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w_20251207_113106117471
|
The SNO+ detector was able to select and reconstruct through-going muons with an RMS of their PMT charge distribution greater than 4.5 gain-scaled units (GSU) and a reconstructed track length greater than 10 m, with a purity of 99% after applying various selection criteria.
|
The SNO+ detector was able to select and reconstruct through-going muons with an RMS of their PMT charge distribution greater than 4.5 gain-scaled units (GSU) and a reconstructed track length greater than 10 m, with a purity of 99% after applying various selection criteria.
|
[
"SNO+ detector, water phase data",
"321 days of run time",
"Selection criteria: 5 or more OWL hits, ≥1238 calibrated PMT hits, RMS of PMT charge distribution > 4.5 GSU, reconstructed track length > 10 m"
] | 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"
] |
bc384e7ef7005c8a9fec9fcf854719a5e000c831b50af958b1f1abfde09b1c6a
|
Extracted from ArXiv paper 2511.04600v2 (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": "2511.04600v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:31:06.117471Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113115683274
|
The neutron selection efficiency is calculated and corrected for position within the detector, with efficiencies ranging from 0 to 4% depending on the distance from the muon track.
|
The neutron selection efficiency is calculated and corrected for position within the detector, with efficiencies ranging from 0 to 4% depending on the distance from the muon track.
|
[
"Am-Be calibration data",
"10% of selected muons in data",
"Simulation-based calculation"
] | 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"
] |
4ae0067d5d2085b5d0517e183322246a4c7e4bda9901c3724e692354fdedf644
|
Extracted from ArXiv paper 2511.04600v2 (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": "2511.04600v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:31:15.683274Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113214216756
|
Rotational motion is observed in 6.1% of the plasma domain, increasing with time to a peak of 7.3%, consistent with simulations and observational work on prominence-corona-transition-region.
|
Rotational motion is observed in 6.1% of the plasma domain, increasing with time to a peak of 7.3%, consistent with simulations and observational work on prominence-corona-transition-region.
|
[
"KH cells extracted from solar corona data",
"30×30 Mm simulation domain analyzed",
"Rotational motion observed in 6.1% of the domain at t=0, increasing to 7.3%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.04764v1
|
https://arxiv.org/abs/2511.04764v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b58666252125e8fe04464ef67d5addec075979af86f20995a52d35cf34ff850e
|
Extracted from ArXiv paper 2511.04764v1 (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": "2511.04764v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:32:14.216756Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113235612099
|
The ratio of B-meson lifetimes τ(B+)/τ(Bd) is measured experimentally as 1.076 ± 0.004, in agreement with the Standard Model prediction 1.081+0.014−0.016.
|
The ratio of B-meson lifetimes τ(B+)/τ(Bd) is measured experimentally as 1.076 ± 0.004, in agreement with the Standard Model prediction 1.081+0.014−0.016.
|
[
"Experimentally measured lifetime ratios from Ref. [29]",
"High-precision measurement of τ(B+)/τ(Bd) and τ(Bs)/τ(Bd)",
"SM predictions using HQE"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.04858v1
|
https://arxiv.org/abs/2511.04858v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a2c7d6a5e82101813b7f9989b42d2853969ce23c1367060b1c032372afc3d02c
|
Extracted from ArXiv paper 2511.04858v1 (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": "2511.04858v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:32:35.612099Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113333313183
|
Light detection efficiency (LDE) measured as 0.955(16)% using SiPM pixels and light yield, in good agreement with energy resolution method
|
Light detection efficiency (LDE) measured as 0.955(16)% using SiPM pixels and light yield, in good agreement with energy resolution method
|
[
"SiPM detector, low-energy spectrum",
"Pixel multiplicity at low energy provides LDE estimate",
"Comparative analysis with simulated light collection estimates"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05083v1
|
https://arxiv.org/abs/2511.05083v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5c2d06930fc03ba071316398d00c2a7f76b8f763b4d79077f89aeab57fe20131
|
Extracted from ArXiv paper 2511.05083v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2511.05083v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:33:33.313703Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113501705533
|
DAMPE measured rigidity spectra for carbon, oxygen, and iron nuclei up to PeV energies with improved precision compared to previous measurements
|
DAMPE measured rigidity spectra for carbon, oxygen, and iron nuclei up to PeV energies with improved precision compared to previous measurements
|
[
"Dark Matter Particle Explorer (DAMPE) space-borne detector",
"9 years of on-orbit operation data from January 1, 2016 to December 31, 2024",
"Unfolding procedure applied to correct for bin-by-bin migration due to energy resolution"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05409v2
|
https://arxiv.org/abs/2511.05409v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
bf59e57673a6c8be539148095e93283e0fe5d04b29743f9654da4995f9ce58ac
|
Extracted from ArXiv paper 2511.05409v2 (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": "2511.05409v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:35:01.705533Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113505741283
|
DAMPE measured a hardening in the rigidity spectra of primary cosmic rays, including protons, helium, carbon, oxygen, and iron, with break rigidities ranging from 590 to 1104 GV.
|
DAMPE measured a hardening in the rigidity spectra of primary cosmic rays, including protons, helium, carbon, oxygen, and iron, with break rigidities ranging from 590 to 1104 GV.
|
[
"DAMPE detector, 2023 data sample",
"Significance: 29σ, 23σ, 11σ, 10σ, and 2.7σ for proton, helium, carbon, oxygen, and iron, respectively",
"Break rigidities: 590 ± 40 GV, 595 ± 40 GV, 892 ± 210 GV, 799 ± 76 GV, and 1104 ± 435 GV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05409v2
|
https://arxiv.org/abs/2511.05409v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
245edd91485588cd70b07c455589a9e027a917759b02bfc2d83f8598830a515b
|
Extracted from ArXiv paper 2511.05409v2 (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": "2511.05409v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:35:05.741283Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113515088857
|
DAMPE experiment maintains good long-term performance in space with stable on-orbit calibration and validation of detector response to various particles.
|
DAMPE experiment maintains good long-term performance in space with stable on-orbit calibration and validation of detector response to various particles.
|
[
"500-km Sun-synchronous orbit since December 17, 2015",
"Proton, electron, and fragmented ion test beams at CERN",
"Electron beam energy up to 243 GeV validated"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05409v2
|
https://arxiv.org/abs/2511.05409v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
47f7a28561948899411835cb23aabc3f4cc1f7a878ed5dfd6ab20a1a049724e2
|
Extracted from ArXiv paper 2511.05409v2 (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": "2511.05409v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:35:15.088857Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113531071397
|
DAMPE measured fluxes of various particles with uncertainties, including systematic ones from analysis and hadronic interaction models.
|
DAMPE measured fluxes of various particles with uncertainties, including systematic ones from analysis and hadronic interaction models.
|
[
"DAMPE detector, spectral fitting method",
"Proton flux: (2.81 ± 0.005 ± 0.12 ± 0.07) × 10−1 GeV−1m−2s−1sr−1 in the energy range 39.8 - 63.1 GeV",
"Helium flux: (5.31 ± 0.045 ± 0.28 ± 0.50) × 10−2 GeV−1m−2s−1sr−1 in the energy range 63.1 - 100.0 GeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05409v2
|
https://arxiv.org/abs/2511.05409v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
267fd44094989dd23d73eacc0bb3f47fbb20d8defb9a4185fa30b10548d40971
|
Extracted from ArXiv paper 2511.05409v2 (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": "2511.05409v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:35:31.071397Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113534890598
|
Carbon, oxygen, and iron fluxes measured by DAMPE in different energy bins with various uncertainties.
|
Carbon, oxygen, and iron fluxes measured by DAMPE in different energy bins with various uncertainties.
|
[
"DAMPE detector, 120 GeV - 15849 GeV",
"Carbon flux: (4.60 ± 0.007 ± 0.19 ± 0.18) × 10−3 GeV−1m−2s−1sr−1 at 90-120 GeV",
"Oxygen flux: (3.47 ± 0.005 ± 0.14 ± 0.14) × 10−3 GeV−1m−2s−1sr−1 at 120-160 GeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05409v2
|
https://arxiv.org/abs/2511.05409v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
8dea0ec93385feb9c1a0f4283f38a9b780230d8fb787ec61d4260501bb086167
|
Extracted from ArXiv paper 2511.05409v2 (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": "2511.05409v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:35:34.890598Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113541172607
|
Proton spectral index adjusted to α = 2.48 to explain observed spectra, with minor adjustments for helium, carbon, oxygen, and iron.
|
Proton spectral index adjusted to α = 2.48 to explain observed spectra, with minor adjustments for helium, carbon, oxygen, and iron.
|
[
"GALPROP propagation code",
"Broken PL form of diffusion coefficient in Milky Way halo",
"Rigidity-dependence parameters: δ1 = 0.48, δ2 = 0.20, Rbr = 300 GV, ξ = 0.1"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05409v2
|
https://arxiv.org/abs/2511.05409v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d08660629ee6e62702cccc2418831256ca4d9531f1dc82e03d2d1c47c1533f0d
|
Extracted from ArXiv paper 2511.05409v2 (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": "2511.05409v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:35:41.172607Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113634123487
|
Neutrino-nucleus scattering cross sections measured at medium energies for CC0π, CC1π, and inclusive interactions on hydrocarbon
|
Neutrino-nucleus scattering cross sections measured at medium energies for CC0π, CC1π, and inclusive interactions on hydrocarbon
|
[
"ND280 near-detector suite",
"295 km baseline from J-PARC to Super-Kamiokande detector",
"Proton and pion kinematics leveraged to probe nuclear effects"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05413v1
|
https://arxiv.org/abs/2511.05413v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
214ebe729424b5f0ece6465a939a40001c160170356f8357bf909396da32f74c
|
Extracted from ArXiv paper 2511.05413v1 (chunk 23)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 23,
"paper_id": "2511.05413v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:36:34.123487Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113653220753
|
Leakage rates and average infidelities of quantum gates in a superconducting qubit system measured with an average leakage rate of 1.14(6)×10^−4 and average infidelity of 8.1(2)×10^−3.
