|
Extracted from ArXiv paper 2511.03564v1 (chunk 115)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 115,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:28:38.104725Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113149443734
|
The 6Li(n,t)4He reaction cross sections were measured from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source.
|
The 6Li(n,t)4He reaction cross sections were measured from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source.
|
[
"Measurement by H. Bai et al.",
"Data from 2020 paper in Chin. Phys. C",
"Cross-sections reported with uncertainties"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03564v1
|
https://arxiv.org/abs/2511.03564v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c22bd50dab7973f74bcafcc1407b318052ad93f3a0199e17fe7be908fa35600a
|
Extracted from ArXiv paper 2511.03564v1 (chunk 179)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 179,
"paper_id": "2511.03564v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:31:49.443734Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112333207185
|
Elliptic flow of f0(980) mesons measured in high-multiplicity p-Pb collisions at √sNN = 5.02 TeV, showing no NC scaling behavior with respect to kaon elliptic flow
|
Elliptic flow of f0(980) mesons measured in high-multiplicity p-Pb collisions at √sNN = 5.02 TeV, showing no NC scaling behavior with respect to kaon elliptic flow
|
[
"ALICE detector data",
"CMS Collaboration measurements",
"f0(980) production via K ¯K coalescence"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03638v1
|
https://arxiv.org/abs/2511.03638v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
12ecc0a9b6058c1b8c0035ff377c02a77725692ad75f007eb962d6f28d665079
|
Extracted from ArXiv paper 2511.03638v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.03638v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:23:33.207185Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112507360206
|
The decay amplitude of B → Dlν is measured as A = 0.011 ± 0.003, which agrees with Standard Model predictions.
|
The decay amplitude of B → Dlν is measured as A = 0.011 ± 0.003, which agrees with Standard Model predictions.
|
[
"Belle II detector",
"Data sample: 2019-2022",
"Cross-section: 1.5 pb"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03786v1
|
https://arxiv.org/abs/2511.03786v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9b75dd246f58c1b18b68fa677c2d7a69740e268abdaaeb0d622b718cad30bc69
|
Extracted from ArXiv paper 2511.03786v1 (chunk 31)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 31,
"paper_id": "2511.03786v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:25:07.360206Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112412406129
|
FastRICH ASIC meets performance requirements for LHCb RICH detector, with successful verification across occupancy scenarios and timing precision
|
FastRICH ASIC meets performance requirements for LHCb RICH detector, with successful verification across occupancy scenarios and timing precision
|
[
"Simulation-based verification",
"Timing precision: 25 ps",
"Occupancy range: 0% to 30%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03857v1
|
https://arxiv.org/abs/2511.03857v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a808655b7ac02833d443905ec8a5d060b0f5afb7a0f96fbf6f8e5661e483efc9
|
Extracted from ArXiv paper 2511.03857v1 (chunk 0)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.03857v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:12.406129Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112807092837
|
Belle II experiment measured the B(B+ →K+ν ¯ν) decay branching fraction to be (2.3 ± 0.5±0.5−0.4) × 10^−5, which is 2.7σ above the Standard Model prediction.
|
Belle II experiment measured the B(B+ →K+ν ¯ν) decay branching fraction to be (2.3 ± 0.5±0.5−0.4) × 10^−5, which is 2.7σ above the Standard Model prediction.
|
[
"Belle II detector",
"50 ab−1 data sample",
"Branching ratio precision: 10%"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03883v1
|
https://arxiv.org/abs/2511.03883v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
0c34d96842374f195b11c6b844013ebd01de1c0e7554e9a7160cff1b209f9630
|
Extracted from ArXiv paper 2511.03883v1 (chunk 73)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 73,
"paper_id": "2511.03883v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:28:07.092837Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112842100895
|
Neutrino-nucleus cross-sections will be measured with unprecedented precision to improve the error of δCP in future experiments.
|
Neutrino-nucleus cross-sections will be measured with unprecedented precision to improve the error of δCP in future experiments.
|
[
"DUNE near detector liquid argon TPC",
"92,000 events analyzed",
"PRISM technique to measure cross sections at different average energies"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03883v1
|
https://arxiv.org/abs/2511.03883v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1fcece8b76d728a73251c7b25a72a170687bf230be3db63464c6baafb82f712d
|
Extracted from ArXiv paper 2511.03883v1 (chunk 84)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 84,
"paper_id": "2511.03883v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:28:42.100895Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112934527607
|
The next-generation gravitational wave detectors, such as the Einstein Telescope and Cosmic Explorer, are expected to significantly extend the science reach of ground-based interferometers.
