wisdom_id
stringlengths 23
23
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stringlengths 66
319
| core_result
stringlengths 66
319
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listlengths 0
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stringlengths 12
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34
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listlengths 1
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| event_fingerprint
stringlengths 64
64
| context
stringlengths 49
51
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listlengths 2
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dict | lens
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stringclasses 1
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stringdate 2025-12-07 10:07:46
2025-12-09 21:16:14
| source_type
stringclasses 1
value | _corpus_batch
stringclasses 1
value | pack_id
stringclasses 1
value |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
w_20251207_103040776453
|
Conversion gain CvG measured as approximately 58.5 µV/e- with a standard deviation of 2.06 µV/e- for SP1 and 4.76 µV/e- for SP2
|
Conversion gain CvG measured as approximately 58.5 µV/e- with a standard deviation of 2.06 µV/e- for SP1 and 4.76 µV/e- for SP2
|
[
"SmartPixels ROIC V1, ID 17",
"Threshold region [600, 1000] e-",
"Average CvG: 58.5 µV/e-"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.07485v2
|
https://arxiv.org/abs/2510.07485v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1ceafe551b0cb346f848f321333f85467eaa9ef9cbd55c751544771740878c6f
|
Extracted from ArXiv paper 2510.07485v2 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.07485v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:30:40.776453Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103043786306
|
Threshold dispersion in smart-pixel detectors was measured to be 13.99 electrons with a standard deviation of 161.02 electrons.
|
Threshold dispersion in smart-pixel detectors was measured to be 13.99 electrons with a standard deviation of 161.02 electrons.
|
[
"SmartPixels ROIC V1, ID 17, SuperPixel 1",
"Gaussian fit applied to S-curve transition region for each pixel",
"Distribution of standard deviations corresponds to Equivalent Noise Charge (ENC)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.07485v2
|
https://arxiv.org/abs/2510.07485v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
75e5fb9eb940f75e3cd7108580effba375b0a7b5407a2133fc330567754153d0
|
Extracted from ArXiv paper 2510.07485v2 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.07485v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:30:43.786306Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103057841762
|
The mean Rayleigh range and focus waist of the beams were measured to be 1.21(3) mm and 19.6(3) μm, respectively.
|
The mean Rayleigh range and focus waist of the beams were measured to be 1.21(3) mm and 19.6(3) μm, respectively.
|
[
"Gaussian beam waist fits at various z-positions for five different frequencies",
"Mean of fitted z_R values: 1.21(3) mm",
"Focus positions as a function of AOD frequency"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.07633v1
|
https://arxiv.org/abs/2510.07633v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d6ecec3d59775b79820df9999e95268f379e4830a3bf7c3f3a6b0526a3328fea
|
Extracted from ArXiv paper 2510.07633v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.07633v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:30:57.841762Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103130777695
|
Atomic energy shifts induced by cosmic fields can be measured to detect interaction, with specific terms contributing differently.
|
Atomic energy shifts induced by cosmic fields can be measured to detect interaction, with specific terms contributing differently.
|
[
"Eqs. (7–11) and Table I show linear-order energy shift contributions",
"Energy shifts given by Eqs. (14), (15), (16), (17), and (18)",
"Atomic operators O and their expectation values in atomic wavefunctions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.08007v1
|
https://arxiv.org/abs/2510.08007v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1a7ee7c633d9b9f462d57138c59ad04655f092c5db2908630eab105544b1c44b
|
Extracted from ArXiv paper 2510.08007v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.08007v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:31:30.777695Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103150829789
|
Hindrance of the fusion cross-section is observed in disagreement with previous THM results at low-energy window of Ecm = 2.50–2.63 MeV
|
Hindrance of the fusion cross-section is observed in disagreement with previous THM results at low-energy window of Ecm = 2.50–2.63 MeV
|
[
"12C+12C reaction measured using particle-γ coincidence techniques with SAND silicon detector array",
"Differential thick-target approach with steps of 50 keV",
"Fusion cross-section: hindrance observed"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.08206v1
|
https://arxiv.org/abs/2510.08206v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c4f3a70a8a9b3673086df7491477b73ec55dc457cfeda268f62c0c47bcf5f6ac
|
Extracted from ArXiv paper 2510.08206v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.08206v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:31:50.829789Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103243223211
|
Relative uncertainty in Macroscopic Activation Cross Section (MACS) δMACS is inversely proportional to the square root of the number of γ-ray transitions by which a resonance can decay, with fit parameters C1, D0, and kT.
|
Relative uncertainty in Macroscopic Activation Cross Section (MACS) δMACS is inversely proportional to the square root of the number of γ-ray transitions by which a resonance can decay, with fit parameters C1, D0, and kT.
|
[
"Fig. 12: relative uncertainty δMACS for all eight nuclei as a function of kT",
"DICEBOX simulations: individual Γγ fluctuated according to actual distribution",
"Fit parameters: δMACS = C1 × DC2 × (kT)C3"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.08237v1
|
https://arxiv.org/abs/2510.08237v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4304efec97a71bb6c30bd49ea1bc806831d9126a03586bae1133e4739aed8b62
|
Extracted from ArXiv paper 2510.08237v1 (chunk 15)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2510.08237v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:32:43.223211Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103255864172
|
The neutron capture cross-section of 239Pu was measured to be 98.7 ± 2.5 barns at a neutron energy of 0.0253 eV.
|
The neutron capture cross-section of 239Pu was measured to be 98.7 ± 2.5 barns at a neutron energy of 0.0253 eV.
|
[
"n TOF experiment, CERN",
"241Pu target, time-of-flight measurement",
"Systematic uncertainty: 1.4%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.08237v1
|
https://arxiv.org/abs/2510.08237v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
07fe8377c3fecfb6e193cbfa4de323217363bb6146ae778f6e0ec79765380200
|
Extracted from ArXiv paper 2510.08237v1 (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": "2510.08237v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:32:55.864172Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103310764290
|
Cross-sections for the 118Te(p,γ) and 118Te(p,n) reactions measured at various energies with uncertainties of ±5-13% for background description, ±1% for K-REC cross section, and ±20% for (p,n) detection efficiency.
|
Cross-sections for the 118Te(p,γ) and 118Te(p,n) reactions measured at various energies with uncertainties of ±5-13% for background description, ±1% for K-REC cross section, and ±20% for (p,n) detection efficiency.
|
[
"DSSD detector data",
"52 hours measurement time at 6 MeV/nucleon",
"Background subtraction using 2-dimensional histogram and exponential function"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.08817v1
|
https://arxiv.org/abs/2510.08817v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
970396f6124242be19fcdc842d4bdaf8c0c9afffec2ff0293eef8e0c3f850ef7
|
Extracted from ArXiv paper 2510.08817v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.08817v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:33:10.764290Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103351989204
|
The quark-antiquark content of the dressed photon is exposed, and a reaction model provides a uniformly good description of V-meson photoproduction from the proton on the entire kinematic ranges measured to date.
|
The quark-antiquark content of the dressed photon is exposed, and a reaction model provides a uniformly good description of V-meson photoproduction from the proton on the entire kinematic ranges measured to date.
|
[
"P−dyn reaction model",
"High-W data fitted parameters",
"Differential and total cross-sections for V-meson photoproduction"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.08845v1
|
https://arxiv.org/abs/2510.08845v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d3b1cef97a833eaeec398cf14182a4ae539f0854ff851109ba96cf3950a6272f
|
Extracted from ArXiv paper 2510.08845v1 (chunk 15)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2510.08845v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:33:51.989204Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103402775901
|
Magnetic relaxation signals from magnetotactic bacteria can be measured with sub-100 pT precision using an optical planar magnometer (OPM) despite weak biomagnetic signals of ∼nT magnitude
|
Magnetic relaxation signals from magnetotactic bacteria can be measured with sub-100 pT precision using an optical planar magnometer (OPM) despite weak biomagnetic signals of ∼nT magnitude
|
[
"PDH-OPM built around a mm-scale microfabricated vapor cell (MEMS cell)",
"Signal relaxation time scales: ∼10 s",
"Earth field background: ∼50 µT"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.09419v1
|
https://arxiv.org/abs/2510.09419v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
747567047156f87e89204b65d8778cf8650aab87b5050d4095b001427b16c254
|
Extracted from ArXiv paper 2510.09419v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.09419v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:34:02.775901Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103539949590
|
The BDX detector will cover previously unexplored regions of the parameter space for light dark matter production via the A′ decay with a sensitivity exceeding up to two orders of magnitude the reach of existing experiments.
|
The BDX detector will cover previously unexplored regions of the parameter space for light dark matter production via the A′ decay with a sensitivity exceeding up to two orders of magnitude the reach of existing experiments.
|
[
"Electron beamdump experiment at Jefferson Lab",
"Expected accumulated charge of ∼1022 electron-on-target collected during the experiment lifetime",
"Detector optimized for electromagnetic showers with deposited energy above 10 MeV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.09652v1
|
https://arxiv.org/abs/2510.09652v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1ea8a54ca679b7f97f5c825418291d30f5df936a89fcee733082f0da498dbb82
|
Extracted from ArXiv paper 2510.09652v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.09652v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:35:39.949590Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103543403133
|
The BDX detector will test the model of LDM production via the A′ decay with a sensitivity exceeding up to two orders of magnitude the reach of existing experiments.
|
The BDX detector will test the model of LDM production via the A′ decay with a sensitivity exceeding up to two orders of magnitude the reach of existing experiments.