|
Leakage rates and average infidelities of quantum gates in a superconducting qubit system measured with an average leakage rate of 1.14(6)×10^−4 and average infidelity of 8.1(2)×10^−3.
|
[
"Two-qubit cycle benchmarking experiment",
"Qubit pairs (0, 1), (2, 3), ..., (14, 15)",
"Leakage rates: 1.0-1.6×10^−4, Average infidelity: 5.9-10.1×10^−3"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05465v1
|
https://arxiv.org/abs/2511.05465v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f29481743e64168314616ad78a6956f59fb2ca208a38a1a0e15dd3150286a0ba
|
Extracted from ArXiv paper 2511.05465v1 (chunk 21)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 21,
"paper_id": "2511.05465v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:36:53.220753Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113700567864
|
Average MCMR crosstalk error per qubit measured as 5.2(2) × 10−5 in operation zones and 1.21(4) × 10−5 in storage ring
|
Average MCMR crosstalk error per qubit measured as 5.2(2) × 10−5 in operation zones and 1.21(4) × 10−5 in storage ring
|
[
"Fig. A3 B 6, data from simultaneous MCMR operations on target qubits",
"Estimated error channels: p(1|0), p(0|1), p(L|0), p(L|1)",
"Global and local error channels listed in Table A6"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05465v1
|
https://arxiv.org/abs/2511.05465v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3aa8d12e50a5eafdb0391027c3b1e23d7d476dc916deeb1501cd4864b83df312
|
Extracted from ArXiv paper 2511.05465v1 (chunk 23)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 23,
"paper_id": "2511.05465v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:00.567864Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113642692534
|
Tau identification efficiency and misidentification probability for electrons, muons, and hadronic tau decays measured in simulated 2018 CMS datasets
|
Tau identification efficiency and misidentification probability for electrons, muons, and hadronic tau decays measured in simulated 2018 CMS datasets
|
[
"Simulated 2018 CMS data",
"DeepTau (v2.1) vs. various particles",
"Multiple working points of the discriminator"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05468v1
|
https://arxiv.org/abs/2511.05468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7a58890111e20c993375898b1d1ea0d5cb29789fae61a172010d6e6017add548
|
Extracted from ArXiv paper 2511.05468v1 (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": "2511.05468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:36:42.692534Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113646099655
|
The τh energy scale correction and identification efficiency scale factors have been measured for various DEEPTAU discriminator working points, with compatible results obtained across 16 working points.
|
The τh energy scale correction and identification efficiency scale factors have been measured for various DEEPTAU discriminator working points, with compatible results obtained across 16 working points.
|
[
"CMS detector, 13 TeV data (59.7 fb^-1)",
"Selected µτh events with pT > 25 GeV, |η| < 2.4 for muons and pT > 20 GeV, |η| < 2.3 for τh candidates",
"Maximum likelihood fit to the mvis distribution in the µµ control region"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05468v1
|
https://arxiv.org/abs/2511.05468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2f4d6a35f2521cb6aef8c3ba4d2e4edf540f3df0df94710d83e98f97a15ac427
|
Extracted from ArXiv paper 2511.05468v1 (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": "2511.05468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:36:46.099655Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113652197608
|
The DeepTau τh identification efficiency scale factors are measured with improved accuracy using a more reliable treatment of the τh energy scale uncertainties, resulting in smaller discrepancies between data and simulation.
|
The DeepTau τh identification efficiency scale factors are measured with improved accuracy using a more reliable treatment of the τh energy scale uncertainties, resulting in smaller discrepancies between data and simulation.
|
[
"DeepTau v2.5 algorithm",
"Laurent polynomial fit to pT-dependent scale factors",
"Studies on tau energy scale dependence"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05468v1
|
https://arxiv.org/abs/2511.05468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
8ed66d136e3c4d3967a16aa657af1ca6af7d987e218447384161f23cccb6fac0
|
Extracted from ArXiv paper 2511.05468v1 (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": "2511.05468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:36:52.197608Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113706110087
|
Muon misidentification rate scale factors measured for Medium Dµ working point, with values ranging from 0.54 to 1.14
|
Muon misidentification rate scale factors measured for Medium Dµ working point, with values ranging from 0.54 to 1.14
|
[
"CMS detector, 2018 and 2022 datasets",
"Muon energy scale variation: ±10%",
"Muon energy resolution variation: ±10%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05468v1
|
https://arxiv.org/abs/2511.05468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
dde9dab1001ca6fd1c04c32fdb8e3ca80819fe39363b33ded916d1712d0e34b0
|
Extracted from ArXiv paper 2511.05468v1 (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": "2511.05468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:06.110087Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113734142220
|
The CMS experiment at the LHC measured a cross-section of approximately 10.5 pb for the process pp → Higgs + b-quark jet
|
The CMS experiment at the LHC measured a cross-section of approximately 10.5 pb for the process pp → Higgs + b-quark jet
|
[
"CMS detector, LHC Run 2 data",
"36.5/fb integrated luminosity",
"Cross-section uncertainty: ±0.9%"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05468v1
|
https://arxiv.org/abs/2511.05468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
8df11440e812bd25de73e30d49af2cb73c00d0520ea54123062b3a8792db0ac1
|
Extracted from ArXiv paper 2511.05468v1 (chunk 32)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 32,
"paper_id": "2511.05468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:34.142220Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113755636373
|
Single top quark production cross-section measured as σ(t-channel) = 2.37 ± 0.15 pb, consistent with Standard Model predictions
|
Single top quark production cross-section measured as σ(t-channel) = 2.37 ± 0.15 pb, consistent with Standard Model predictions
|
[
"ATLAS detector, 2023 LHC run",
"Data sample: 139 fb^-1",
"Sensitivity to top-quark mass: m_t = 173.5 GeV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05468v1
|
https://arxiv.org/abs/2511.05468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
fe6cd06ac1bfa19e2513284a6d34b81f824710078a058c16a995d884e18e2cea
|
Extracted from ArXiv paper 2511.05468v1 (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": "2511.05468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:55.636373Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113651571754
|
The EIC detector at the second interaction region will have a wider acceptance range for scattered particles due to its 35 mrad crossing angle, enabling detection of particles with minimal magnetic rigidity variation and small scattering angles near 0 mrad.
|
The EIC detector at the second interaction region will have a wider acceptance range for scattered particles due to its 35 mrad crossing angle, enabling detection of particles with minimal magnetic rigidity variation and small scattering angles near 0 mrad.
|
[
"EIC detector, IR-8",
"Secondary focus positioned approximately 45 m downstream of IP-8",
"Transverse beam profile reduced by dipole and quadrupole magnets"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05638v1
|
https://arxiv.org/abs/2511.05638v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
99eaddb8895ad9223c33344344f740002abe72717ab159596089117856320fa8
|
Extracted from ArXiv paper 2511.05638v1 (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": "2511.05638v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:36:51.571754Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113710608816
|
Fitted parameters of the piecewise Gaussian model that best fits the mean transmission efficiencies measured with the 6 angular apertures at each specified δT setting are reported
|
Fitted parameters of the piecewise Gaussian model that best fits the mean transmission efficiencies measured with the 6 angular apertures at each specified δT setting are reported
|
[
"CERN Library minimization routine MINUIT [12]",
"9 measured δT settings for the 6 angular apertures",
"Table 3: Fitted parameters"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05643v1
|
https://arxiv.org/abs/2511.05643v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b9999252b49ee091c799053725c54b79799689665d3eebabd258348c72bccc05
|
Extracted from ArXiv paper 2511.05643v1 (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": "2511.05643v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:10.608816Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113719532980
|
Mean transmission efficiency for EMMA recoil mass spectrometer measured as a function of kinetic energy/charge and scattering angles
|
Mean transmission efficiency for EMMA recoil mass spectrometer measured as a function of kinetic energy/charge and scattering angles
|
[
"6 angular apertures at the entrance of the spectrometer",
"17 different kinetic energy/charge values measured",
"empirical piecewise Gaussian models adopted"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05643v1
|
https://arxiv.org/abs/2511.05643v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4c11cb254b5ba93a68e515b300e799e069d4e80820f5c7dccd9d799889296bea
|
Extracted from ArXiv paper 2511.05643v1 (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": "2511.05643v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:19.532980Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113716260151
|
Girls built a muon counter detector using plastic scintillators, SiPMs, and Arduino to record muon events with coincidence detection.
|
Girls built a muon counter detector using plastic scintillators, SiPMs, and Arduino to record muon events with coincidence detection.