|
The next-generation gravitational wave detectors, such as the Einstein Telescope and Cosmic Explorer, are expected to significantly extend the science reach of ground-based interferometers.
|
[
"Einstein Telescope (ET) in Europe",
"Cosmic Explorer in the US",
"Expected to detect 104 NS mergers up to a redshift of z ∼3"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03883v1
|
https://arxiv.org/abs/2511.03883v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
de79c4ca447fd01ad49c3103aad8cc8fe66c2279fc7562c61ac7c181d89d06ba
|
Extracted from ArXiv paper 2511.03883v1 (chunk 102)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 102,
"paper_id": "2511.03883v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:29:34.527607Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113133363895
|
Current direct detection experiments exclude large areas of parameter space for heavy WIMPs, with no credible signal observed to date.
|
Current direct detection experiments exclude large areas of parameter space for heavy WIMPs, with no credible signal observed to date.
|
[
"XENONnT experiment at LNGS in Italy",
"PandaX-4t in China, LZ in the US, and DEAP-3600 in Canada",
"No signal detected within grey shaded region of Fig. 9.6"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03883v1
|
https://arxiv.org/abs/2511.03883v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3fbd7673883a84732234580447fdb352c2a62be1ea371ba0039c69b5a45231b5
|
Extracted from ArXiv paper 2511.03883v1 (chunk 143)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 143,
"paper_id": "2511.03883v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:31:33.363895Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113354258515
|
Development of new detector technologies and experimental setups for dark matter searches, including noble liquids, cryogenic bolometers, and quantum sensors.
|
Development of new detector technologies and experimental setups for dark matter searches, including noble liquids, cryogenic bolometers, and quantum sensors.
|
[
"XENONnT and LZ detectors",
"Large xenon observatory with 60-ton active target",
"Axion helioscope IAXO with superconducting toroidal magnet"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03883v1
|
https://arxiv.org/abs/2511.03883v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c9bede03e3c3570eedacde10a5f9fbf458f1080095f8d41be5b8b9bf1f16c5d1
|
Extracted from ArXiv paper 2511.03883v1 (chunk 190)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 190,
"paper_id": "2511.03883v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:33:54.259033Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112431667345
|
A neural network is developed to reconstruct neutrino events detected by the IceCube-Gen2 Radio detector in South Polar ice with improved resolution and uncertainty quantification
|
A neural network is developed to reconstruct neutrino events detected by the IceCube-Gen2 Radio detector in South Polar ice with improved resolution and uncertainty quantification
|
[
"IceCube-Gen2 Neutrino Observatory, planned successor to IceCube",
"Neural network predicts posterior PDF of neutrino direction and shower energy",
"Conditional normalizing flows used for uncertainty estimation"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03910v1
|
https://arxiv.org/abs/2511.03910v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9229d0314488e7783f12563db8643e2b9ee65ca72520eabf6d615a72669b23a7
|
Extracted from ArXiv paper 2511.03910v1 (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": "2511.03910v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:31.667345Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112447061345
|
A neural network is trained to distinguish between νx - NC and νe - CC events in a uniform spectrum of neutrino arrival directions, using simulated antenna waveforms from the IceCube-Gen2 detector.
|
A neural network is trained to distinguish between νx - NC and νe - CC events in a uniform spectrum of neutrino arrival directions, using simulated antenna waveforms from the IceCube-Gen2 detector.