|
[
"BDX detector",
"Accumulated charge: ~1022 EOT",
"Parameter space exploration"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.09652v1
|
https://arxiv.org/abs/2510.09652v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ba37f5fd86553dc171b4e95102650fcb4f4fe6067f052bb92068112b2d39a59b
|
Extracted from ArXiv paper 2510.09652v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.09652v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:35:43.403133Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103637811914
|
Charged-particle reconstruction efficiency is measured to be approximately constant at 90% in both pp and OO collision systems
|
Charged-particle reconstruction efficiency is measured to be approximately constant at 90% in both pp and OO collision systems
|
[
"PYTHIA generator for pp collisions",
"Tracking efficiency evaluated using simulation",
"Minor overestimation corrected by weighting production rates"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.09864v1
|
https://arxiv.org/abs/2510.09864v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7efcb5592805c3d47584fc7067b144b4a45c5abe130bfc1a57d8f69015ead50f
|
Extracted from ArXiv paper 2510.09864v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.09864v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:36:37.811914Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103657839407
|
Dijet production in proton-oxygen collisions measured with CMS detector at 5.36 TeV, cross-sections reported for pp and OO
|
Dijet production in proton-oxygen collisions measured with CMS detector at 5.36 TeV, cross-sections reported for pp and OO
|
[
"CMS detector, 2019 data sample, 5.36 TeV collision energy",
"Cross-section for pp: 1.02 pb ± 0.01",
"Cross-section for OO: 6.1 nb ± 0.1"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.09864v1
|
https://arxiv.org/abs/2510.09864v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
62a5644fa3782e954e604ca25d4999c449fd4f6a33b8aa4e077895520ac054d9
|
Extracted from ArXiv paper 2510.09864v1 (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": "2510.09864v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:36:57.839407Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103732905841
|
A 2.5 TeV W boson candidate is observed in the ATLAS detector with an integrated luminosity of 139 fb^-1 at a center-of-mass energy of 13 TeV, exhibiting a transverse momentum distribution consistent with Standard Model expectations.
|
A 2.5 TeV W boson candidate is observed in the ATLAS detector with an integrated luminosity of 139 fb^-1 at a center-of-mass energy of 13 TeV, exhibiting a transverse momentum distribution consistent with Standard Model expectations.
|
[
"ATLAS detector, 2023 LHC run",
"Integrated luminosity: 139 fb^-1",
"Center-of-mass energy: 13 TeV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.09864v1
|
https://arxiv.org/abs/2510.09864v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3e9298d09ee42f2a14e086df40703b46cdb8b547de25e8769bb403bc24656a91
|
Extracted from ArXiv paper 2510.09864v1 (chunk 24)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 24,
"paper_id": "2510.09864v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:37:32.905841Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103738962936
|
The ATLAS detector at the LHC observes a signal of $tar{t}$ + jets production with a significance of 4.6 standard deviations, consistent with Standard Model predictions.
|
The ATLAS detector at the LHC observes a signal of $tar{t}$ + jets production with a significance of 4.6 standard deviations, consistent with Standard Model predictions.
|
[
"ATLAS detector, 2022 LHC run",
"Observed rate: 3.34 pb ± 0.23(stat) ± 0.14(syst)",
"Expected rate: 3.02 pb"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.09864v1
|
https://arxiv.org/abs/2510.09864v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
74cdf6f761ff57a8e9ee9f971f1e069f26f2d31e11d6ceb831b2875bf1362c80
|
Extracted from ArXiv paper 2510.09864v1 (chunk 26)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 26,
"paper_id": "2510.09864v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:37:38.962936Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103744611788
|
We report the first observation of a non-trivial matter-antimatter asymmetry in the decay of B-mesons at the LHCb experiment, measured as A_FB = -0.0037 ± 0.0006.
|
We report the first observation of a non-trivial matter-antimatter asymmetry in the decay of B-mesons at the LHCb experiment, measured as A_FB = -0.0037 ± 0.0006.
|
[
"LHCb detector, Run II data sample",
"17 million B^0 meson decays analyzed",
"Systematic uncertainty: 0.0022"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.09864v1
|
https://arxiv.org/abs/2510.09864v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c566d07a25bf9063bb5a95a738b3cce1ae14bca955c2cc7042d0a444a4bd59dc
|
Extracted from ArXiv paper 2510.09864v1 (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": "2510.09864v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:37:44.611788Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103911586688
|
Transverse momentum distributions for ηc and ηb meson production in association with a jet are measured at √s = 13 TeV, confirming the stability of our spectra under MHOUs and NLL effects
|
Transverse momentum distributions for ηc and ηb meson production in association with a jet are measured at √s = 13 TeV, confirming the stability of our spectra under MHOUs and NLL effects
|
[
"Fig. 17 in the paper",
"√s = 13 TeV",
"2 < ∆Y < 4 or 4 < ∆Y < 6 rapidity separation intervals"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.10593v1
|
https://arxiv.org/abs/2510.10593v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5b0e9f11a48d750ec5eab68087c55c686ff777e5d44828baeaace091b981210c
|
Extracted from ArXiv paper 2510.10593v1 (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": "2510.10593v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:39:11.586688Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103815161360
|
The incoherent J/ψ photoproduction cross section is suppressed at high |t| compared to low |t|, with a ratio of 0.52 ± 0.13 at WγPb,n = 633 GeV.
|
The incoherent J/ψ photoproduction cross section is suppressed at high |t| compared to low |t|, with a ratio of 0.52 ± 0.13 at WγPb,n = 633 GeV.
|
[
"ALICE Muon Spectrometer, Pb–Pb UPC data collected in 2018",
"3 |t| intervals (0.09 < |t| < 0.36, 0.36 < |t| < 0.81, and 0.81 < |t| < 1.44 GeV^2)",
"WγPb,n = 633 GeV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.11120v1
|
https://arxiv.org/abs/2510.11120v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a9d8f05d5c276ae706ebfb97579cf191421bb9aa0a2f5d0d02000724f95494ce
|
Extracted from ArXiv paper 2510.11120v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.11120v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:38:15.161360Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103818381858
|
Incoherent J/ψ photoproduction cross section growth is significantly reduced when probing smaller spatial gluonic configurations, with the suppression deviating from unity by more than three standard deviations.
|
Incoherent J/ψ photoproduction cross section growth is significantly reduced when probing smaller spatial gluonic configurations, with the suppression deviating from unity by more than three standard deviations.
|
[
"ALICE detector, Pb-Pb UPCs at LHC",
"Mandelstam-t range: -0.36 GeV to 1.44 GeV",
"Data compared with model predictions including shadowing-based and saturation-based approaches"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.11120v1
|
https://arxiv.org/abs/2510.11120v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b76682aa545956705eed3e0ca7d7b0f9f86248c268eb63b5dcd65c65eccd427d
|
Extracted from ArXiv paper 2510.11120v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.11120v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:38:18.381858Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103845682444
|
Approximately 75% of weakly collisional models exhibit lower variability than their ideal counterparts, with a systematic decrease in variability observed in all MAD EGRMHD simulations.
|
Approximately 75% of weakly collisional models exhibit lower variability than their ideal counterparts, with a systematic decrease in variability observed in all MAD EGRMHD simulations.
|
[
"MAD EGRMHD simulations",
"Comparison to observations: M. Wielgus et al. 2022 report M3 ∈ [0.024, 0.051]",
"Power spectral density (PSD) of lightcurves indicates similar slopes at timescales ≲2 hours"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.11365v1
|
https://arxiv.org/abs/2510.11365v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
a62a09166030f4f6c36d8e9cd9ce4b0b20cd3282df2ddd793c8f78a3b5eec01c
|
Extracted from ArXiv paper 2510.11365v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.11365v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:38:45.682444Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_103919531111
|
17 unique γ rays connecting 11 low-lying excited states in 70Ge were observed with CHICO2 and GRETINA detectors
|
17 unique γ rays connecting 11 low-lying excited states in 70Ge were observed with CHICO2 and GRETINA detectors
|
[
"CHICO2 detector, 208Pb target, scattered 70Ge ions",
"GRETINA array detected 1215 keV γ ray (excluded from analysis)",
"17 unique γ rays observed, including previously reported transitions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.11641v1
|
https://arxiv.org/abs/2510.11641v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f3fedda8f820a650431f1a015ef18231f6e2f63520cb100a9d12218685000060
|
Extracted from ArXiv paper 2510.11641v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.11641v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:39:19.531111Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104000354143
|
The mass of 101Sn was precisely measured using the Advanced Cryogenic Gas Stopper and LEBIT's 9.4 T Penning trap mass spectrometer, resulting in a value consistent with predictions.
|
The mass of 101Sn was precisely measured using the Advanced Cryogenic Gas Stopper and LEBIT's 9.4 T Penning trap mass spectrometer, resulting in a value consistent with predictions.
|
[
"FRIB Facility",
"124Xe primary beam accelerated to 228 MeV/u",
"LEBIT's 9.4 T Penning trap mass spectrometer"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.11815v1
|
https://arxiv.org/abs/2510.11815v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
57a912437aec7cda1eb5cf2c4d66765a0f3c8304e5b4bb2a036f58bd363a25ed
|
Extracted from ArXiv paper 2510.11815v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.11815v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:40:00.354143Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104013393494
|
We measured a Faraday filter spectrum with a maximum transmittance of approximately 82% at zero detuning for the 7Li D2 transition, with an equivalent noise bandwidth (ENBW) of 5.32 GHz and a figure of merit (FOM) of 0.154 GHz−1.
|
We measured a Faraday filter spectrum with a maximum transmittance of approximately 82% at zero detuning for the 7Li D2 transition, with an equivalent noise bandwidth (ENBW) of 5.32 GHz and a figure of merit (FOM) of 0.154 GHz−1.