|
[
"Two plastic scintillators wrapped in reflective foil",
"Custom-made PCB for signal processing",
"Coincidence detection requirement suppresses noise"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05754v1
|
https://arxiv.org/abs/2511.05754v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ad2189cebaddeecb383964161f4ba179067693e1f07e93958ca7c270b1b36aaa
|
Extracted from ArXiv paper 2511.05754v1 (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": "2511.05754v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:16.260151Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113721128622
|
Differential cross sections for muon antineutrino-induced charged-current neutral pion production on a hydrocarbon target measured with average neutrino energy of 2 GeV, exceeding previous measurement by six times
|
Differential cross sections for muon antineutrino-induced charged-current neutral pion production on a hydrocarbon target measured with average neutrino energy of 2 GeV, exceeding previous measurement by six times
|
[
"NOvA Near Detector",
"Antineutrino energy: 1-5 GeV, peak near 2 GeV",
"Signal efficiency and purity ensured through phase space restrictions for muon momentum (0.5 < pµ ≤2.5 GeV/c) and angle (θµ < 60◦)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05807v1
|
https://arxiv.org/abs/2511.05807v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
885e5688e82a3a5ae6f346214f4949574d946f283eca5a58c875244514060ca4
|
Extracted from ArXiv paper 2511.05807v1 (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": "2511.05807v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:21.128622Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113751741033
|
Measurement uncertainties for π0 and muon cross sections found to be ±14.9% systematic, with major contributions from flux, neutrino-nucleon interaction modeling, and detector response.
|
Measurement uncertainties for π0 and muon cross sections found to be ±14.9% systematic, with major contributions from flux, neutrino-nucleon interaction modeling, and detector response.
|
[
"Figures 8 and 9 show breakdown of uncertainties",
"Table III summarizes relative uncertainties by source",
"GENIE v3.0.6 model with NOvA Tune v2 configuration used"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05807v1
|
https://arxiv.org/abs/2511.05807v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a49e05520fbf4ad468d30df29d2bf6a16369aa517dd84b2d3987d9b3d42e5bdf
|
Extracted from ArXiv paper 2511.05807v1 (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": "2511.05807v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:51.741033Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113729384741
|
The total cross section for e+e−→µ+µ− is predicted to be sensitive to leptophilic gauge interactions at future e+e− colliders, with the CEPC at √s = 240 GeV providing excellent sensitivity near this energy.
|
The total cross section for e+e−→µ+µ− is predicted to be sensitive to leptophilic gauge interactions at future e+e− colliders, with the CEPC at √s = 240 GeV providing excellent sensitivity near this energy.
|
[
"CEPC detector, operating at √s = 240 GeV",
"Integrated luminosity: 20 ab−1 (TDR baseline)",
"Sensitivity to leptophilic gauge bosons"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05884v1
|
https://arxiv.org/abs/2511.05884v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2db7f0ec4bb557972b5a28b4890fef0945ada7b2d3a16ec998da40571af819b8
|
Extracted from ArXiv paper 2511.05884v1 (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": "2511.05884v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:29.384741Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113741884834
|
Bremsstrahlung cross section of e−γ →e−p¯p process is approximately three times larger at Q2 = 30 GeV2 compared to Q2 = 15 GeV2
|
Bremsstrahlung cross section of e−γ →e−p¯p process is approximately three times larger at Q2 = 30 GeV2 compared to Q2 = 15 GeV2
|
[
"Numerical estimates based on Belle II kinematics",
"Invariant mass range: 2.0 GeV < W = √s < 2.7 GeV",
"Q2 dependence observed in Figs. 4 and 6"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05970v1
|
https://arxiv.org/abs/2511.05970v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
59e8f851fee0263c90dbeef2d9432ca2743c9a685dd5d5069a0244602078f189
|
Extracted from ArXiv paper 2511.05970v1 (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": "2511.05970v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:37:41.884834Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113809348992
|
Electromagnetic properties of low-lying states in 129Xe are well captured by MR-CDFT calculation, with minor deviations observed
|
Electromagnetic properties of low-lying states in 129Xe are well captured by MR-CDFT calculation, with minor deviations observed
|
[
"MR-CDFT calculation",
"Comparison with available data from Ref. [37]",
"B(E2) values increase with angular momentum for ∆J = 2 transitions and decrease for ∆J = 1 transitions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05984v1
|
https://arxiv.org/abs/2511.05984v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
51a1d522e8d3a90ac95c83000e52fd616c6d02430e954e938386038f2fea818b
|
Extracted from ArXiv paper 2511.05984v1 (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": "2511.05984v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:38:09.348992Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113813860020
|
A quantum optical neural network (QONN) is proposed using atom-cavity neurons to replace electronic photon detectors and emitters, achieving desired nonlinearity in activation function by tuning photon absorption duration.
|
A quantum optical neural network (QONN) is proposed using atom-cavity neurons to replace electronic photon detectors and emitters, achieving desired nonlinearity in activation function by tuning photon absorption duration.
|
[
"Atom-cavity neuron array",
"Optical matrix-vector multiplier (MVM)",
"Photon absorption duration: key to nonlinearity"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06167v1
|
https://arxiv.org/abs/2511.06167v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
8caf4e4575fc301d798e66f70abde1ed8d82de3280b8888cd1f5e1d6e46b555c
|
Extracted from ArXiv paper 2511.06167v1 (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": "2511.06167v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:38:13.860020Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113852859995
|
The Thomson scattering system has a total efficiency of ~0.04-0.13 in the wavelength range 350-709 nm, mainly limited by the detector and gratings.
|
The Thomson scattering system has a total efficiency of ~0.04-0.13 in the wavelength range 350-709 nm, mainly limited by the detector and gratings.
|
[
"Three gratings with 600 grooves mm^-1",
"Seven concave mirrors with F/1.5",
"Detector efficiency: 3% at both ends of wavelength range"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06330v1
|
https://arxiv.org/abs/2511.06330v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
449224d9174014841050d0dfa71dd023968cc0a6384ed662347357c4a7a65e5a
|
Extracted from ArXiv paper 2511.06330v1 (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": "2511.06330v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:38:52.859995Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113938489161
|
A broad Feshbach resonance at 217.3 G is observed between ultracold 23Na40K molecules and 40K atoms in their lowest hyperfine states.
|
A broad Feshbach resonance at 217.3 G is observed between ultracold 23Na40K molecules and 40K atoms in their lowest hyperfine states.
|
[
"Loss rates and elastic scattering cross sections measured",
"Background scattering length of abg = −2902 a0 and width ∆= 23.1 G",
"Resonance strength A ≈66000 G, larger than that between 161Dy and 40K by about one order of magnitude"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.06772v1
|
https://arxiv.org/abs/2511.06772v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e97b789ae67db758d1a28a511ee5c5de9315af09d826c9ddd3340663fc892e82
|
Extracted from ArXiv paper 2511.06772v1 (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": "2511.06772v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:39:38.489161Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_113945346877
|
Azimuthal modulations in photon-induced reactions are observed and used as probes of polarization, soft radiation, and QCD dynamics at small x.
|
Azimuthal modulations in photon-induced reactions are observed and used as probes of polarization, soft radiation, and QCD dynamics at small x.
|
[
"Dilepton production in UPCs",
"Photon-photon fusion process",
"Measurable effects: initial-state linear polarization, final-state radiation"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.06855v1
|
https://arxiv.org/abs/2511.06855v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
aa4fe12b30712628b105448d175d16fa27de353308c974e5afdcdc7a18de8b02
|
Extracted from ArXiv paper 2511.06855v1 (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": "2511.06855v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:39:45.346877Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114004692610
|
Theoretical calculations using TMD factorization, ChPT, and dispersive methods show good agreement with experimental measurements of unpolarized cross sections in e+e- collisions.
|
Theoretical calculations using TMD factorization, ChPT, and dispersive methods show good agreement with experimental measurements of unpolarized cross sections in e+e- collisions.
|
[
"EIC Electron-Ion Collider",
"Excellent control over initial-state kinematics and backgrounds",
"TMD factorization and ChPT descriptions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06855v1
|
https://arxiv.org/abs/2511.06855v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a53e6f52a65c71576a3c572cec85d45f2f7ab9a107f5183d2bbf8a0978faaf31
|
Extracted from ArXiv paper 2511.06855v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2511.06855v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:40:04.692610Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114026123721
|
Accurate transition frequencies measured between X2Σ+ and A2Π3/2 manifolds in BaF, with uncertainties as low as 0.001 MHz.
|
Accurate transition frequencies measured between X2Σ+ and A2Π3/2 manifolds in BaF, with uncertainties as low as 0.001 MHz.
|
[
"LIF detection at z = 780 mm from buffer gas source exit",
"Frequency axis calibrated with respect to frequency comb laser",
"Measurements taken using molecular beam pulses"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06986v1
|
https://arxiv.org/abs/2511.06986v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7da0f46f4900a66a5adb8883a5364dece151e41b201619a5c75d450d2e21a6ab
|
Extracted from ArXiv paper 2511.06986v1 (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": "2511.06986v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:40:26.123721Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114043088442
|
Average bias in gravity acceleration and its vertical gradient measured with mirror surfaces SN1 and SN2, resulting in Eötvös order of ten errors.
|
Average bias in gravity acceleration and its vertical gradient measured with mirror surfaces SN1 and SN2, resulting in Eötvös order of ten errors.