|
[
"Simulated data with uniform spectrum of neutrino arrival directions",
"Neural network architecture combining several architectures into one large model",
"Detector temperature: 300 K"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03910v1
|
https://arxiv.org/abs/2511.03910v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d49f8cb94954ba276d9749e1e003adc9c04e3650c66fbe9961d18e04878b17b1
|
Extracted from ArXiv paper 2511.03910v1 (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": "2511.03910v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:47.061345Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112456121208
|
Shower energy resolution measured with median uncertainty of 0.2-0.35 in log(E) for νx - NC events and 0.3-0.4 in log(E) for νe - CC events
|
Shower energy resolution measured with median uncertainty of 0.2-0.35 in log(E) for νx - NC events and 0.3-0.4 in log(E) for νe - CC events
|
[
"4-dimensional Euclidean normalizing flow model",
"Test dataset with shower energy range from 1017 eV to higher energies",
"68% highest density interval (HDI) used to calculate resolution"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03910v1
|
https://arxiv.org/abs/2511.03910v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
442e9a8142ed4387d187213d245b927ea55e5963237ecebfad2ed23536b962e9
|
Extracted from ArXiv paper 2511.03910v1 (chunk 9)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2511.03910v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:56.121735Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112459485591
|
Shower energy resolution measured with median 68% uncertainty between 0.2 and 0.35 in log(E) for νx - NC events, and between 0.3 and 0.4 in log(E) for νe - CC events
|
Shower energy resolution measured with median 68% uncertainty between 0.2 and 0.35 in log(E) for νx - NC events, and between 0.3 and 0.4 in log(E) for νe - CC events
|
[
"shallow station component",
"νx-NC events: 16th to 84th percentile of resolution per bin shown in figure 4",
"νe-CC events: systematic uncertainty 0.008"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03910v1
|
https://arxiv.org/abs/2511.03910v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1c1a09b94052051813332e8ab3445144cb8b4692d1735853e07f064fe9fd582d
|
Extracted from ArXiv paper 2511.03910v1 (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": "2511.03910v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:24:59.485591Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112531888594
|
A neural network capable of performing a full reconstruction for in-ice radio neutrino detectors was developed, achieving significant improvements in shower energy and neutrino direction resolution.
|
A neural network capable of performing a full reconstruction for in-ice radio neutrino detectors was developed, achieving significant improvements in shower energy and neutrino direction resolution.
|
[
"IceCube-Gen2 radio detector, 'shallow' and 'deep' detector components",
"Shower energy resolution improved by a factor of two without analysis cuts",
"Neutrino direction resolution improved by roughly a factor of 30"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03910v1
|
https://arxiv.org/abs/2511.03910v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
52d37ef89d530f0f3a4310a9eed10f198cc2aebcb3f4f353dfd17ddebb17e109
|
Extracted from ArXiv paper 2511.03910v1 (chunk 20)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 20,
"paper_id": "2511.03910v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:25:31.889131Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112535412985
|
Neutrino arrival direction is reconstructed in deep-ice radio detectors using surface reflections and implications for neutrino energy resolution are discussed
|
Neutrino arrival direction is reconstructed in deep-ice radio detectors using surface reflections and implications for neutrino energy resolution are discussed
|
[
"Eur. Phys. J. C 83 (2023) 443",
"J. Cosmol. Astropart. Phys. 11 (2019) 030",
"NuRadioMC: simulating the radio emission of neutrinos from interaction to detector, Eur. Phys. J. C 80 (2020) 77"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03910v1
|
https://arxiv.org/abs/2511.03910v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
0ced71cae0e3162f6d2ed78008fa937c6dbbd052e2eadb4b8b088ccaa5662fd9
|
Extracted from ArXiv paper 2511.03910v1 (chunk 22)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 22,
"paper_id": "2511.03910v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:25:35.412985Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112601149483
|
The simulated B(R) and B(Z) profiles reasonably reproduce the measurement-based profiles of magnetic power, with distinct profile shapes observed from the probe measurements.
|
The simulated B(R) and B(Z) profiles reasonably reproduce the measurement-based profiles of magnetic power, with distinct profile shapes observed from the probe measurements.
|
[
"Hall sensor probe data",
"n = 1 oscillation frequency (f = 35 kHz)",
"Simulated profiles using a toroidal loop of current model"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03930v1
|
https://arxiv.org/abs/2511.03930v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b72da55e4ebf7528524b56bdb6f50aec8a032efa06e15aa7a5b199ca52bce62e
|
Extracted from ArXiv paper 2511.03930v1 (chunk 16)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 16,
"paper_id": "2511.03930v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:26:01.149483Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112638390354
|
Jet quenching effects in PbPb collisions at the LHC are observed through increased photon-jet momentum imbalance and enhanced jet fragmentation function in the large ξ region.
|
Jet quenching effects in PbPb collisions at the LHC are observed through increased photon-jet momentum imbalance and enhanced jet fragmentation function in the large ξ region.
|
[
"JEWEL simulation, GEN level",
"Centrality range: 0-10%",
"Quenching classes: Q 0-20%, Q 80-100%"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.04005v2
|
https://arxiv.org/abs/2511.04005v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ca3f65faa2dd060074b27cdff14d38456c4992c89ea6ee9919e554e15561b973
|
Extracted from ArXiv paper 2511.04005v2 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.04005v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:26:38.390354Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112641686574
|
Jet energy loss due to quenching is observed in PbPb collisions, with strongly quenched jets exhibiting greater redistribution of energy to softer particles.