|
[
"Faraday filter experiment",
"Magnetic field: 269 G",
"Temperature: 264 °C"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.11859v1
|
https://arxiv.org/abs/2510.11859v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
98dff4c3e88a985ac57c4bc3c394907915bf112736cf920656cac02156d6e661
|
Extracted from ArXiv paper 2510.11859v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.11859v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:40:13.393494Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104108061064
|
The populations of four atomic states in a Rydberg atom are measured as a function of RF Rabi frequency, exhibiting five distinct dynamical regions.
|
The populations of four atomic states in a Rydberg atom are measured as a function of RF Rabi frequency, exhibiting five distinct dynamical regions.
|
[
"Four-level Ladder system in 85RbD1 manifold",
"Steady-state (SS) condition with ΩRF ≪ Γr2",
"Population analysis via simulation and experiment"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.11918v1
|
https://arxiv.org/abs/2510.11918v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b8754746254bdb351f5cfd7a384996248bc5d9e83e4b105d4335c1d9c6777d2e
|
Extracted from ArXiv paper 2510.11918v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.11918v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:41:08.061064Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104209693510
|
The kink mode in a tokamak plasma is stabilized when decreasing the aspect ratio R0/a, and this trend is observed in MHD and gyrokinetic simulations.
|
The kink mode in a tokamak plasma is stabilized when decreasing the aspect ratio R0/a, and this trend is observed in MHD and gyrokinetic simulations.
|
[
"ORB5 facility data",
"MHD growth rates match well for all values of the aspect ratio",
"Full 3D magnetic perturbations needed to describe the kink mode accurately"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.12432v1
|
https://arxiv.org/abs/2510.12432v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
09a270261e4dc63c387a71cd250520d3b9e2217f78612d8254e0e9a772f6d3c3
|
Extracted from ArXiv paper 2510.12432v1 (chunk 15)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2510.12432v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:42:09.693510Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104234059972
|
Linear growth rate of instability due to Ion Cyclotron Scattering (ICS) measured and compared across different density regimes.
|
Linear growth rate of instability due to Ion Cyclotron Scattering (ICS) measured and compared across different density regimes.
|
[
"Plasma dispersion function, Eqs. (77), (82)",
"Maximum growth wavenumber for ICS given by Eq. (78) in collective limit",
"Validity condition for intermediate and high density regimes expressed as Eq. (86)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.12869v1
|
https://arxiv.org/abs/2510.12869v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e1b05e8c00868137b0107028acf1070cbdfbee5f70680af35b8a58d361dbfe66
|
Extracted from ArXiv paper 2510.12869v1 (chunk 12)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 12,
"paper_id": "2510.12869v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:42:34.059972Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104203296832
|
Super-K detector experiences a cosmic-ray muon rate of approximately 2 s−1 at its depth, producing spallation radioactivity backgrounds.
|
Super-K detector experiences a cosmic-ray muon rate of approximately 2 s−1 at its depth, producing spallation radioactivity backgrounds.
|
[
"Super-K water-based experiment with an inner detector mass of 32 kton",
"Approximately 2 s−1 cosmic-ray muon rate",
"Muons interact with oxygen nuclei in water to produce radioactive isotopes"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.12873v1
|
https://arxiv.org/abs/2510.12873v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
86322131cedcf253afe70c89f4fa827d3c31ff5aefb87ae96c2e36194c203915
|
Extracted from ArXiv paper 2510.12873v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.12873v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:42:03.297351Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104209024305
|
The JUNO neutrino detector aims to achieve an energy threshold of ∼2 MeV with world-leading capabilities for precision measurements of solar neutrinos and reactor neutrino oscillations.
|
The JUNO neutrino detector aims to achieve an energy threshold of ∼2 MeV with world-leading capabilities for precision measurements of solar neutrinos and reactor neutrino oscillations.
|
[
"liquid scintillator detector, 20 kton of linear alkylbenzene (LAB), shielded under ∼650 m of overburden",
"energy resolution: ∼3% at 1 MeV",
"purification techniques, energy-dependent fiducial volume cuts, and coincidence-based rejection"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.12873v1
|
https://arxiv.org/abs/2510.12873v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
52ee82997c7bcfae3fbf6c15d8496f0cd42bec62bd3a76a2e553f53372d5943f
|
Extracted from ArXiv paper 2510.12873v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.12873v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:42:09.024305Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104221169398
|
Self-trapping phenomenon observed in a SOC + ML BEC with ground state phase diagram exhibiting spin-polarization and left-right population imbalance.
|
Self-trapping phenomenon observed in a SOC + ML BEC with ground state phase diagram exhibiting spin-polarization and left-right population imbalance.
|
[
"Stem-Gerlach separation combined with time-of-flight imaging",
"Spin-polarization (Sz) calculated as (N↑−N↓)/(N↑+ N↓)",
"kL/kR ≈ 0.89"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.13056v1
|
https://arxiv.org/abs/2510.13056v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2aa94b4e2d216078f96770ad8fbc66ac7e4a39a8ce3d12f0d17b85d561011166
|
Extracted from ArXiv paper 2510.13056v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.13056v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:42:21.169398Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104238010959
|
A dynamical phase transition is observed in a spin chain system with long-range interactions, characterized by a logarithmic divergence of the oscillation period at criticality.
|
A dynamical phase transition is observed in a spin chain system with long-range interactions, characterized by a logarithmic divergence of the oscillation period at criticality.
|
[
"Macroscopic quantum self-trapping experiment",
"Effective potential W(sz) shows two relevant roots for ℏΩL < gnχ",
"Spin polarization averaged over time window shorter than 10 ms"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.13056v1
|
https://arxiv.org/abs/2510.13056v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
81ecfa22f6b50d9b417557845011b8cdd01d405394317f1150f848a76d0bd25e
|
Extracted from ArXiv paper 2510.13056v1 (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": "2510.13056v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:42:38.010959Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104348700064
|
The splitting isotope shift (SIS) between the isotopes 12C and 14C was measured with a total uncertainty of 2 kHz, consistent with theoretical predictions.
|
The splitting isotope shift (SIS) between the isotopes 12C and 14C was measured with a total uncertainty of 2 kHz, consistent with theoretical predictions.
|
[
"Bare ion experiment with 12C and 14C ions",
"Fine-structure transitions in the 1s2p 3PJ states",
"10-MHz close-up of Fig. 1 showing experimental and theoretical SIS"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.13779v1
|
https://arxiv.org/abs/2510.13779v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
da058f3a2dae2e4bd0649cbfeccca03ef4d4c97e9cc6cd9a7b8a99dc4d649488
|
Extracted from ArXiv paper 2510.13779v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.13779v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:43:48.700064Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104409954574
|
The splitting isotope shift (SIS) in helium-like carbon ions was measured with excellent agreement, surpassing previous measurements by orders of magnitude.
|
The splitting isotope shift (SIS) in helium-like carbon ions was measured with excellent agreement, surpassing previous measurements by orders of magnitude.
|
[
"12C4+, 13C4+, and 14C4+ isotopes",
"Fine-structure mixing effects included",
"Theory validated through hyperfine analysis"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.13779v1
|
https://arxiv.org/abs/2510.13779v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
90af8b3a88fdf797eab7ba6c4ca7021a3637fa724c3dcdb4105d608dafa47ce5
|
Extracted from ArXiv paper 2510.13779v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.13779v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:44:09.954574Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104519817756
|
Proton beam energy measured using the stacked foil method with a Bayesian approach, achieving an uncertainty of ±2.5 MeV for energies up to 20 MeV
|
Proton beam energy measured using the stacked foil method with a Bayesian approach, achieving an uncertainty of ±2.5 MeV for energies up to 20 MeV
|
[
"Stacked foil technique",
"Bayesian inference method",
"48V activity induced in titanium foils"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.14440v1
|
https://arxiv.org/abs/2510.14440v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
bdedda14395a7d11eadea18c1a9f74c3f2f1368157abe810a2bb4ca2e5bff5d3
|
Extracted from ArXiv paper 2510.14440v1 (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": "2510.14440v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:45:19.817756Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104532235693
|
The activity of the irradiated foils was measured using a gamma spectrometer, with a focus on constraining the proton beam energy E0.
|
The activity of the irradiated foils was measured using a gamma spectrometer, with a focus on constraining the proton beam energy E0.
|
[
"Mirion/Canberra N-type GR2019 HPGe detector",
"Multi-gamma source calibration",
"Foil activities evaluated at 1312 keV γ-emission for 48V and 1116 keV γ-emission for 65Zn"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.14440v1
|
https://arxiv.org/abs/2510.14440v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
440390be66af86ba8d4cafac588e0b739900b7deb04288fccd968f1bc0d63a46
|
Extracted from ArXiv paper 2510.14440v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.14440v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:45:32.235693Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104548581153
|
The proton beam energy can be measured using the stacked foil method with a reliability that does not depend on current-on-target measurement, and it can achieve equivalent relative error with sample sizes smaller than the complete datasets.
|
The proton beam energy can be measured using the stacked foil method with a reliability that does not depend on current-on-target measurement, and it can achieve equivalent relative error with sample sizes smaller than the complete datasets.
|
[
"Stacked foil method",
"Proton beam energies between 8 MeV and 19 MeV",
"10 Ti foils of 25 µm thickness"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.14440v1
|
https://arxiv.org/abs/2510.14440v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
821d03b6fbbf6c43d580ed751e16892c4a31167aeab0bc44e31a7e30cb3a8691
|
Extracted from ArXiv paper 2510.14440v1 (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": "2510.14440v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:45:48.581153Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104555335399
|
The p–Σ+ correlation function in high-multiplicity triggered pp collisions at √s = 13 TeV is measured, showing a significant deviation from the Coulomb-only function.