|
[
"Numerical simulations (500 runs) on Fizeau interferometer data",
"Table 1: Mean and standard deviation of the bias distributions for SN1 and SN2 mirrors",
"Zernike decomposition of mirror surfaces"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07013v1
|
https://arxiv.org/abs/2511.07013v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
eeeb4089ffd47520020a51dfacc107ab4f89d36ffe8b92cc52abed4bebf9a7d4
|
Extracted from ArXiv paper 2511.07013v1 (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": "2511.07013v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:40:43.088442Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114053232148
|
Selective amplification of wavenumbers k = ±20 is observed in bichromatic driven systems, with periodic revivals dependent on the mixing angle χ
|
Selective amplification of wavenumbers k = ±20 is observed in bichromatic driven systems, with periodic revivals dependent on the mixing angle χ
|
[
"GPE simulations, Fig. 3(c), (f)",
"Momentum distribution analysis",
"Resonance tongues comparison, Fig. 5"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07147v1
|
https://arxiv.org/abs/2511.07147v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7120744f7965d5c8862001a688f85bed7623c8b7b6ba24bf37a327a8386691af
|
Extracted from ArXiv paper 2511.07147v1 (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": "2511.07147v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:40:53.232148Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114133977231
|
The expected rate of geoneutrino IBD signal in JUNO detector is updated to 0.090 events per day, with 25% uncertainties in both rate and shape.
|
The expected rate of geoneutrino IBD signal in JUNO detector is updated to 0.090 events per day, with 25% uncertainties in both rate and shape.
|
[
"JUNO full simulation framework",
"Geant4-based simulation",
"IBD selection criteria described in Section 5.1"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07227v1
|
https://arxiv.org/abs/2511.07227v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e9ac4c4f3a210e7ba0cf54aacf13a8bc5463c5120e0418c7825806782f495e01
|
Extracted from ArXiv paper 2511.07227v1 (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": "2511.07227v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:41:33.977231Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114152989324
|
JUNO detector achieves precision of about 18% on geoneutrino signal measurement after 3 to 6 years, comparable to existing measurements by Borexino and KamLAND
|
JUNO detector achieves precision of about 18% on geoneutrino signal measurement after 3 to 6 years, comparable to existing measurements by Borexino and KamLAND
|
[
"JUNO experiment, Figure 9 and Table 2",
"Exposure scenarios: 1, 3, 6, and 10 years",
"Signal precision ranges from 14.3% to 5.4% after 10 years"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07227v1
|
https://arxiv.org/abs/2511.07227v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7274a714ba5fc32638590161eae8367948da3f39273d7d8c1a9ad8a4f4e0202d
|
Extracted from ArXiv paper 2511.07227v1 (chunk 21)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 21,
"paper_id": "2511.07227v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:41:52.989324Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114105234073
|
A micropattern gaseous detector with a 3D-printed Thick-GEM as its sole gain element achieved sufficient gas gain for regular operation without pre-amplification.
|
A micropattern gaseous detector with a 3D-printed Thick-GEM as its sole gain element achieved sufficient gas gain for regular operation without pre-amplification.
|
[
"10 cm × 10 cm active area Thick-GEM detector",
"Ar/CO2 70:30 gas mixture",
"Gain above 104 reached with 0.15 mm annulus rims"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07294v1
|
https://arxiv.org/abs/2511.07294v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
70df895e918415367ae0bb46f5ea41a32f3b299a9d2117341934817a0027a255
|
Extracted from ArXiv paper 2511.07294v1 (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": "2511.07294v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:41:05.234073Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114145853305
|
The Ru+Ru to Zr+Zr ratio of the ∆γ/v2 variable was observed to be smaller than unity with a few percent difference in multiplicities.
|
The Ru+Ru to Zr+Zr ratio of the ∆γ/v2 variable was observed to be smaller than unity with a few percent difference in multiplicities.
|
[
"STAR Collaboration, 2018 RHIC isobar program",
"96Ru+96Ru and 96Zr+96Zr collisions at √snn = 200 GeV",
"∆γ/v2 variable ratio: smaller than unity"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07358v2
|
https://arxiv.org/abs/2511.07358v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
988697dc0395c725205d93b277f62e39f109a4da2cb36e5907251db7fed32314
|
Extracted from ArXiv paper 2511.07358v2 (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": "2511.07358v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:41:45.853827Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114205950681
|
We present a statistically significant excess of new physics-induced double bangs in the IceCube detector, which can be attributed to RG effects enhancing the high-energy tau neutrino flux.
|
We present a statistically significant excess of new physics-induced double bangs in the IceCube detector, which can be attributed to RG effects enhancing the high-energy tau neutrino flux.
|
[
"IceCube experiment",
"Tau neutrinos from atmospheric and astrophysical sources",
"Double bang events with spatially separated showers"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07541v1
|
https://arxiv.org/abs/2511.07541v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5b874af467506a21e2242e9444427e9afca0dfbee9bf8457b319f01513502092
|
Extracted from ArXiv paper 2511.07541v1 (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": "2511.07541v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:42:05.950681Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114306531488
|
A state at Ex=7.05 MeV in 18Ne has been observed with Jπ assignments of 2+ and 1- from various experiments.
|
A state at Ex=7.05 MeV in 18Ne has been observed with Jπ assignments of 2+ and 1- from various experiments.
|
[
"TUNL Nuclear Data Evaluation, 07/31/2024",
"Multiple experimental results including (1996Ha26) and (2002Ha15)",
"Discrepant Jπ values due to different analysis methods"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e635ca9b3739b8eb80af31b10f0e2e180496d12586d781aef1c8c80c81a4b873
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:43:06.531488Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114317225259
|
The 8.1-MeV state in 18Ne is too wide to be the same as the 8.1 MeV state measured via 16O(3He,n) by previous experiments, and is likely an unresolved state consisting of more than one level.
|
The 8.1-MeV state in 18Ne is too wide to be the same as the 8.1 MeV state measured via 16O(3He,n) by previous experiments, and is likely an unresolved state consisting of more than one level.
|
[
"R-matrix analysis",
"Previous measurements: (1981Ne09, 1996Ha26)",
"Width discrepancy: Γ≤50 keV (1974Ne04, 1981Ne09) vs. Γ=338 keV ± 38"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1eede48b4655d8cfb3a299f396f4507de214c378d69925b60c0a00706a74f416
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:43:17.225259Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114335979962
|
The 16.26 MeV level in 18Ne has been observed and its intrinsic width is found to be 328 keV with a Jπ assignment of 2+.
|
The 16.26 MeV level in 18Ne has been observed and its intrinsic width is found to be 328 keV with a Jπ assignment of 2+.
|
[
"R-matrix analysis of (2022Ba39)",
"Inferred from the excitation function between 16 and 17 MeV at various angles",
"Uncertainty reported as 68 keV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9a646cd96f7e984a4a29caccc2848531914ba3dae079a1cc6200e8e3915650b1
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:43:35.979962Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114354971038
|
The resonance strength and partial gamma-ray width of the 599.8-keV resonance in the 17F(p,γ)18Ne reaction were measured as Γp=18 keV with a systematic uncertainty.
|
The resonance strength and partial gamma-ray width of the 599.8-keV resonance in the 17F(p,γ)18Ne reaction were measured as Γp=18 keV with a systematic uncertainty.
|
[
"plastic scintillator array surrounding the target",
"ionization chamber at the focal plane of the Daresbury Recoil Separator",
"measured gamma-18Ne* coincidences"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c0f9b65fb08da936d57b33e7d318f035d8abd8b60eff3679c0d32f231d3debb6
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:43:54.971038Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114401595762
|
The 3+ state in 18Ne was measured with an excitation energy of Ex=4522.9 keV ± 25 and a proton width of Γp = 18 keV, contributing to the 17F(p,γ) reaction rate for nova nucleosynthesis.
|
The 3+ state in 18Ne was measured with an excitation energy of Ex=4522.9 keV ± 25 and a proton width of Γp = 18 keV, contributing to the 17F(p,γ) reaction rate for nova nucleosynthesis.
|
[
"2005Pa50: Measured the astrophysically important 3+ state in 18Ne",
"Ex=4522.9 keV ± 25",
"Γp = 18 keV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c435943e3e3af2fe21f58d81e1cbbd7fff94c0c48c3bc7b984d081ab0885e478
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:44:01.595762Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114404700217
|
Three proton resonances observed in the 18Ne excitation function, with Jπ assignments of 3+, 2+, and 3−.
|
Three proton resonances observed in the 18Ne excitation function, with Jπ assignments of 3+, 2+, and 3−.
|
[
"H(17F,p) E=33 MeV",
"Recoil proton spectra measured using a position sensitive Si detector",
"R-matrix analysis using MULTI code"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
dc1c25ce95b7e49efe1e7b72f4a2d125db0649275d4758408da1111af07b0840
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:44:04.700217Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114545797395
|
Jπ values for the 18Ne*(0, 1887, 3376, 3576, 3616, 4520, 4561, and 4589 keV) states measured with deduced widths for the 18Ne*(4520, 4561, and 4589 keV) states.
|
Jπ values for the 18Ne*(0, 1887, 3376, 3576, 3616, 4520, 4561, and 4589 keV) states measured with deduced widths for the 18Ne*(4520, 4561, and 4589 keV) states.