|
Jet energy loss due to quenching is observed in PbPb collisions, with strongly quenched jets exhibiting greater redistribution of energy to softer particles.
|
[
"JEWEL simulation of PbPb collisions",
"DELPHES RECO level with detector effects simulated",
"ML classification results for five quenching classes"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.04005v2
|
https://arxiv.org/abs/2511.04005v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c4d85559265529ea90015d6b20206e2d8c1234691a6f06e762df0f69558d69da
|
Extracted from ArXiv paper 2511.04005v2 (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": "2511.04005v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:26:41.686574Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112657620114
|
Improved core confinement is observed in EAST discharge #93890, with ITB present in the ion temperature profile.
|
Improved core confinement is observed in EAST discharge #93890, with ITB present in the ion temperature profile.
|
[
"EAST tokamak plasma profiles from discharge #93890",
"Ion temperature: 150 million °C",
"ITG turbulence and fishbone interactions studied using global gyrokinetic simulations"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.04051v1
|
https://arxiv.org/abs/2511.04051v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
eec7436386057d9b48cdb9b7d827294c6c909ddb119f2e3945d338d4ed4e6ae3
|
Extracted from ArXiv paper 2511.04051v1 (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": "2511.04051v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:26:57.620114Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112727477957
|
The gravitational wave event GW150914 is reanalyzed with the new method ASPIRE, incorporating 40 additional parameters for detector calibration uncertainty, without introducing bias.
|
The gravitational wave event GW150914 is reanalyzed with the new method ASPIRE, incorporating 40 additional parameters for detector calibration uncertainty, without introducing bias.
|
[
"GW150914 first detection",
"40 additional parameters for detector calibration",
"7-fold reduction in evaluations per sample"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.04218v1
|
https://arxiv.org/abs/2511.04218v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
20f55cb20de430c8857ec9804510121b8d2d4c09f1fe25c643568b96226b6c93
|
Extracted from ArXiv paper 2511.04218v1 (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": "2511.04218v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:27:27.477957Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_112815171461
|
The fully differential cross sections for the photoproduction of meson pairs are computed and observed to have reflection symmetry about the line u' = M_2^12/2, with values reaching up to a thousand in certain processes.
|
The fully differential cross sections for the photoproduction of meson pairs are computed and observed to have reflection symmetry about the line u' = M_2^12/2, with values reaching up to a thousand in certain processes.
|
[
"JLab kinematics",
"Computed using automated methods",
"Processes include gamma N →N ′M1M2 where M1 and M2 can be rho mesons or pions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.04315v1
|
https://arxiv.org/abs/2511.04315v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
fbcaeaeb185caa0f4e2e48cb062280d401ca26a47f42be9ecb965699cdc7e6ec
|
Extracted from ArXiv paper 2511.04315v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.04315v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:28:15.171461Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113025127177
|
Superfluid fraction tensor measured with nearly isotropic components, and compressibility and speed of sound used to determine superfluid fraction as fs = 0.82(2)
|
Superfluid fraction tensor measured with nearly isotropic components, and compressibility and speed of sound used to determine superfluid fraction as fs = 0.82(2)
|
[
"Experiment using ultracold atomic cloud in a lattice potential",
"Compressibility measured by applying static force May along direction y and extracting CoM displacement δy",
"Speed of sound determined from CoM oscillation frequency νy"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.04575v1
|
https://arxiv.org/abs/2511.04575v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
60f550ae7f3fcb926fe7a6ecad2b3fc897bd15bcb1fbbb84baa91d241da1fac6
|
Extracted from ArXiv paper 2511.04575v1 (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": "2511.04575v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:30:25.127177Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113059490456
|
Neutron capture efficiency in water measured to be approximately 50% near the centre of the SNO+ detector
|
Neutron capture efficiency in water measured to be approximately 50% near the centre of the SNO+ detector
|
[
"Am-Be calibration source, 241Am α-decays with a half-life of 432 years",
"Neutron detection efficiency: 50%",
"Neutron capture time: 202.53±0.87 µs"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.04600v2
|
https://arxiv.org/abs/2511.04600v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4695ed47ef626f8409fe991392915953578a1ce0c882d05dc1ecb35ee934a52f
|
Extracted from ArXiv paper 2511.04600v2 (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": "2511.04600v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:30:59.490456Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
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