wisdom_id stringlengths 23 23 | core_insight stringlengths 66 319 | core_result stringlengths 66 319 | evidence listlengths 0 6 | posterior float64 0.85 1 | warmth stringclasses 2 values | tier stringclasses 1 value | domain stringclasses 1 value | source stringclasses 1 value | arxiv_id stringlengths 12 12 | url stringlengths 34 34 | categories listlengths 1 5 | event_fingerprint stringlengths 64 64 | context stringlengths 49 51 | motifs listlengths 2 2 | witnessed_by stringclasses 1 value | lineage dict | lens stringclasses 1 value | contract_version stringclasses 1 value | ts stringdate 2025-12-07 10:07:46 2025-12-09 21:16:14 | source_type stringclasses 1 value | _corpus_batch stringclasses 1 value | pack_id stringclasses 1 value |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
w_20251207_122641070958 | The branching fraction for the Λ→pµ−νµ decay measured as B(Λ→pµ−νµ) = (1.462 ± 0.016 ± 0.100 ± 0.011) × 10^−4 | The branching fraction for the Λ→pµ−νµ decay measured as B(Λ→pµ−νµ) = (1.462 ± 0.016 ± 0.100 ± 0.011) × 10^−4 | [
"LHCb experiment, pp collision data at 13 TeV",
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] | 0.85 | high | universal | physics | arxiv | 2511.15681v1 | https://arxiv.org/abs/2511.15681v1 | [
"hep-ex",
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] | 9c09df9bf00b857890dd24d9f6fb053ba0679750de57f51037467450c2d4a945 | Extracted from ArXiv paper 2511.15681v1 (chunk 0) | [
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} | science | WO-ARX-01 | 2025-12-07T12:26:41.071471Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122701777418 | The Mg II λ2798 Å emission line flux was measured with an uncertainty of 14% due to Fe II subtraction, signal-to-noise ratio, and flux calibration error. | The Mg II λ2798 Å emission line flux was measured with an uncertainty of 14% due to Fe II subtraction, signal-to-noise ratio, and flux calibration error. | [
"A&A proofs: manuscript no. aa55413-25",
"Signal-to-noise ratio quantified as standard deviation of observed spectrum within same wavelength range",
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] | 0.85 | medium | universal | physics | arxiv | 2511.15695v1 | https://arxiv.org/abs/2511.15695v1 | [
"hep-ex",
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] | d0400f4e152f06a774f97a5a4ee1c75feb6f22d8447bb37dedc9eec31a6cfd90 | Extracted from ArXiv paper 2511.15695v1 (chunk 5) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:27:01.777418Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122736065217 | Intrinsic strain amplitudes for bulge MSPs responsible for the GCE were predicted, with detectability by next-generation detectors like CE and ET. | Intrinsic strain amplitudes for bulge MSPs responsible for the GCE were predicted, with detectability by next-generation detectors like CE and ET. | [
"ATNF pulsar catalog",
"Pop I and Pop II MSP population models",
"Sensitivity curves for current and future ground-based GW detectors"
] | 0.85 | high | universal | physics | arxiv | 2511.15793v1 | https://arxiv.org/abs/2511.15793v1 | [
"hep-ex",
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] | ecbd6460dbd51dc7e45530f720e1ae53dadf3c08805a7bf4acdd8aa25e93957a | Extracted from ArXiv paper 2511.15793v1 (chunk 11) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:27:36.065217Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122805984127 | Cooler and hotter gas temperatures in the galaxy cluster A2029 measured as 4.81+0.62−0.42 keV and 8.97+2.77−0.65 keV, respectively | Cooler and hotter gas temperatures in the galaxy cluster A2029 measured as 4.81+0.62−0.42 keV and 8.97+2.77−0.65 keV, respectively | [
"Resolve spectral fitting from XRISM data",
"Two-temperature model with Galactic neutral column density applied",
"Best-fit temperatures consistent with previous studies"
] | 0.85 | high | universal | physics | arxiv | 2511.15809v1 | https://arxiv.org/abs/2511.15809v1 | [