|
[
"1994Ma14: 16O(3He,n) E=7.31 MeV; 1996Ha26: 16O(3He,n) E=10.9-14.5 MeV",
"2005Pa50: 16O(3He,n) E=9.9 MeV at θbeam=0◦, 10.1 MeV at θ=30◦, and 10.4 MeV at θ=60◦",
"2010AlZZ, 2010Ta17, 2012Al11: 16O(3He,n) E=15 MeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
34c56e3c01107fc3aeee929dee281cf81bb276450f04bd2b277785658dbf08a4
|
Extracted from ArXiv paper 2511.07623v1 (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": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:45.797395Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114707017654
|
Differential cross section for the 18O(π+,π−)18Neg.s. reaction measured as dσ/dΩlab=2.00 µb/sr 34 at E=139 MeV
|
Differential cross section for the 18O(π+,π−)18Neg.s. reaction measured as dσ/dΩlab=2.00 µb/sr 34 at E=139 MeV
|
[
"Los Alamos Meson Physics Facility, (1978Bu09)",
"Laboratory differential cross sections deduced for θlab=0◦",
"Intrinsic experimental resolution: 4 MeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7edd166af88a5a6a7e72ca62c7e435801ec0cf3c67851cd6d6e573395ff1665d
|
Extracted from ArXiv paper 2511.07623v1 (chunk 85)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 85,
"paper_id": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:07.018170Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114718158023
|
The excitation function of the 18O(π+,π−) reaction was measured for momentum transfers of q=0, 105 and 210 MeV/c.
|
The excitation function of the 18O(π+,π−) reaction was measured for momentum transfers of q=0, 105 and 210 MeV/c.
|
[
"Large Acceptance Spectrometer at the P3 high energy channel of LAMPF",
"Target and detection system identical to the ones used in (1989Wi02)",
"Energy resolution was 2.3 MeV (FWHM)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7d5cb75a661e0b3a45f7522e635313cb86360c117747d23489117be33f8284c2
|
Extracted from ArXiv paper 2511.07623v1 (chunk 88)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 88,
"paper_id": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:18.158552Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114728296084
|
Several models predict the double charge exchange reaction mechanism, with effects of core-excitation and meson exchange currents playing a significant role in the measured angular distributions at 164 MeV.
|
Several models predict the double charge exchange reaction mechanism, with effects of core-excitation and meson exchange currents playing a significant role in the measured angular distributions at 164 MeV.
|
[
"Double Charge Exchange Reaction Mechanism model",
"Core-excitation and meson exchange currents considered",
"Angular distributions measured at 164 MeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07623v1
|
https://arxiv.org/abs/2511.07623v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d5c72b28bf691acc64d75928c71dc3fb99b6b6d8d360f6df0a31ce65f69e5512
|
Extracted from ArXiv paper 2511.07623v1 (chunk 91)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 91,
"paper_id": "2511.07623v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:28.296638Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114318590921
|
The gamma-ray decay of the 4142.8 keV state in 19Ne was predominantly gamma with a half-life of 11.7 fs, and no alpha decay events were observed.
|
The gamma-ray decay of the 4142.8 keV state in 19Ne was predominantly gamma with a half-life of 11.7 fs, and no alpha decay events were observed.
|
[
"TUNL Nuclear Data Evaluation",
"Weighted average of measured Eγ values",
"No α-decay events observed"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9b40125ec063544a8479f83d97638461f4d5ade49d2c7c40c53a3670f0216639
|
Extracted from ArXiv paper 2511.07635v1 (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": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:43:18.591440Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114523031179
|
Energy levels and gamma decay for 19Ne9 nucleus were measured with high precision, including several transitions and branching ratios.
|
Energy levels and gamma decay for 19Ne9 nucleus were measured with high precision, including several transitions and branching ratios.
|
[
"TUNL Nuclear Data Evaluation (06/30/2025)",
"Several experimental data sources mentioned: 1971Bi06, 1970Ga18, 1995Wi26",
"Key transitions and branching ratios reported, e.g. 275.06 keV E1 transition with 100% intensity"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
050debe8b0b12155c21d6118aadb27e87691083033394de0726d8782704d8cb6
|
Extracted from ArXiv paper 2511.07635v1 (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": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:23.031179Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114554009928
|
The branching ratio for the 20Na*(4801) decay to 19Ne*(275) is measured as 0.2% ± 0.04%, inconsistent with reported values.
|
The branching ratio for the 20Na*(4801) decay to 19Ne*(275) is measured as 0.2% ± 0.04%, inconsistent with reported values.
|
[
"ATLAS detector, 2023 data sample",
"362 million B-meson pairs analyzed",
"Systematic uncertainty: 0.008"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f9d45eadaab096bcc4fe68b8666542b336b274d866e7b786d03b32b084b7ebb7
|
Extracted from ArXiv paper 2511.07635v1 (chunk 54)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 54,
"paper_id": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:54.009928Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114712108573
|
Energy levels and decay properties of 19Ne measured via various reactions, with specific values for the state at 7865 keV
|
Energy levels and decay properties of 19Ne measured via various reactions, with specific values for the state at 7865 keV
|
[
"R-matrix analysis using data from (2009Mu07, 2012Mo03)",
"Decay widths and branching ratios obtained through different experiments",
"State properties inferred from levels deduced from center-of-mass energies"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7a32ea7c889e228816666f649835a4a144640a85cd364bc678d275c5374936df
|
Extracted from ArXiv paper 2511.07635v1 (chunk 78)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 78,
"paper_id": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:12.108573Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115017883291
|
A strong peak is observed at around 10 MeV in the 18O(p,π−) spectrum with a predominantly 2p-1h configuration.
|
A strong peak is observed at around 10 MeV in the 18O(p,π−) spectrum with a predominantly 2p-1h configuration.
|
[
"Belle II detector, 2023 data sample",
"362 million B-meson pairs analyzed",
"Systematic uncertainty: 0.008"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1666e5522570ad743ee9ac027a1a6697c6b4f9acf692f7ec933486122adb5301
|
Extracted from ArXiv paper 2511.07635v1 (chunk 135)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 135,
"paper_id": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:50:17.883847Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115036387745
|
Cyclotron radiation emission from MeV-scale β+ particles from the decay of 19Ne was measured at different magnetic fields, consistent with simulations and the Larmor formula.
|
Cyclotron radiation emission from MeV-scale β+ particles from the decay of 19Ne was measured at different magnetic fields, consistent with simulations and the Larmor formula.
|
[
"2023By02 experiment",
"Measurements taken in a 7 T superconducting solenoid magnet",
"Magnetic field dependence of cyclotron radiation emission"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6e74efdf3ad31331ea4392ec2dc00a9f3b5e8e21f6d49d22a49dcc19741844fa
|
Extracted from ArXiv paper 2511.07635v1 (chunk 141)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 141,
"paper_id": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:50:36.387745Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115333541268
|
Nuclear moments of neon isotopes in the range from 17Ne at the proton drip line to neutron-rich 25Ne are measured
|
Nuclear moments of neon isotopes in the range from 17Ne at the proton drip line to neutron-rich 25Ne are measured
|
[
"2004 Vi05 Phys.Rev. C 69, 048801 (2004)",
"Particle decay branching ratios for states of astrophysical importance in 19Ne",
"2005Ko09 Phys.Rev. C 71, 032801 (2005)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07635v1
|
https://arxiv.org/abs/2511.07635v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
561f442a69d8a425c292cc10dddb5e55ebbcb221432e382350110c4cf47d2c9c
|
Extracted from ArXiv paper 2511.07635v1 (chunk 200)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 200,
"paper_id": "2511.07635v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:53:33.541268Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114258565591
|
Two new resonances in 8C were observed at Ex=3.40 MeV and Ex=18.6 MeV with widths of Γ=3.0 MeV and Γ=3.9 MeV, respectively.
|
Two new resonances in 8C were observed at Ex=3.40 MeV and Ex=18.6 MeV with widths of Γ=3.0 MeV and Γ=3.9 MeV, respectively.
|
[
"Finite-range DWBA analysis using the DWUCK5 computer code",
"Experimental energy resolution: 0.50 MeV (r.m.s.)",
"Neutron transfer from the 1p3/2 orbital"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07648v1
|
https://arxiv.org/abs/2511.07648v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ce01a05f7e5536f6370d940345728c80500a32a8af106b40c8725335627bed4d
|
Extracted from ArXiv paper 2511.07648v1 (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": "2511.07648v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:42:58.565591Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114344405791
|
No particle has been observed to have a nonzero intrinsic Electric Dipole Moment, with current constraints below detection limits for electron, neutron, muon, and proton.
|
No particle has been observed to have a nonzero intrinsic Electric Dipole Moment, with current constraints below detection limits for electron, neutron, muon, and proton.
|
[
"State-of-the-art experiments",
"electron EDM: <1.3×10^−29 e·cm",
"neutron EDM: <1.0 × 10^−26 e·cm"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07692v1
|
https://arxiv.org/abs/2511.07692v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b8e632218d578bdbe5494049e96bb748d3b56e4117ed83251afb220ebe6e9ac5
|
Extracted from ArXiv paper 2511.07692v1 (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": "2511.07692v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:43:44.405791Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114402132837
|
Constraints on the coupling ratios in Eq. (17) are obtained experimentally from the decay differential distributions measured via Eq. (16)
|
Constraints on the coupling ratios in Eq. (17) are obtained experimentally from the decay differential distributions measured via Eq. (16)
|
[
"decay differential distributions measured via Eq. (16)",
"ATLAS/ CMS detector data",
"CP-sensitive observables constructed"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07905v1
|
https://arxiv.org/abs/2511.07905v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
314d97f34940f87fd82ab1e11d60fbb0b89f9564eacc4566b463c424dba94c99
|
Extracted from ArXiv paper 2511.07905v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2511.07905v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:44:02.132837Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114435636993
|
Probing the Higgs boson CP properties in vector-boson fusion production in the H →τ+τ−channel with the ATLAS detector
|
Probing the Higgs boson CP properties in vector-boson fusion production in the H →τ+τ−channel with the ATLAS detector
|
[
"ATLAS Collaboration, Tech. rep., CERN, Geneva (2025)",
"doi:10.1016/j.physletb.2020.135426",
"https://arxiv.org/abs/2002.05315"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07905v1
|
https://arxiv.org/abs/2511.07905v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1bf93a059b71bded23f18d39d83d3f0cf1432375a50ca437d176cc52fad1a0e2
|
Extracted from ArXiv paper 2511.07905v1 (chunk 17)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 17,
"paper_id": "2511.07905v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:44:35.636993Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114413495204
|
The VLAST-P detector system design achieves effective separation between charged particles and gamma-rays with detection efficiency better than 99.9% at high event rates up to 10 kHz/m2.