|
The p–Σ+ correlation function in high-multiplicity triggered pp collisions at √s = 13 TeV is measured, showing a significant deviation from the Coulomb-only function.
|
[
"ALICE Collaboration data sample",
"Mean transverse mass ⟨mT⟩ of (1.94 ± 0.03) GeV/c2",
"Effective source size of (0.98+0.03−0.02) fm"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.14448v1
|
https://arxiv.org/abs/2510.14448v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b55012c09da6b4f1122b3de0276b5b723c436aa5f5734e029073f6b9fb68f817
|
Extracted from ArXiv paper 2510.14448v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.14448v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:45:55.335399Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104603903921
|
p–Σ+ femtoscopic correlation function measured with a statistical uncertainty of 15% in the singlet channel and 20% in the triplet channel
|
p–Σ+ femtoscopic correlation function measured with a statistical uncertainty of 15% in the singlet channel and 20% in the triplet channel
|
[
"ALICE Collaboration data, √s = 13 TeV pp collisions",
"Singlet scattering length: -3.03 ± 0.82 fm",
"Triplet scattering length: 0.21 ± 0.12 fm"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.14448v1
|
https://arxiv.org/abs/2510.14448v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
24e06b3ce75cd850b8435e1ec6ad83ff5ba8c2bea32b8d490745345dd26619c4
|
Extracted from ArXiv paper 2510.14448v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.14448v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:46:03.903921Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104616533457
|
The p–Σ+ correlation function in pp collisions at √s = 13 TeV is measured by the ALICE Collaboration.
|
The p–Σ+ correlation function in pp collisions at √s = 13 TeV is measured by the ALICE Collaboration.
|
[
"ALICE detector, 2023 LHC run",
"pp collisions at √s = 13 TeV",
"10^6 events recorded"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.14448v1
|
https://arxiv.org/abs/2510.14448v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
19f2375559ac5a3772563b58f2d83a201553086c5d19b5ee69377d02514699f1
|
Extracted from ArXiv paper 2510.14448v1 (chunk 18)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 18,
"paper_id": "2510.14448v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:46:16.533457Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104631082571
|
A significant p–Σ+ correlation function is observed in pp collisions at √s = 13 TeV, indicating a non-trivial spin-orbit interaction.
|
A significant p–Σ+ correlation function is observed in pp collisions at √s = 13 TeV, indicating a non-trivial spin-orbit interaction.
|
[
"ALICE Collaboration",
"√s = 13 TeV collision energy",
"2.3 × 10^8 Pb-Pb interactions analyzed"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.14448v1
|
https://arxiv.org/abs/2510.14448v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6df3a96deff9720701b9ce2fcf13d961e9d0a26cee2eb24ada49e304eb7b1e83
|
Extracted from ArXiv paper 2510.14448v1 (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": "2510.14448v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:46:31.082571Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104640507210
|
A phase shift induced by rotation is observed in an atomic interferometer, with a dominant contribution from Coriolis acceleration.
|
A phase shift induced by rotation is observed in an atomic interferometer, with a dominant contribution from Coriolis acceleration.
|
[
"Atomic interferometer setup",
"Sensor mean angular velocity: up to 4 mrad/s",
"Coriolis acceleration term: 4Ω0 S^2σ^2_vy"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.14755v1
|
https://arxiv.org/abs/2510.14755v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2192f9bf8c2950f12acb3ccfa8fc07eaff5ed68f1601ad65c0325751eb7d17f1
|
Extracted from ArXiv paper 2510.14755v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.14755v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:46:40.507725Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104648166847
|
The normalized factorial cumulants of proton and deuteron multiplicity distributions are measured in heavy-ion collisions by HADES, extending trends observed by STAR toward lower energies for the ratios C2/C1 and C3/C1.
|
The normalized factorial cumulants of proton and deuteron multiplicity distributions are measured in heavy-ion collisions by HADES, extending trends observed by STAR toward lower energies for the ratios C2/C1 and C3/C1.
|
[
"HADES experiment at SIS18 synchrotron",
"Ag+Ag collisions at √sNN = 2.55 GeV",
"Efficiency correction and data-driven event-mixing procedure applied"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.15353v1
|
https://arxiv.org/abs/2510.15353v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b7ceb8157ecf1756ed92ab4f0f240758c8a226e72eb80e610add857612b7081b
|
Extracted from ArXiv paper 2510.15353v1 (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": "2510.15353v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:46:48.166847Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104654464035
|
Proton factorial cumulants were measured as a function of rapidity acceptance, showing convergence towards the small number Poisson limit with decreasing acceptance.
|
Proton factorial cumulants were measured as a function of rapidity acceptance, showing convergence towards the small number Poisson limit with decreasing acceptance.
|
[
"HADES detector, proton-kaon collision system",
"Rapidity acceptance range: (400 MeV/c < pt < 1600 MeV/c)",
"Correlations included using Metropolis algorithm"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.15353v1
|
https://arxiv.org/abs/2510.15353v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2c3654a4cd924ac4cf3103a37fe00614ae12a2de5d1840404058108a69571a92
|
Extracted from ArXiv paper 2510.15353v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.15353v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:46:54.464035Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104718990081
|
Attenuation length and light yield of three types of scintillation fibers measured under beta, gamma, and alpha irradiation conditions
|
Attenuation length and light yield of three types of scintillation fibers measured under beta, gamma, and alpha irradiation conditions
|
[
"241Am (1.0 𝜇Ci) α-source used for alpha irradiation",
"90Sr β-source used for beta irradiation",
"22Na γ-source used for gamma irradiation"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.15913v2
|
https://arxiv.org/abs/2510.15913v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f97482f135ed00027262b1d12b659b775be1ddf3c12bf3b18265a5d91885a8bc
|
Extracted from ArXiv paper 2510.15913v2 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.15913v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:47:18.990081Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104720983635
|
HDC-capsule's surface normal displacement measured using laser-ultrasonic microscopy, with detected signal proportional to surface acoustic waves
|
HDC-capsule's surface normal displacement measured using laser-ultrasonic microscopy, with detected signal proportional to surface acoustic waves
|
[
"Frequency domain laser ultrasound setup",
"532 nm continuous-wave laser for detection",
"Laser power: approximately half of the optical power impinges on the sample"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.15997v2
|
https://arxiv.org/abs/2510.15997v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
40e7d25c53773f103967c5874930cc40c777777557ca99e2b23fe81bff118c8e
|
Extracted from ArXiv paper 2510.15997v2 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.15997v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:47:20.983635Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104730942141
|
ZGV-resonance observed at 105 MHz in HDC-shell dispersion, caused by constructive interference of bulk waves
|
ZGV-resonance observed at 105 MHz in HDC-shell dispersion, caused by constructive interference of bulk waves
|
[
"FEM simulations and experimental data from FreDomLUS",
"Two-fold FFT analysis",
"ZGV1-point identified as first two ZGV-points"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.15997v2
|
https://arxiv.org/abs/2510.15997v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9de710e1d83d8f8583106678892a71a0d37a40617e29ebfc19a2c21fc241d0ba
|
Extracted from ArXiv paper 2510.15997v2 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.15997v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:47:30.942141Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104723844824
|
CEνNS search yields a best-fit ratio of observed rate to Standard Model prediction as ρ = 0.26±1534.74 with low significance, indicating high background rates at low energies
|
CEνNS search yields a best-fit ratio of observed rate to Standard Model prediction as ρ = 0.26±1534.74 with low significance, indicating high background rates at low energies
|
[
"Cryogenic sapphire detectors deployed at MINER near the TRIGA research reactor",
"Exposures of 158 g-days (reactor-on) and 381 g-days (reactor-off)",
"Baseline energy resolution of ∼40 eV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.15999v1
|
https://arxiv.org/abs/2510.15999v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6661cc01b88c40ccaef0816e106962753867c0d08d737b21d74d62b08cf2cf8b
|
Extracted from ArXiv paper 2510.15999v1 (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": "2510.15999v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:47:23.844824Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104746060724
|
The experimentally measured integrated CEνNS event rate is RS+B ≈341 ± 229 (stat)±23 (sys) kg−1day−1, with a significance of α = 0.007 ± 0.022 (stat) ± 0.001 (sys)
|
The experimentally measured integrated CEνNS event rate is RS+B ≈341 ± 229 (stat)±23 (sys) kg−1day−1, with a significance of α = 0.007 ± 0.022 (stat) ± 0.001 (sys)
|
[
"Experiment: data from reactor-on period",
"Event rate measurement: RS+B ≈341 ± 229 (stat)±23 (sys) kg−1day−1",
"Background removal: reactor correlated background removed"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.15999v1
|
https://arxiv.org/abs/2510.15999v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
0ad3da24019c8e0234ebaa0ae0ab59c02ec2f35dab33ccd9f3c49c7741fc8e74
|
Extracted from ArXiv paper 2510.15999v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.15999v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:47:46.060724Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104831715507
|
Tokamak plasma detachment asymmetry observed between inner and outer divertors, with earlier onset of outer divertor detachment due to neutral accumulation and local momentum losses.
|
Tokamak plasma detachment asymmetry observed between inner and outer divertors, with earlier onset of outer divertor detachment due to neutral accumulation and local momentum losses.
|
[
"KSTAR tokamak experiments",
"UEDGE simulations",
"DIII-D tokamak comparisons"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.16199v1
|
https://arxiv.org/abs/2510.16199v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
588091d8e551db1228a42a7e89e238939628aec2864a697d8501fcf8c4a5238a
|
Extracted from ArXiv paper 2510.16199v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.16199v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:48:31.715507Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104914826990
|
The ionization yield Qy of argon was measured directly for the first time between 2 and 10 keV, extending experimental coverage below 7 keV.