"hep-ex",
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] | 9993e9fabc9ef9eef665103d36dcce70819d81478cab2a4c3900c9d1fbb66af7 | Extracted from ArXiv paper 2511.15809v1 (chunk 7) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:28:05.984127Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122812642862 | A2029 cluster's chemical abundance ratios are measured with high precision, but with varying degrees of reliability across different instruments. | A2029 cluster's chemical abundance ratios are measured with high precision, but with varying degrees of reliability across different instruments. | [
"Resolve detector, high spectral resolution and sensitivity",
"EPIC, Chandra, Xtend, RGS detectors used for various elements",
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] | 0.85 | medium | universal | physics | arxiv | 2511.15809v1 | https://arxiv.org/abs/2511.15809v1 | [
"hep-ex",
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] | dae8ae9aca38ec6a72b42227533806bd724566aa493579a3dd27d565833e76e3 | Extracted from ArXiv paper 2511.15809v1 (chunk 9) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:28:12.643381Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122828971776 | The observed spectrum displays characteristics consistent with a Narrow Line Seyfert 1 (NLS1) galaxy, including faint [O III] lines and strong Fe II emission. | The observed spectrum displays characteristics consistent with a Narrow Line Seyfert 1 (NLS1) galaxy, including faint [O III] lines and strong Fe II emission. | [
"UT1 spectrum data",
"FHWM(Hβ)=(1015±117) km s−1",
"[O III]/Hβ flux ratio ∼2.24"
] | 0.85 | medium | universal | physics | arxiv | 2511.15814v1 | https://arxiv.org/abs/2511.15814v1 | [
"hep-ex",
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] | f5923aebd668614845c5e18d3d7e0350899b6e4419af00ff498af3c337423c18 | Extracted from ArXiv paper 2511.15814v1 (chunk 10) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.15814v1"
} | science | WO-ARX-01 | 2025-12-07T12:28:28.971776Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122900098136 | Light elements are present at the surface of young neutron stars, evident from observed soft X-ray thermal spectra and inferred effective temperatures | Light elements are present at the surface of young neutron stars, evident from observed soft X-ray thermal spectra and inferred effective temperatures | [
"Soft X-ray thermal spectra of isolated cooling neutron stars",
"Absorption lines in the cases of 1E 1207.44-5209 (electron cyclotron line and its harmonic(s))",
"Spectral fit with different atmosphere models"
] | 0.85 | high | universal | physics | arxiv | 2511.15913v1 | https://arxiv.org/abs/2511.15913v1 | [
"hep-ex",
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"astro-ph.HE"
] | b6c8d03603ef16a62d9326185b90a8625f1327df6b0aaf4481e04f9e314ab537 | Extracted from ArXiv paper 2511.15913v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:29:00.098136Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122848085704 | Belle II detector measures B0 and B+ meson production rates in e+e− collisions at the SuperKEKB collider, with a focus on energy-dependent cross-section measurements | Belle II detector measures B0 and B+ meson production rates in e+e− collisions at the SuperKEKB collider, with a focus on energy-dependent cross-section measurements | [
"Belle II detector, 2019-2022 data sample",
"1000 exclusive hadronic final states analyzed",
"Signal candidates peak at zero in the ∆E distribution"
] | 0.85 | medium | universal | physics | arxiv | 2511.15926v1 | https://arxiv.org/abs/2511.15926v1 | [
"hep-ex",
"nucl-ex",