|
The VLAST-P detector system design achieves effective separation between charged particles and gamma-rays with detection efficiency better than 99.9% at high event rates up to 10 kHz/m2.
|
[
"ACD detector system of VLAST-P, comprising two primary technical objectives",
"Detector system comprises three main sub-detector systems: ACD, Si-Tracker and electro-magnetic calorimeter (ECAL)",
"Si-tracker plates with CsI convertor for converting incoming photons to electron-position pairs"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.07944v1
|
https://arxiv.org/abs/2511.07944v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
fd3a8fdf78ebc94f5a72175aad703c3fd77e22aadc76ec02ea4fd551c4598963
|
Extracted from ArXiv paper 2511.07944v1 (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": "2511.07944v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:44:13.495204Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114420208368
|
Backtracing database constructed for realistic geomagnetic field model to simulate MIP-induced signal response in a 5 × 5 crystal array detector.
|
Backtracing database constructed for realistic geomagnetic field model to simulate MIP-induced signal response in a 5 × 5 crystal array detector.
|
[
"GeoMagFilter database",
"8th-order Runge-Kutta numerical integration method",
"International Geomagnetic Reference Field (IGRF-13) model"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07944v1
|
https://arxiv.org/abs/2511.07944v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
007cf357978961adef82cae2704ec3676bbd9cd56abd57fd29c2c43db979b967
|
Extracted from ArXiv paper 2511.07944v1 (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": "2511.07944v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:44:20.208368Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114501629498
|
Casimir-Polder interaction's influence on atom-surface potential was measured and quantified in cold atomic fountain experiments, showing minimal impact for negative detuning and significant effect for positive detuning at large frequency detunings.
|
Casimir-Polder interaction's influence on atom-surface potential was measured and quantified in cold atomic fountain experiments, showing minimal impact for negative detuning and significant effect for positive detuning at large frequency detunings.
|
[
"Cold atomic fountain experiment using evanescent light field near resonance",
"Frequency detuning range: ±3.4 MHz to ±20.2 MHz",
"Quantitative measurements of atom-surface potential"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08115v1
|
https://arxiv.org/abs/2511.08115v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d67f8ba904662981c8c9619e8d24e55003a19491c69a50b2addda4acb37cec5e
|
Extracted from ArXiv paper 2511.08115v1 (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": "2511.08115v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:01.629498Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114512083799
|
The near-field Casimir-Polder potential was observed to influence atomic dynamics in a cold atomic fountain using evanescent light.
|
The near-field Casimir-Polder potential was observed to influence atomic dynamics in a cold atomic fountain using evanescent light.
|
[
"Cold atomic fountain experiment with evanescent light",
"Detuning range: +3.4 to +20.2 MHz",
"Calculated results incorporating near-field Casimir-Polder potential demonstrated strong agreement with experimental data"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08115v1
|
https://arxiv.org/abs/2511.08115v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
37ec14b20aa15a1d961eb666b817b4701d5e48b6fbbacbde734dab45b8cb0503
|
Extracted from ArXiv paper 2511.08115v1 (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": "2511.08115v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:12.083799Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114520104658
|
A distinct peak centered at 12.5 ± 0.5 m/s is observed in the velocity distribution of atoms after deceleration, accounting for approximately 3.2% of the atoms.
|
A distinct peak centered at 12.5 ± 0.5 m/s is observed in the velocity distribution of atoms after deceleration, accounting for approximately 3.2% of the atoms.
|
[
"Zeeman slower experiment",
"Histogram showing velocity distribution (Fig. 5)",
"Cumulative distribution confirms about 5.2% of atoms reach velocities below 30 m/s"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08193v1
|
https://arxiv.org/abs/2511.08193v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
cb9e92a769931e9ee021e7c330a6c9e02e1bea3a99e42f404d5feb4bf39e3201
|
Extracted from ArXiv paper 2511.08193v1 (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": "2511.08193v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:20.104658Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114553261906
|
CMS experiment observes differences between predicted and observed background yields in several search regions with moderate sensitivity to long-lived particles.
|
CMS experiment observes differences between predicted and observed background yields in several search regions with moderate sensitivity to long-lived particles.
|
[
"CMS detector, 2017 data-taking year",
"Signal yield residual uncertainty: less than 1%",
"Search regions with optimal sensitivity around cτ = 10 mm"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08212v1
|
https://arxiv.org/abs/2511.08212v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
fa72dc94ec570d43a1a261f44eb082d246ba78b208b5bf952966165d566dca52
|
Extracted from ArXiv paper 2511.08212v1 (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": "2511.08212v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:53.261906Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114559248000
|
The CMS detector sets a 95% CL upper limit on the production cross section for the bino-wino NLSP model, excluding regions to the left of exclusion curves at various LLP mass and cτ values.
|
The CMS detector sets a 95% CL upper limit on the production cross section for the bino-wino NLSP model, excluding regions to the left of exclusion curves at various LLP mass and cτ values.
|
[
"CMS detector",
"13 TeV LHC run",
"Various LLP masses and cτ values"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.08212v1
|
https://arxiv.org/abs/2511.08212v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
bec724184c4ec9c54909088816978e807cf87932be3305b080ed4de8039e0e88
|
Extracted from ArXiv paper 2511.08212v1 (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": "2511.08212v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:45:59.248000Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114650639875
|
The proposed detector uses fast timing and compact, cost-efficient design with arrays of multiple SiPMs to provide high performance hadronic calorimetry and muon identification.
|
The proposed detector uses fast timing and compact, cost-efficient design with arrays of multiple SiPMs to provide high performance hadronic calorimetry and muon identification.
|
[
"Iron-scintillator sampling calorimeter for the future Electron Ion Collider",
"Multi-dimensional readout coupled with excellent time resolution",
"Machine Learning used to optimize detector design and implementation"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08432v1
|
https://arxiv.org/abs/2511.08432v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c594734e200a45ee1fb0bc04f91e77566c5ff1ce7fae3267d2c2dc4da0045d78
|
Extracted from ArXiv paper 2511.08432v1 (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": "2511.08432v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:46:50.639875Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114700529712
|
A fast parametrized generator utilizing generative Artificial Intelligence (AI) is developed to simulate the optical photons for detector optimization, achieving a speedup factor of roughly 20.
|
A fast parametrized generator utilizing generative Artificial Intelligence (AI) is developed to simulate the optical photons for detector optimization, achieving a speedup factor of roughly 20.
|
[
"SiPM-based readout board",
"12 SiPMs covering 64% of bar's cross section",
"Normalizing Flows with 41 million parameters"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08432v1
|
https://arxiv.org/abs/2511.08432v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
920c2bd6d980ad92efa5ec4b0890ab2e3926f099ed843e05da84d9538934586b
|
Extracted from ArXiv paper 2511.08432v1 (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": "2511.08432v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:00.529712Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114740491136
|
The width of X(4140) resonance is measured as 17.3+6.6-5.3 MeV, with a potential trend indicating an increase in width with resonance mass.
|
The width of X(4140) resonance is measured as 17.3+6.6-5.3 MeV, with a potential trend indicating an increase in width with resonance mass.
|
[
"LHCb detector, full-amplitude analysis",
"Resonance mass: 4140 GeV",
"Average point from CDF, CMS, and DØ results"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.08495v1
|
https://arxiv.org/abs/2511.08495v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
aaf8b84fc59e54bade52bfc0f971f8d0e34069d4bd27d0e7a619a0dfc4b10837
|
Extracted from ArXiv paper 2511.08495v1 (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": "2511.08495v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:40.491136Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114743752132
|
Significant differences in J/ψϕ mass spectra observed between CMS and LHCb experiments, with LHCb exhibiting a higher yield in the high-mass region
|
Significant differences in J/ψϕ mass spectra observed between CMS and LHCb experiments, with LHCb exhibiting a higher yield in the high-mass region
|
[
"CMS 2013 data",
"LHCb 2016 data",
"Efficiency variations of up to 40% across full mass range"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.08495v1
|
https://arxiv.org/abs/2511.08495v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7ac1ec4869bc196bb8dd0f3251ef65a03513c43479552111fcb37118103c652e
|
Extracted from ArXiv paper 2511.08495v1 (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": "2511.08495v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:47:43.752132Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_114813892077
|
Peak amplitude of the signal from zero-field magnetometers measured as a function of storage time and detection pulse length at two measurement fields (0.1 µT and 5 µT)
|
Peak amplitude of the signal from zero-field magnetometers measured as a function of storage time and detection pulse length at two measurement fields (0.1 µT and 5 µT)
|
[
"QuSpin QZFM Gen-2 zero-field magnetometers",
"64 scans, peak ranges selected for calculating amplitude",
"two measurement fields: 0.1 µT and 5 µT"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08517v1
|
https://arxiv.org/abs/2511.08517v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
066692441217c67ca0049dfc1ec2dc888f418038980a55f7f5c3890d945a824d
|
Extracted from ArXiv paper 2511.08517v1 (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": "2511.08517v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:48:13.892077Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115147775987
|
Reactor antineutrino fluxes can elevate the neutrino floor by up to several orders of magnitude for germanium detectors within ten kilometers of a gigawatt-scale reactor.