|
The ionization yield Qy of argon was measured directly for the first time between 2 and 10 keV, extending experimental coverage below 7 keV.
|
[
"ReD experiment using a dual-phase argon Time Projection Chamber (TPC)",
"Ionization measurements via neutrons from a 252Cf source",
"18 plastic scintillators detected scattered neutrons for recoil energy reconstruction"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.16404v2
|
https://arxiv.org/abs/2510.16404v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4c57a53d64459bedeb3d93dd91fcd4e1d6817614f23cf137a01f6134f8051c45
|
Extracted from ArXiv paper 2510.16404v2 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.16404v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:49:14.827512Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_104953770636
|
Ionization yield Qy for Nuclear Recoils (NRs) measured between 2 and 10 keV with uncertainties of 1.5% to 2.5%
|
Ionization yield Qy for Nuclear Recoils (NRs) measured between 2 and 10 keV with uncertainties of 1.5% to 2.5%
|
[
"DarkSide-50 data used as input for MC simulation",
"Statistical uncertainty on N fit e: approximately 0.7 electrons",
"Systematic uncertainty on ±Er: between 0.04 and 0.06 keV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.16404v2
|
https://arxiv.org/abs/2510.16404v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2e369c81142b4f9ad7e8becf87293069e024c993c2a229ac8c8b94b2a9e36d14
|
Extracted from ArXiv paper 2510.16404v2 (chunk 14)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 14,
"paper_id": "2510.16404v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:49:53.770636Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105003673581
|
Measurement of the energy threshold for nuclear reactions induced by cosmic ray interactions in a liquid scintillator detector
|
Measurement of the energy threshold for nuclear reactions induced by cosmic ray interactions in a liquid scintillator detector
|
[
"Borexino detector, 2018-2020 data sample",
"Threshold energy: 2.1 MeV",
"Event rate: 35.6 ± 4.7 Hz"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.16404v2
|
https://arxiv.org/abs/2510.16404v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c95d5c40eaa115d2615aac35a6dcf98863ec507427e562f3b42250e5d48e9bbb
|
Extracted from ArXiv paper 2510.16404v2 (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": "2510.16404v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:50:03.673581Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105009122932
|
The vibrational ground state of the b3Π0 potential for LiK molecules is observed with a transition frequency from X1Σ+, v = 0, J = 0 to b3Π0, v′ = 0, J′ = 1 at 314,230.5(5) GHz.
|
The vibrational ground state of the b3Π0 potential for LiK molecules is observed with a transition frequency from X1Σ+, v = 0, J = 0 to b3Π0, v′ = 0, J′ = 1 at 314,230.5(5) GHz.
|
[
"Ultra-cold 6Li40K molecules",
"Microwave spectroscopy and diode laser system",
"Population loss feature measurement"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.17166v2
|
https://arxiv.org/abs/2510.17166v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
29d66da605e332d70d452aabebb7ac0574bd632f13c3bdd2bf1e26b189cfc143
|
Extracted from ArXiv paper 2510.17166v2 (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": "2510.17166v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:50:09.122932Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105026781085
|
The half-width at half-maximum (HWHM) of the STIRAP two-photon line profile is measured to be 112(10) kHz.
|
The half-width at half-maximum (HWHM) of the STIRAP two-photon line profile is measured to be 112(10) kHz.
|
[
"Spectroscopy measurement for b3Π0 with Feshbach molecules",
"Frequency range: 314,173.5 GHz to 314,516.0 GHz",
"Laser intensity and transition strength estimated in Section IIIA"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.17166v2
|
https://arxiv.org/abs/2510.17166v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
20d5861d768aa3150c7d7fca52c7934e082d91dd858568afde367c774d5e88b0
|
Extracted from ArXiv paper 2510.17166v2 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.17166v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:50:26.781085Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105044036015
|
Two-qubit gate error rate measured to be as low as 8.4(7) × 10−5 for sequences of up to N = 200 Cliffor, increasing by ≈3 × 10−5 for longer sequences
|
Two-qubit gate error rate measured to be as low as 8.4(7) × 10−5 for sequences of up to N = 200 Cliffor, increasing by ≈3 × 10−5 for longer sequences
|
[
"SLERB experiment",
"100 randomizations of SLERB sequences of length N = 200",
"Spin-motion entanglement errors: εleak ≈8×10−5"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.17286v1
|
https://arxiv.org/abs/2510.17286v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
52deec5d22160eae96309f62df699b5002d16f2e719deb8b86662f416c0bd31b
|
Extracted from ArXiv paper 2510.17286v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.17286v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:50:44.036534Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105042579693
|
Excellent agreement found between calculated and measured Einstein A-values for Te iv forbidden transitions, with good precision on the order of 10^-2 s^-1.
|
Excellent agreement found between calculated and measured Einstein A-values for Te iv forbidden transitions, with good precision on the order of 10^-2 s^-1.
|
[
"grasp0 code, compared with flexible atomic code (fac) by Gu (2008)",
"good agreement seen in Fig. 1 for range of transitions",
"excellent agreement found for weakest lines (less than 10^-1 s^-1)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.17357v1
|
https://arxiv.org/abs/2510.17357v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
24b933fe6fd9b1e40e4cc15a71eac1f1ebcf1b7e85878125a969f62d4cde06b2
|
Extracted from ArXiv paper 2510.17357v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.17357v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:50:42.579693Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105105355920
|
Photoionization cross sections for transitions between tellurium ions are calculated using the R-matrix method, providing accurate opacities for astrophysical modeling.
|
Photoionization cross sections for transitions between tellurium ions are calculated using the R-matrix method, providing accurate opacities for astrophysical modeling.
|
[
"Theoretical calculations using the Te ii target model from Mulholland et al. (2024b)",
"22-state continuum basis size with R-matrix boundary at r=29.76 a.u.",
"629 Te ii energy levels retained in level expansion"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.17357v1
|
https://arxiv.org/abs/2510.17357v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
35518df149a495ad77a09dd5a84986ac339d6f6bb2d2a6a081b18239795df971
|
Extracted from ArXiv paper 2510.17357v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.17357v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:51:05.355920Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105212998634
|
Ion velocity distribution functions (IVDFs) measured near a grounded electrode show a non-monotonic trend in ion temperature and skewness, indicating deviations from Maxwellian distributions.
|
Ion velocity distribution functions (IVDFs) measured near a grounded electrode show a non-monotonic trend in ion temperature and skewness, indicating deviations from Maxwellian distributions.
|
[
"Langmuir probe measurements at p = 0.8 mTorr and PRF = 500 W",
"Debye length estimated as λD ≈40–80 µm",
"Ion-neutral collision cross section σ ∼10−18 m2"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.18384v1
|
https://arxiv.org/abs/2510.18384v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c09146ce9d10956b219b0edac16193eabda7104b95ca4b6226880b0cc3e3eb53
|
Extracted from ArXiv paper 2510.18384v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.18384v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:52:12.998634Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105212235504
|
High-precision atomic transition frequency of the 1S0→3P1 line in neutral Hg measured to be 253.7 nm with a relative uncertainty of 2%
|
High-precision atomic transition frequency of the 1S0→3P1 line in neutral Hg measured to be 253.7 nm with a relative uncertainty of 2%
|
[
"Magneto-optical trap (MOT) setup at 150 µK temperature",
"Frequency stabilized laser system with a finesse of 74,100(660)",
"Measurement campaign over several weeks"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.18514v2
|
https://arxiv.org/abs/2510.18514v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c19078a8d26ea723d1c7a0961e51194fa54eda13035aa54ca66556b65991d933
|
Extracted from ArXiv paper 2510.18514v2 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.18514v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:52:12.235504Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105215099801
|
RAA of inclusive charged hadrons measured to be approximately unity at high pT > 7 GeV/c in 0–10% collisions, with about 15% uncertainty
|
RAA of inclusive charged hadrons measured to be approximately unity at high pT > 7 GeV/c in 0–10% collisions, with about 15% uncertainty
|
[
"STAR detector, O+O collisions at √sNN = 200 GeV",
"pT range: 7-30 GeV/c",
"Centrality class: 0-10%"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.18616v2
|
https://arxiv.org/abs/2510.18616v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
430d0917d234949439734bc7d63aa69039ed54fe63ad3e1fd44c54156a673057
|
Extracted from ArXiv paper 2510.18616v2 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.18616v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:52:15.099801Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105239604123
|
The transverse momentum distribution of D0 mesons at mid-rapidity is measured with ALICE Collaboration at LHC √sNN = 5.02 TeV energy, showing agreement between coalescence and fragmentation production mechanisms.
|
The transverse momentum distribution of D0 mesons at mid-rapidity is measured with ALICE Collaboration at LHC √sNN = 5.02 TeV energy, showing agreement between coalescence and fragmentation production mechanisms.
|
[
"ALICE detector, Pb-Pb collisions at √sNN = 5.02 TeV",
"0-10% centrality, 362 million D0 meson pairs analyzed",
"Transverse momentum distribution of D0 mesons produced by coalescence and fragmentation"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.18673v1
|
https://arxiv.org/abs/2510.18673v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
86a65d6d9ac588f0d44dcd14ca92183fcb02800619085fa5b95ff8b2755ea8db
|
Extracted from ArXiv paper 2510.18673v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.18673v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:52:39.604123Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105248575265
|
Reconstructed particles from DELPHI detector match with generator-level MC simulations, validating the PYTHIA-to-DELSIM pipeline
|
Reconstructed particles from DELPHI detector match with generator-level MC simulations, validating the PYTHIA-to-DELSIM pipeline
|
[
"DELPHI detector data",
"PYTHIA 8.3 and Monash Tune used for simulation",
"Good agreement with DELPHI official PYTHIA 5 sample"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.18762v1
|
https://arxiv.org/abs/2510.18762v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
774f29411efaa9e62bb7b9018612c72cff3ced0f145eddf5e256500f9f229031
|
Extracted from ArXiv paper 2510.18762v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.18762v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:52:48.575265Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105307825437
|
The detector built by the DELPHI collaboration exhibits excellent resolution, with a small smearing effect despite some deterioration in the very small and very large θL regions.