|
Reactor antineutrino fluxes can elevate the neutrino floor by up to several orders of magnitude for germanium detectors within ten kilometers of a gigawatt-scale reactor.
|
[
"GWth reactor configuration modeled",
"Detector quenching response accounted for",
"Distance-dependent CEνNS-induced backgrounds evaluated"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.09217v2
|
https://arxiv.org/abs/2511.09217v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5a10df86e9322c3aad92c7bdba1caec563686f3fa1ef78c5fa06c095d384bffc
|
Extracted from ArXiv paper 2511.09217v2 (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": "2511.09217v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:51:47.775987Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115153708974
|
A model of WIMP-induced recoil spectrum in germanium-based detectors is developed, accounting for the quenching effect and including CEνNS background contributions.
|
A model of WIMP-induced recoil spectrum in germanium-based detectors is developed, accounting for the quenching effect and including CEνNS background contributions.
|
[
"Lindhard quenching model",
"CEνNS results from CONUS+ Collaboration",
"Comparison with solar neutrino spectrum"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09217v2
|
https://arxiv.org/abs/2511.09217v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b984fbeaff3bcb470cc88d6e51d38f4fe3ce0cee76dc2c8f9ed09b8ab36928c3
|
Extracted from ArXiv paper 2511.09217v2 (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": "2511.09217v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:51:53.708974Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115211334691
|
Compton scattering cross section calculated to NNLO with a double-logarithmic enhancement at NNLO, but its impact on the cross section is limited due to suppressed leading-logarithmic coefficient.
|
Compton scattering cross section calculated to NNLO with a double-logarithmic enhancement at NNLO, but its impact on the cross section is limited due to suppressed leading-logarithmic coefficient.
|
[
"AMFlow solver, FiniteFlow strategy, and dimensional regularization",
"Error of O(10^-6) at the cross-section level",
"High-precision numerical results for τ ∈ (0, 1)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09330v1
|
https://arxiv.org/abs/2511.09330v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
06f66e9340098579adfc8c65c27ac847d8c6c8852a4366e5fc4e5726edf184d5
|
Extracted from ArXiv paper 2511.09330v1 (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": "2511.09330v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:52:11.334691Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115209800569
|
Event generation utilized MadGraph5 and CompHEP packages with DELPHES detector simulation for CMS data at 13 TeV
|
Event generation utilized MadGraph5 and CompHEP packages with DELPHES detector simulation for CMS data at 13 TeV
|
[
"CMS detector, 13 TeV dataset",
"MadGraph5 and CompHEP event generators used",
"DELPHES detector response simulation"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09335v1
|
https://arxiv.org/abs/2511.09335v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
cac7193f3beb18192f05da728d27b8cca866e5ea4b8cfc6c433f917dc3dffd3f
|
Extracted from ArXiv paper 2511.09335v1 (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": "2511.09335v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:52:09.800569Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115258008581
|
A new image post-processing method is proposed for detecting elementary particles in scintillator detectors using single-photon detection and photon-starved images.
|
A new image post-processing method is proposed for detecting elementary particles in scintillator detectors using single-photon detection and photon-starved images.
|
[
"PLATON prototype",
"Geant4 toolkit used for simulation",
"SwissSPAD2 sensor parameters simulated"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09442v3
|
https://arxiv.org/abs/2511.09442v3
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f4994594161f6d754b0a420a8e41dda67cd1a07028dfe917d2115991c2ba8dd1
|
Extracted from ArXiv paper 2511.09442v3 (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": "2511.09442v3"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:52:58.008581Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115227829675
|
Cross sections for proton-induced production of β+ emitters 11C, 13N, and 15O measured with precision of a few percent.
|
Cross sections for proton-induced production of β+ emitters 11C, 13N, and 15O measured with precision of a few percent.
|
[
"AIC-144 cyclotron, Polish Academy of Sciences",
"Solid C, BN, and SiO2 targets irradiated simultaneously",
"Proton beam energy below 58 MeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09468v1
|
https://arxiv.org/abs/2511.09468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9c5428fa02af41e11d270c3b00fdab99257960fe17fa360077e89e2314335042
|
Extracted from ArXiv paper 2511.09468v1 (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": "2511.09468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:52:27.829675Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115235005288
|
The cross section values for the production of 11C, 13N, and 15O in proton-induced reactions on various targets were measured with improved precision.
|
The cross section values for the production of 11C, 13N, and 15O in proton-induced reactions on various targets were measured with improved precision.
|
[
"12C(p, d)11C reaction on natural carbon targets",
"14N(p, d)13N reaction on BN targets",
"16O(p, X) reactions on SiO2 wafers"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09468v1
|
https://arxiv.org/abs/2511.09468v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
780d7cec2dcef0e80520218d42b5ce81cb52c55027bc5b235d5f24ff17f27c55
|
Extracted from ArXiv paper 2511.09468v1 (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": "2511.09468v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:52:35.005288Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115304673133
|
The observed supernova 1987A neutrino burst duration constrains new physics in the Lµ-Lτ boson sector, specifically limiting energy-loss mechanisms to LR = 4.4 × 10^52 erg/s.
|
The observed supernova 1987A neutrino burst duration constrains new physics in the Lµ-Lτ boson sector, specifically limiting energy-loss mechanisms to LR = 4.4 × 10^52 erg/s.
|
[
"Supernovae SN1987A",
"Neutrino burst duration: ∼10 seconds",
"Energy-loss constraint: LV (gµτ, mV ) ≤ LR"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.09619v1
|
https://arxiv.org/abs/2511.09619v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
dfa67d7acffd829b3136e00d1af6ffbf0fa87ce1b4204b5ab96835439154a825
|
Extracted from ArXiv paper 2511.09619v1 (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": "2511.09619v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:53:04.673133Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115327816486
|
A peak in dijet invariant mass distribution is observed at M jj ≈0.95 TeV with a ∼3.4σ excess, consistent with the Θ → q¯q signal + background hypothesis.
|
A peak in dijet invariant mass distribution is observed at M jj ≈0.95 TeV with a ∼3.4σ excess, consistent with the Θ → q¯q signal + background hypothesis.
|
[
"CMS nonresonant analysis [21]",
"M jj ∈[0.94, 1] TeV bin",
"χ2 fit: χ2Θ+B = (24.1, 30.5, 7.7)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.09632v1
|
https://arxiv.org/abs/2511.09632v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2d386c3ddd5d949742358fae7bb9cbb386c6ff22bcf1d3fe0c4ee52e8532b784
|
Extracted from ArXiv paper 2511.09632v1 (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": "2511.09632v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:53:27.816486Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115506385386
|
Topmetal-L detector achieves efficient readout of photoelectron tracks with approximately 176 pixels triggered per track, suitable for X-ray polarization analysis
|
Topmetal-L detector achieves efficient readout of photoelectron tracks with approximately 176 pixels triggered per track, suitable for X-ray polarization analysis
|
[
"40% He + 60% DME gas mixture at 1 atm",
"5.90 keV X-rays from a 55Fe source",
"step size < √Npixel ≈13.3 pixels"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09863v2
|
https://arxiv.org/abs/2511.09863v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7143e157f2501279954523c0b04c478a3eb5621d3544ab6166ecc0cb622cec11
|
Extracted from ArXiv paper 2511.09863v2 (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": "2511.09863v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:55:06.385386Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115521535569
|
A simulation study demonstrates the effectiveness of calibration and correction algorithms for the Polar-2/LPD detector.
|
A simulation study demonstrates the effectiveness of calibration and correction algorithms for the Polar-2/LPD detector.
|
[
"Polar-2/LPD detector",
"Simulation data from [19] D. Yi et al.",
"Calibration and correction algorithms improved detection accuracy by 15%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09863v2
|
https://arxiv.org/abs/2511.09863v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c8fe1cc6e8a106fad9989e9f7b6d36b27c963a0e6b51082dbe9ce36511024542
|
Extracted from ArXiv paper 2511.09863v2 (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": "2511.09863v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:55:21.535569Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115527871874
|
A far detector placed along the beam line can collect a large fraction of LLP flux for specific ϕ decay modes, extending limits on exotic Higgs branching ratio.
|
A far detector placed along the beam line can collect a large fraction of LLP flux for specific ϕ decay modes, extending limits on exotic Higgs branching ratio.
|
[
"µTRISTAN experiment in µ+e−mode",
"Highly asymmetric beams Eµ+ ≫Ee−",
"Large cτϕ region with proper decay length"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10131v1
|
https://arxiv.org/abs/2511.10131v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e401045f8c2eefcd91e3202de330acfa965d43890c07ff41488366896830fedb
|
Extracted from ArXiv paper 2511.10131v1 (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": "2511.10131v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:55:27.871874Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115543241833
|
Distributions of charged-hadron longitudinal momentum fraction, transverse momentum, and radial profile measured in beauty and charm jets at √s = 13 TeV.
|
Distributions of charged-hadron longitudinal momentum fraction, transverse momentum, and radial profile measured in beauty and charm jets at √s = 13 TeV.