|
The detector built by the DELPHI collaboration exhibits excellent resolution, with a small smearing effect despite some deterioration in the very small and very large θL regions.
|
[
"DELPHI detector",
"θL parametrization",
"2D response matrix"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.18762v1
|
https://arxiv.org/abs/2510.18762v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
d00e62c26b9947383af7718e6103271666553ecc4e67e73197d30b4bcf7f57bd
|
Extracted from ArXiv paper 2510.18762v1 (chunk 14)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 14,
"paper_id": "2510.18762v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:53:07.825437Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105359384183
|
The track-only thrust distribution, unfolded and corrected for detector effects, shows agreement to within 2% with a legacy measurement from the DELPHI collaboration.
|
The track-only thrust distribution, unfolded and corrected for detector effects, shows agreement to within 2% with a legacy measurement from the DELPHI collaboration.
|
[
"track-only thrust analysis using 1994 data",
"comparison with DELPHI measurement [15]",
"agreement within 2% in primary region of interest"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.18762v1
|
https://arxiv.org/abs/2510.18762v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
5e038f94a71fadb07773106266ffe83383ae5f77f0dd31948b433fcc59dc7214
|
Extracted from ArXiv paper 2510.18762v1 (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": "2510.18762v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:53:59.384183Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105306020029
|
Resistivity shows strong deviation from first-Born approximation and saturates at large U/t, with measured value a factor of seven lower than anticipated.
|
Resistivity shows strong deviation from first-Born approximation and saturates at large U/t, with measured value a factor of seven lower than anticipated.
|
[
"Full T-matrix calculations for current dissipation rate",
"Measured temperature and density at various interaction strengths U/t",
"Saturation observed in frequency-averaged Re ρ"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19395v1
|
https://arxiv.org/abs/2510.19395v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
dddf9e361117986668544d6e62998f2d7422cd3ad741c0142f31b8f8a65b4a74
|
Extracted from ArXiv paper 2510.19395v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.19395v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:53:06.020029Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105406646324
|
15 new half lives of isotopes near 54Ca were measured with a dramatic change in systematic behavior for neutron-rich nuclei beyond N=34
|
15 new half lives of isotopes near 54Ca were measured with a dramatic change in systematic behavior for neutron-rich nuclei beyond N=34
|
[
"FRIB Decay Station initiator (FDSi) at Facility for Rare Isotope Beams",
"New analysis method accounting for β-delayed neutron emission branches",
"State-of-the-art shell-model calculations with tensor interactions"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19757v1
|
https://arxiv.org/abs/2510.19757v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f0b0ecd0c155db7a997a3bb3d139381f488580482e091f040a414820302b575d
|
Extracted from ArXiv paper 2510.19757v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.19757v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:54:06.646324Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105409809262
|
Fifteen new half lives were measured for various isotopes through decay curve fits, including 48−51Cl, 51−53Ar, and 55K.
|
Fifteen new half lives were measured for various isotopes through decay curve fits, including 48−51Cl, 51−53Ar, and 55K.
|
[
"FRIB experiment in January 2024",
"ARIS beam settings centered on 54K",
"Particle identification using ∆E-TOF method"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19757v1
|
https://arxiv.org/abs/2510.19757v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
27867ce0278e8bc5afe14a72502dab807c797e4133023265cff3f9b7e7e07d24
|
Extracted from ArXiv paper 2510.19757v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.19757v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:54:09.809262Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105423980867
|
Fifteen new half-lives were measured for nuclei with Z ∼ 20 and N = 34, confirming the existence of a 'kink' at N = 35 along the calcium and scandium isotopic chains.
|
Fifteen new half-lives were measured for nuclei with Z ∼ 20 and N = 34, confirming the existence of a 'kink' at N = 35 along the calcium and scandium isotopic chains.
|
[
"FDSi experiment",
"15 new half-life measurements",
"Good agreement with LSSM calculations using sdpf-mu and ufp-ca interactions"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19757v1
|
https://arxiv.org/abs/2510.19757v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9d336b59c47d0c45653f9229e448482fade7546f397bf1d8305f60bed27e149f
|
Extracted from ArXiv paper 2510.19757v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.19757v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:54:23.980867Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105414801282
|
Dispersive shock waves were first observed in an intense electron beam using the University of Maryland Electron Ring, exhibiting characteristics consistent with Korteweg–de Vries predictions.
|
Dispersive shock waves were first observed in an intense electron beam using the University of Maryland Electron Ring, exhibiting characteristics consistent with Korteweg–de Vries predictions.
|
[
"University of Maryland Electron Ring (UMER)",
"Localized induction-cell perturbation produced a negative density pulse",
"Leading soliton-like peak followed by an expanding train of oscillations"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19786v1
|
https://arxiv.org/abs/2510.19786v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6840d98c060f10681f9fe14687e83e717eaebfa172473427217de56c860c939d
|
Extracted from ArXiv paper 2510.19786v1 (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": "2510.19786v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:54:14.801282Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105548803221
|
AEDGE detector is expected to detect a minimum of a few hundred mergers per year, while MAGIS Space forecasts a maximum of 3 WDB merger detections per year
|
AEDGE detector is expected to detect a minimum of a few hundred mergers per year, while MAGIS Space forecasts a maximum of 3 WDB merger detections per year
|
[
"Comparison between MAGIS Space and AEDGE detectors",
"Detector-dependent results for the model approach (Figure 12)",
"Sensitivity improvement in AEDGE leads to rates of detection roughly three orders of magnitude larger than for MAGIS Space"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19913v1
|
https://arxiv.org/abs/2510.19913v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
fd9d16b6cb3890fcc459f982857b815c57d6f23e789929a6b7b56f41b5af6f55
|
Extracted from ArXiv paper 2510.19913v1 (chunk 26)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 26,
"paper_id": "2510.19913v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:55:48.803746Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105547730738
|
A boron nitride coating on CR-39 plastic nuclear track detectors enhances neutron detection efficiency by converting neutrons into energetic alpha particles.
|
A boron nitride coating on CR-39 plastic nuclear track detectors enhances neutron detection efficiency by converting neutrons into energetic alpha particles.
|
[
"CR-39 detector, AmBe and 252Cf neutron source spectra",
"10B(n,α)7Li reaction with 2.31 MeV energy release",
"Up to 10x increase in neutron detection at 5 MeV neutron energies"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.20924v1
|
https://arxiv.org/abs/2510.20924v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4318a360a5c4047e8e0fee90d309c54347210ecde34ef6e56f8cd5bd20486411
|
Extracted from ArXiv paper 2510.20924v1 (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": "2510.20924v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:55:47.730738Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105609204836
|
CR-39 detectors with BN coating increased neutron detection efficiency by a factor of up to 10x for AmBe source and 4x for 252Cf source
|
CR-39 detectors with BN coating increased neutron detection efficiency by a factor of up to 10x for AmBe source and 4x for 252Cf source
|
[
"AmBe and 252Cf sources",
"Optical microscope: 10x enhancement for AmBe, 4x for 252Cf",
"SEM imaging: 2.2x enhancement for AmBe"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.20924v1
|
https://arxiv.org/abs/2510.20924v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
6bb14ffe2b8023e80be7f4f4be7dd12ce349428c38ac42bdf551b55d9d11fe49
|
Extracted from ArXiv paper 2510.20924v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.20924v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:56:09.205361Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105638703224
|
Blobs and voids, magnetic-field-aligned filaments of excess or reduced density, are observed at the boundary region of magnetic confinement plasma.
|
Blobs and voids, magnetic-field-aligned filaments of excess or reduced density, are observed at the boundary region of magnetic confinement plasma.
|
[
"Experimental studies in magnetic confinement fusion",
"Detection at the boundary region between the last closed flux surface (LCFS) and scrape-off layer (SOL)",
"Characterized by positive/negative skewness of density fluctuations"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21170v1
|
https://arxiv.org/abs/2510.21170v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
7d9400b773526ab0261249ee4e1a60164d54a5920022a556496bb462ce3a501f
|
Extracted from ArXiv paper 2510.21170v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.21170v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:56:38.703224Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105656971402
|
Multiple local minima in turbulence correlation length measured in Tore Supra L-mode plasmas, correlating with shear flow layers and rational q surfaces.
|
Multiple local minima in turbulence correlation length measured in Tore Supra L-mode plasmas, correlating with shear flow layers and rational q surfaces.
|
[
"Tore Supra L-mode plasmas",
"GYSELA data analysis",
"Flow shear extrema correlated with correlation length minima"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.21170v1
|
https://arxiv.org/abs/2510.21170v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
66dfd2f5c01a7ae723a2e0d560628abc303dae48832eed3b3834580f27ea5331
|
Extracted from ArXiv paper 2510.21170v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.21170v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:56:56.971402Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105653171922
|
The linear growth rate of the Drift-Kink instability is observed to be approximately 2.67 in mixed-shear simulations, consistent with but not entirely matching analytic predictions.
|
The linear growth rate of the Drift-Kink instability is observed to be approximately 2.67 in mixed-shear simulations, consistent with but not entirely matching analytic predictions.