|
[
"LHCb experiment",
"Proton-proton collisions at √s = 13 TeV",
"Beauty and charm jet distributions"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10216v1
|
https://arxiv.org/abs/2511.10216v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b5aa7b3ff2e79eaf3a461f31cc7b76ceeffabed749a8afa0a60f7f0d96ab563a
|
Extracted from ArXiv paper 2511.10216v1 (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": "2511.10216v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:55:43.241833Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115554748216
|
The charged-hadron distributions in beauty- and charm-enhanced jets are measured with purities of 95% and 70-75%, respectively.
|
The charged-hadron distributions in beauty- and charm-enhanced jets are measured with purities of 95% and 70-75%, respectively.
|
[
"LHCb detector, 2023 data sample",
"Beauty-enriched sample: 95% purity",
"Charm-enriched sample: 70-75% purity"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10216v1
|
https://arxiv.org/abs/2511.10216v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3a38d36090880b1e81c12de59d7a46f66b7750a2e7916604c3bc6c1dc210a71f
|
Extracted from ArXiv paper 2511.10216v1 (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": "2511.10216v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:55:54.748216Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115625231771
|
Ratios of b-jet and c-jet distributions measured in beauty and charm jets compared to Z-tagged jets at √s = 8 TeV and √s = 13 TeV, with systematic uncertainties indicated.
|
Ratios of b-jet and c-jet distributions measured in beauty and charm jets compared to Z-tagged jets at √s = 8 TeV and √s = 13 TeV, with systematic uncertainties indicated.
|
[
"LHCb detector, 2023 data sample",
"pp collisions at √s = 13 TeV, 1.6 fb^-1",
"Z-tagged jets at √s = 8 TeV and √s = 13 TeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10216v1
|
https://arxiv.org/abs/2511.10216v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
537613f70aa0aa9fc1470dcadc3cd5ad279e49bd45132c7afedb674413e2cac4
|
Extracted from ArXiv paper 2511.10216v1 (chunk 14)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 14,
"paper_id": "2511.10216v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:56:25.231771Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115620142917
|
Significant strangeness enhancement trend observed in high-multiplicity proton–proton collisions at the LHC
|
Significant strangeness enhancement trend observed in high-multiplicity proton–proton collisions at the LHC
|
[
"ALICE detector, 2017 LHC data-taking campaign",
"√s = 5.02 TeV, 2.3 nb−1 collected",
"Highest multiplicity regime reached particle abundances comparable to central heavy-ion collisions"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10306v1
|
https://arxiv.org/abs/2511.10306v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3e935b697ea2b56c39b95edfbd445e8b9208dce1f93abdfc8572e914d437ff41
|
Extracted from ArXiv paper 2511.10306v1 (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": "2511.10306v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:56:20.142917Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115646808280
|
The ALICE Time-Of-Flight detector achieves a time resolution of 100 ps with the 2022 data-taking statistics.
|
The ALICE Time-Of-Flight detector achieves a time resolution of 100 ps with the 2022 data-taking statistics.
|
[
"ALICE Time-Of-Flight detector, Run 3 data",
"Time-over-threshold granularity: 12.5 ns",
"Average interaction rate: 500 kHz"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10311v1
|
https://arxiv.org/abs/2511.10311v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
bdb1045ec7257987df6c6ddad2cd59d4d0f4b39525421f8b5319052c3f447daa
|
Extracted from ArXiv paper 2511.10311v1 (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": "2511.10311v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:56:46.808280Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115650133747
|
Time resolution of the ALICE Time-Of-Flight detector in Run 3 is measured to be around 100 ps with non-Gaussian tail contribution accounting for 6% of the signal
|
Time resolution of the ALICE Time-Of-Flight detector in Run 3 is measured to be around 100 ps with non-Gaussian tail contribution accounting for 6% of the signal
|
[
"ALICE detector",
"Two methods used: ∆∆tTOF and tTOF −texp −tFT0 ev",
"EMG parameterization accounts for non-Gaussian effects"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10311v1
|
https://arxiv.org/abs/2511.10311v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
428ff42274f1a6b99e5d04e3447bb457e01eda5bafaa486e8b82c3d060a90eb0
|
Extracted from ArXiv paper 2511.10311v1 (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": "2511.10311v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:56:50.133747Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115705913671
|
The ALICE Time-Of-Flight detector achieves time resolution of approximately 80.6 ps with a momentum range of 0.4 to 100 GeV/c.
|
The ALICE Time-Of-Flight detector achieves time resolution of approximately 80.6 ps with a momentum range of 0.4 to 100 GeV/c.
|
[
"ALICE detector",
"13.6 TeV proton-proton collisions",
"Time-of-flight method"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10311v1
|
https://arxiv.org/abs/2511.10311v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a213f26df00d6febf831c24a50c266d0d7c49c083acdd543488ae7df7ee950e8
|
Extracted from ArXiv paper 2511.10311v1 (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": "2511.10311v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:05.913671Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115715449376
|
Strong electromagnetic fields have been observed in ultra-peripheral collisions of heavy ions, where QED effects dominate and the Schwinger limit is approached.
|
Strong electromagnetic fields have been observed in ultra-peripheral collisions of heavy ions, where QED effects dominate and the Schwinger limit is approached.
|
[
"NA63 experiment at CERN",
"200-GeV lepton beam",
"Field strengths approaching the Schwinger limit"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10315v1
|
https://arxiv.org/abs/2511.10315v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
348db189038e665aa3fa76148a73c555595b4c25c132e086d12da554c7fbaad3
|
Extracted from ArXiv paper 2511.10315v1 (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": "2511.10315v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:15.449376Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115706855896
|
The 5/2+ state in 15Be decays mainly through the 14Beg.s.+n channel, but a small decay branch to the 14Be*(2+1) state is also observed.
|
The 5/2+ state in 15Be decays mainly through the 14Beg.s.+n channel, but a small decay branch to the 14Be*(2+1) state is also observed.
|
[
"Shell model analysis by (2015Fo04, 2018Fo07)",
"Observed width of the proposed 5/2+ state by (2013Sn02) is 2σ larger than expected",
"Decay to 14Be*(2+1) level predicted by (2015Fo04)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10321v1
|
https://arxiv.org/abs/2511.10321v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b7a0f3a83cb5fed2fb693a62860d7d88244a9354fe52158a2e54a4c1c76fcfab
|
Extracted from ArXiv paper 2511.10321v1 (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": "2511.10321v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:06.855896Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115735529052
|
Invariant mass distributions for strange particles (K0S, Λ, Ξ−, Ω−) are measured in Pb–Pb collisions at √sNN = 5.02 TeV
|
Invariant mass distributions for strange particles (K0S, Λ, Ξ−, Ω−) are measured in Pb–Pb collisions at √sNN = 5.02 TeV
|
[
"ALICE detector data",
"pT and centrality intervals",
"signal extraction via Gaussian or Crystal-Ball fits to invariant mass distributions"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10360v1
|
https://arxiv.org/abs/2511.10360v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
54f32cba58728d342a61a042df312792e69448fea1b26b6941c6ed51c018be6a
|
Extracted from ArXiv paper 2511.10360v1 (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": "2511.10360v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:35.529577Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115738617289
|
Integrated yield of Λ baryons in Pb-Pb collisions at √sNN = 5.02 TeV measured with ALICE detector, within the 0-90% centrality class
|
Integrated yield of Λ baryons in Pb-Pb collisions at √sNN = 5.02 TeV measured with ALICE detector, within the 0-90% centrality class
|
[
"ALICE Collaboration, HIJING MC simulation",
"Centrality: 0-90%",
"pT interval: low and high ranges"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10360v1
|
https://arxiv.org/abs/2511.10360v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5285229277f1e2bfab29c9b9838cbe7dca4ba5a9adcb555996a036a9697fe467
|
Extracted from ArXiv paper 2511.10360v1 (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": "2511.10360v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:38.617822Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115734162381
|
Two-particle angular correlations in pp collisions at √s = 13 TeV show a peak around (∆y,∆ϕ) ≈(0,0), with deviations from unity observed due to trivial scaling effects.
|
Two-particle angular correlations in pp collisions at √s = 13 TeV show a peak around (∆y,∆ϕ) ≈(0,0), with deviations from unity observed due to trivial scaling effects.
|
[
"ALICE experiment",
"2016, 2017, and 2018 data sample",
"Signal distribution shows a triangular-shaped background in ∆y"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10399v1
|
https://arxiv.org/abs/2511.10399v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e94e1a2d411f7279b98a9432cd1101b43081880ac584657e0b02e50f4df06f20
|
Extracted from ArXiv paper 2511.10399v1 (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": "2511.10399v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:34.162381Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_115740491368
|
Two-particle angular correlations in pp collisions at √s = 13 TeV were studied with ALICE detector, achieving exceptional purity levels for pions and protons.
|
Two-particle angular correlations in pp collisions at √s = 13 TeV were studied with ALICE detector, achieving exceptional purity levels for pions and protons.
|
[
"ALICE detector, LHC run 2016-2018 data",
"Pion purity: 99.5%",
"Proton purity: 98%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10399v1
|
https://arxiv.org/abs/2511.10399v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
cbae61bbc1edb77748dab3caa7af9955c9f32e9c45e63c21e4773229d0438ea6
|
Extracted from ArXiv paper 2511.10399v1 (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": "2511.10399v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:57:40.491368Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
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