|
[
"Simulation data from mixed-shear cases (uj < 0.6) at y/de,j = 200",
"Growth rates fitted using equation 25 in Zenitani & Hoshino (2007)",
"Comparison to analytical expectations for DKI and KH instabilities"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21187v1
|
https://arxiv.org/abs/2510.21187v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
504562307c1cee818eb3e2890a251ea86e80a83ae58338a8777777805055bda0
|
Extracted from ArXiv paper 2510.21187v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.21187v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:56:53.171922Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105733035998
|
Electron plasma frequency ωp,e is measured in the quasi-steady state plasma with sufficient cell resolution to resolve the electron plasma Debye length λD,e.
|
Electron plasma frequency ωp,e is measured in the quasi-steady state plasma with sufficient cell resolution to resolve the electron plasma Debye length λD,e.
|
[
"Penning discharge benchmark",
"Table 2.1 lists numerical and physical parameters",
"Grid size: Nx = Ny = 256, ∆x = ∆y = 1.953 × 10^−4 m"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21261v1
|
https://arxiv.org/abs/2510.21261v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
c4f829cd427c9ef1b1b38810ef9125ed67af4b5e83ddf26dd156fa8d8caad861
|
Extracted from ArXiv paper 2510.21261v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.21261v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:57:33.035998Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105741743698
|
The mean period of spoke rotation is measured as 23.1 µs with a corresponding frequency of 43.2 kHz in a single simulation.
|
The mean period of spoke rotation is measured as 23.1 µs with a corresponding frequency of 43.2 kHz in a single simulation.
|
[
"Single simulation data, 300 µs averaging time",
"13 rotations analyzed",
"Diagnostic used: Section 2.3"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21261v1
|
https://arxiv.org/abs/2510.21261v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2005fb3ab360f16f0d6f6c6f06b725ca4ab30ab662ef71ab30008e7f567a411f
|
Extracted from ArXiv paper 2510.21261v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.21261v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:57:41.743698Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105800586720
|
Antikaon absorption cross-section in nuclear medium measured as 11.5 ± 2.3 mb, with implications for kaonic atoms
|
Antikaon absorption cross-section in nuclear medium measured as 11.5 ± 2.3 mb, with implications for kaonic atoms
|
[
"J-PARC experiment data",
"Kaon-nucleus collision energy: 1.8 GeV/c",
"Absorption length: 120 fm"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.21519v1
|
https://arxiv.org/abs/2510.21519v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4eba6412bf8e833ff9855dbfd75f3c8023ae1edabc575bb0f0ceb483c103d47e
|
Extracted from ArXiv paper 2510.21519v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.21519v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:58:00.586720Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105947165780
|
The electrization field Eλ is proportional to the nuclear electric dipole moment dN_e, and its dependence on temperature T can be measured by subtracting datasets collected at different Isol values.
|
The electrization field Eλ is proportional to the nuclear electric dipole moment dN_e, and its dependence on temperature T can be measured by subtracting datasets collected at different Isol values.
|
[
"Tantalum data",
"Lead zero-field datasets",
"Systematic uncertainty: temperature and Isol-dependent"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21768v1
|
https://arxiv.org/abs/2510.21768v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
141bfdc923b321793cb6cd70a2daa10d94567bda85ab8e88c56049220d8ae506
|
Extracted from ArXiv paper 2510.21768v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.21768v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:59:47.165780Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110010248985
|
Self-inductance of the sample solenoid was measured to be 4.5 × 10^-6 H, with a persistence of 9 days.
|
Self-inductance of the sample solenoid was measured to be 4.5 × 10^-6 H, with a persistence of 9 days.
|
[
"REGEN dataset, SQUID voltage data points",
"Ta and Pb wire radii: 0.25 mm and 0.5 mm respectively",
"Numerically calculated inductances using solenoid dimensions"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21768v1
|
https://arxiv.org/abs/2510.21768v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
dd34bf27ebf54c22de407cc46e3b2fd453dcc7b142cd7c64cced814f5fa8a0aa
|
Extracted from ArXiv paper 2510.21768v1 (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": "2510.21768v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:00:10.248985Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_105945746510
|
Differential A(γ, J/ψp)X cross section measured with 23% normalization uncertainty, showing deviations from plane-wave calculations
|
Differential A(γ, J/ψp)X cross section measured with 23% normalization uncertainty, showing deviations from plane-wave calculations
|
[
"CLAS12 detector",
"Data taken at Jefferson Lab",
"Light-cone momentum fraction αmiss: 0.5"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.22076v1
|
https://arxiv.org/abs/2510.22076v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3722316082e211933cadbc40753568dc567f59859dd9f5655386d4dd31585d07
|
Extracted from ArXiv paper 2510.22076v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.22076v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T10:59:45.746510Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110002936834
|
The installation of a forward Transition Radiation Detector (TRD) is planned to improve e/π separation, reducing background uncertainties in J/ψ yields and normalization
|
The installation of a forward Transition Radiation Detector (TRD) is planned to improve e/π separation, reducing background uncertainties in J/ψ yields and normalization
|
[
"GlueX spectrometer",
"Expected factor of 10 improvement in forward pion rejection",
"Reduced statistical uncertainty inflation factor from background to ~1.25"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.22076v1
|
https://arxiv.org/abs/2510.22076v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
aed2a6dcc3b819230311f06cdf6b77bd93a0b09d82051ffeca34d74f8aea42b4
|
Extracted from ArXiv paper 2510.22076v1 (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": "2510.22076v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:00:02.936834Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110008858434
|
Projected precision on incoherent J/ψ photoproduction cross section σ(γ4He →J/ψpX) as a function of beam photon energy Eγ, with estimated statistical uncertainties ranging from 14% to 20%
|
Projected precision on incoherent J/ψ photoproduction cross section σ(γ4He →J/ψpX) as a function of beam photon energy Eγ, with estimated statistical uncertainties ranging from 14% to 20%
|
[
"Simulations described in Sec. 4.2",
"Expected yields: ∼25 subthreshold J/ψ photoproduction events and roughly 800 higher-energy events",
"Fractional statistical uncertainties calculated as 1/√N for each bin"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.22076v1
|
https://arxiv.org/abs/2510.22076v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2d368c205a3ca20cb0abbfe6202bc1f3b6283df49b74e2331187a63c241dfd60
|
Extracted from ArXiv paper 2510.22076v1 (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": "2510.22076v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:00:08.858434Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110142705274
|
Gravity gradient tensor off-diagonal elements measured with modest averaging times using a tilted single-axis atom interferometer gradiometer
|
Gravity gradient tensor off-diagonal elements measured with modest averaging times using a tilted single-axis atom interferometer gradiometer
|
[
"Bose-Einstein condensates, improved gyroscopes, and tip-tilt mirror characterization",
"Off-diagonal signals measurable with 10^−100 E sensitivity",
"LMT techniques increase keff by a factor of 100"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.22350v2
|
https://arxiv.org/abs/2510.22350v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
4313cf889dc8d908d0d64f0b645eb19e7fc409b9092262136352011d8b2eded2
|
Extracted from ArXiv paper 2510.22350v2 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.22350v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:01:42.705274Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110111519621
|
The E4 transition probability in 93Mo is explained by the neutron-proton interaction, contrasting with its particle-hole conjugate 99Cd where no E4 isomer is observed.
|
The E4 transition probability in 93Mo is explained by the neutron-proton interaction, contrasting with its particle-hole conjugate 99Cd where no E4 isomer is observed.
|
[
"Shell-model calculations for 93Mo within the ν1d5/2 ⊗π0g2 model space",
"Neutron-proton (νπ) interaction matrix elements: Vνπ(J = 2) = 0.135, Vνπ(J = 4) = 0.480, etc.",
"Single-particle reduced matrix elements for the E4 transition"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.22352v1
|
https://arxiv.org/abs/2510.22352v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f6cad7090bfe1e0708f6d6d6019eab523f74460a73b0928a31c57482e67fd1c6
|
Extracted from ArXiv paper 2510.22352v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.22352v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:01:11.519621Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110133300466
|
The Roper resonance, N(1440)1/2+, has a measured pole mass of 1366 ± 3 MeV with a width of 192 ± 4 MeV.
|
The Roper resonance, N(1440)1/2+, has a measured pole mass of 1366 ± 3 MeV with a width of 192 ± 4 MeV.
|
[
"Particle Data Group values",
"Pole mass: 1366 ± 3 MeV",
"Width: 192 ± 4 MeV"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.22425v1
|
https://arxiv.org/abs/2510.22425v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
daebc93badbf8f30b028d90ca744a612394df8091ecff1a21d0a2924e5c1a1ba
|
Extracted from ArXiv paper 2510.22425v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.22425v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:01:33.300466Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110227534579
|
New neutron capture measurements on 165Ho were performed at the Gamma ToF Absorption Facility with a 4π γ-ray detector array, achieving substantially improved resolution and statistical precision.
|
New neutron capture measurements on 165Ho were performed at the Gamma ToF Absorption Facility with a 4π γ-ray detector array, achieving substantially improved resolution and statistical precision.
|
[
"Gamma ToF Absorption Facility (GTAF), China Spallation Neutron Source (CSNS)",
"Back-streaming White Neutron beam line",
"40 BaF2 modules operating at CSNS"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.22965v1
|
https://arxiv.org/abs/2510.22965v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
3147a4df51c96fb388b17abd756c7694a35e4e6e40513f0094b0e77c468c2581
|
Extracted from ArXiv paper 2510.22965v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.22965v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:02:27.534579Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110251562252
|
The neutron strength function of 165Ho was measured to be 10^(-4)S0 = 2.01(1), indicating the interaction strength between neutrons and the nucleus in 165Ho.
|
The neutron strength function of 165Ho was measured to be 10^(-4)S0 = 2.01(1), indicating the interaction strength between neutrons and the nucleus in 165Ho.
|
[
"Experiment performed at CSNS Back-n facility",
"Neutron energy range: 1 eV to 1 keV",
"Data evaluated for consistency with ENDF/B-VIII.0 library"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.22965v1
|
https://arxiv.org/abs/2510.22965v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2802083753af538a33d92b62d9dae2891358a8285e2d64f80d57484dbf643701
|
Extracted from ArXiv paper 2510.22965v1 (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": "2510.22965v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:02:51.562252Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110231984234
|
The CsI(Tl) detector was built with 26 crystals in a compact, symmetric detection volume and achieved linearity over the 0.1–2 MeV range with an energy resolution of approximately 6%.
|
The CsI(Tl) detector was built with 26 crystals in a compact, symmetric detection volume and achieved linearity over the 0.1–2 MeV range with an energy resolution of approximately 6%.
|
[
"CsI(Tl) crystals from CLEO experiment [12], arranged in a 5 × 5 square matrix",
"Energy resolution: 6%",
"Detector threshold efficiency: 200 keV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23001v1
|
https://arxiv.org/abs/2510.23001v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b97229d292232e8032e7bced3bed22903eaf100d0a5005b945d0b6fbdd8addd0
|
Extracted from ArXiv paper 2510.23001v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.23001v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:02:31.984756Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110314075023
|
The muon lifetime was determined individually for different HPGe detectors and gamma lines emitted after OMC, with a time profile extraction and lifetime fit.
|
The muon lifetime was determined individually for different HPGe detectors and gamma lines emitted after OMC, with a time profile extraction and lifetime fit.
|
[
"ALPACA and MIDAS data sets",
"HPGe detector energy and time since the muon signal",
"Timing information extracted from HF HPGe detector waveforms and LF PMT waveforms"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23401v1
|
https://arxiv.org/abs/2510.23401v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
9d0ab9b711729d26b126749d7708aae56d54ab4970e16a794140a66f5ff3e5f6
|
Extracted from ArXiv paper 2510.23401v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.23401v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:03:14.075023Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110328519796
|
A Faraday rotation of α(s) can be measured with ~9% attenuation error due to multi-pathing in a Uniform BTOF, allowing for complex B||(s) profiles to be retrieved from the fiber.
|
A Faraday rotation of α(s) can be measured with ~9% attenuation error due to multi-pathing in a Uniform BTOF, allowing for complex B||(s) profiles to be retrieved from the fiber.
|
[
"Uniform BTOF design",
"Attenuation error: ~9%",
"Faraday rotation measurement"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23562v1
|
https://arxiv.org/abs/2510.23562v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
ee5a88956c813f0a1925c9acf929aabccfa542c970e1ed6900a32fcf3ab1a839
|
Extracted from ArXiv paper 2510.23562v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.23562v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:03:28.519796Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110339325011
|
The dynamic critical exponent z of coarsening dynamics in a coupled two-dimensional bilayer system is measured to be 1.73(9) via diffusion-like scaling.
|
The dynamic critical exponent z of coarsening dynamics in a coupled two-dimensional bilayer system is measured to be 1.73(9) via diffusion-like scaling.
|
[
"Classical-field simulations within the truncated Wigner approximation",
"Numerical results from quenched 2D Bose gas (z ≈1.74)",
"Bootstrap fitting of pooled, collapsed data"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23600v1
|
https://arxiv.org/abs/2510.23600v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
fff66c8cdfcd4bb9397d938d012ea201645e31004880529d6d99e64b5d10f464
|
Extracted from ArXiv paper 2510.23600v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.23600v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:03:39.325011Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110425594123
|
The cross-sections of pKL and nKL scattering into various final states are measured with an accuracy of about 10%.
|
The cross-sections of pKL and nKL scattering into various final states are measured with an accuracy of about 10%.
|
[
"Experimental data from Fig. 11, which shows the cross sections obtained by our method",
"Datasets used: total cross section from Ref. [116], charge exchange cross section from Ref. [118], and regeneration cross section from Ref. [119]",
"Fitting results for elastic scattering dominant at klab ≳1 GeV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23695v1
|
https://arxiv.org/abs/2510.23695v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
401814dc861c0239107529f65fc04802312603903b9bff271b4c7151c1510c72
|
Extracted from ArXiv paper 2510.23695v1 (chunk 16)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 16,
"paper_id": "2510.23695v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:04:25.594646Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110443635016
|
The upper bound on axion lifetime τa is within a few percent uncertainty, with some dependence on the hadronic cross section ratio.
|
The upper bound on axion lifetime τa is within a few percent uncertainty, with some dependence on the hadronic cross section ratio.
|
[
"BBN constraint from He-4 abundance",
"Hadronic decay channels (π±, kaons, baryons) with secondary hadrons",
"Upper bound in (ma, τa) space"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23695v1
|
https://arxiv.org/abs/2510.23695v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
e304a9278d77f705cc83756e6b792b1768b2a5e7fb74d1836c13c0288c333840
|
Extracted from ArXiv paper 2510.23695v1 (chunk 22)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 22,
"paper_id": "2510.23695v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:04:43.635016Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110500380133
|
Cross-sections for nπ+ →pγ and pγ →nπ+ are inferred using time reversal transformation with PWA cross sections
|
Cross-sections for nπ+ →pγ and pγ →nπ+ are inferred using time reversal transformation with PWA cross sections
|
[
"PWA [126-128]",
"SAID program data",
"Fitted threshold energy consistent with PWA cross sections"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.23695v1
|
https://arxiv.org/abs/2510.23695v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
2e9fd523ae8cf4ad40dae4c95dfc420cf7f38ff54190d44b96c5064fab5323da
|
Extracted from ArXiv paper 2510.23695v1 (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": "2510.23695v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:05:00.380133Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110412776869
|
Ionization rate γexp measured to be 1.23 × 10^(-6) s^(-1) with 10% error, varying Rydberg state and density
|
Ionization rate γexp measured to be 1.23 × 10^(-6) s^(-1) with 10% error, varying Rydberg state and density
|
[
"ion spectrometer, pulsed dye laser, and ToF spectra analysis",
"number of ions counted from VMI images: 2 to 100 on average",
"Rydberg atom density estimated with 10% error"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24045v1
|
https://arxiv.org/abs/2510.24045v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
f011bbaef4254ad7d30fa05235bebac272cdee52472448703a7af04f1a569f57
|
Extracted from ArXiv paper 2510.24045v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.24045v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:04:12.777388Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110518287217
|
Bunching features are observed in the trailing beam after betatron cooling, with radial bunches forming due to radiation losses.
|
Bunching features are observed in the trailing beam after betatron cooling, with radial bunches forming due to radiation losses.
|
[
"Simulation of down-ramp region shows several bunches as modulations of radial beam profile",
"Fig. 2(a.3) demonstrates radial bunches (z −ct ∈ [−15, −10] µm)",
"Preliminary PIC simulations show onset of ICL in wiggler regime"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24567v1
|
https://arxiv.org/abs/2510.24567v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
b6c86485271693c950da8cc2024eab47b9bd17f846b78d39cc095e3ed5bd2205
|
Extracted from ArXiv paper 2510.24567v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.24567v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:05:18.287217Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110525977159
|
Branching ratios for 214Pb beta decay measured with uncertainties as low as ±0.5% for GS and ±1.2% for ES295,352 channels
|
Branching ratios for 214Pb beta decay measured with uncertainties as low as ±0.5% for GS and ±1.2% for ES295,352 channels
|
[
"PandaX-4T TPC detector, 2023 data sample",
"Half a million 214Pb events collected from 222Rn injection campaign",
"Systematic uncertainty: 3.42% (SS) and 3.31% (MS)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24612v2
|
https://arxiv.org/abs/2510.24612v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
1bf41bcd6fab6f143b95048766da08c00d678b348ccb8035d40c3d91a69b7762
|
Extracted from ArXiv paper 2510.24612v2 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.24612v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:05:25.977159Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110539357873
|
The overall efficiency of the SS spectrum is measured to be 99.87% ± 0.03%, while the MS spectrum's efficiency is 99.86% ± 0.03%
|
The overall efficiency of the SS spectrum is measured to be 99.87% ± 0.03%, while the MS spectrum's efficiency is 99.86% ± 0.03%
|
[
"SS/MS discrimination algorithm using BambooMC simulation framework",
"Geant4-based energy depositions and S2 signal processing",
"99.87% (SS) and 99.86% (MS) efficiencies"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24612v2
|
https://arxiv.org/abs/2510.24612v2
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
20a09e9a137b206d115e48693100c298af92e699845a09cd0153a7027bbc4cb6
|
Extracted from ArXiv paper 2510.24612v2 (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": "2510.24612v2"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:05:39.358391Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251207_110530274750
|
Phoswich detector array PARIS achieves signal separation using the PSA method, resolving signals from LaBr3(Ce) and NaI(Tl) crystals with a time resolution of 820 ns.
|
Phoswich detector array PARIS achieves signal separation using the PSA method, resolving signals from LaBr3(Ce) and NaI(Tl) crystals with a time resolution of 820 ns.
|
[
"PARIS phoswich detector array",
"PSA method for signal separation",
"Time gate: 120 ns (short), 820 ns (long)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24766v1
|
https://arxiv.org/abs/2510.24766v1
|
[
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] |
316413d4d859935684fd64c38194dee35c4ce7005366350dbc1c2523f222d8ca
|
Extracted from ArXiv paper 2510.24766v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.24766v1"
}
|
science
|
WO-ARX-01
|
2025-12-07T11:05:30.275290Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
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