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] | 13010c9bf54fd4d0467d94cc0e9cf04b43ad046e61364a5436fcb32514e5c1fa | Extracted from ArXiv paper 2511.15926v1 (chunk 4) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:28:48.085704Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122900919080 | The energy dependence of the ratio of visible cross sections σv(e+e−→B0 ¯B0) / σv(e+e−→B+B−) measured in Belle and Belle II data, with a slight increase of Rv with energy | The energy dependence of the ratio of visible cross sections σv(e+e−→B0 ¯B0) / σv(e+e−→B+B−) measured in Belle and Belle II data, with a slight increase of Rv with energy | [
"Belle detector, 571 fb-1 data",
"Belle II detector, 365 fb-1 data",
"Energy bins: 10.574 to 10.582 GeV"
] | 0.85 | high | universal | physics | arxiv | 2511.15926v1 | https://arxiv.org/abs/2511.15926v1 | [
"hep-ex",
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] | 4963852b637804b1d56363d36bee352360a1bca870ca59307fcca9bb85dc8e57 | Extracted from ArXiv paper 2511.15926v1 (chunk 8) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:29:00.919080Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122911106709 | The B+ and B0 meson masses are measured as m(B+) = 5,274.35 MeV/c^2 ± 0.04 and m(B0) = 5,279.18 MeV/c^2 ± 0.05, with a statistical uncertainty of 0.24 MeV/c^2 | The B+ and B0 meson masses are measured as m(B+) = 5,274.35 MeV/c^2 ± 0.04 and m(B0) = 5,279.18 MeV/c^2 ± 0.05, with a statistical uncertainty of 0.24 MeV/c^2 | [
"Belle II detector, 2023 data sample",
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"24 fit parameters, including ∆EBaBar"
] | 0.85 | high | universal | physics | arxiv | 2511.15926v1 | https://arxiv.org/abs/2511.15926v1 | [
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] | 8bd913bf9a5e5927cfeb3062254c0691aa85e59748aafc0b0fe29228136b68c4 | Extracted from ArXiv paper 2511.15926v1 (chunk 11) | [
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} | science | WO-ARX-01 | 2025-12-07T12:29:11.107225Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122917135495 | The measured value of ∆m is (0.495 ± 0.024 ± 0.005) MeV/c2, differing significantly from the BaBar result | The measured value of ∆m is (0.495 ± 0.024 ± 0.005) MeV/c2, differing significantly from the BaBar result | [
"BaBar experiment",
"Combined fit with Belle and Belle II data on Rv(Ecm)",
"Exclusion of Rv data for precision analysis"
] | 0.85 | high | universal | physics | arxiv | 2511.15926v1 | https://arxiv.org/abs/2511.15926v1 | [
"hep-ex",
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] | 26ce61d2be9d283a2f3b79353a8a47053afab6216fcf37e8f381949a674f7471 | Extracted from ArXiv paper 2511.15926v1 (chunk 13) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:29:17.135495Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122921004232 | The dressed cross-section ratio R/(pB0/pB+)3 is measured to be consistent with the original second-order polynomial in a wide energy range, with systematic shifts due to variation of Rv and ∆m by ±1 σ. | The dressed cross-section ratio R/(pB0/pB+)3 is measured to be consistent with the original second-order polynomial in a wide energy range, with systematic shifts due to variation of Rv and ∆m by ±1 σ. | [
"Ecm bins of width 2.5 MeV",
"13 bins in the energy range 10.56-10.5925 GeV",
"Values of R/(pB0/pB+)3 with statistical and systematic uncertainties for different Ecm bins given in table 5"
] | 0.85 | medium | universal | physics | arxiv | 2511.15926v1 | https://arxiv.org/abs/2511.15926v1 | [
"hep-ex",
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] | 69e49948b05ca21483008cb1b28dc340ec40d9c6d7fbe2e3712f33bee9603ce9 | Extracted from ArXiv paper 2511.15926v1 (chunk 14) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:29:21.004232Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_122942928770 | The JUNO experiment measured sin^2θ12 = 0.3092 ± 0.0087, improving precision by a factor of 1.6 over previous combined results. | The JUNO experiment measured sin^2θ12 = 0.3092 ± 0.0087, improving precision by a factor of 1.6 over previous combined results. | [
"JUNO detector",
"362 million B-meson pairs analyzed",
"Systematic uncertainty: 0.008"
] | 0.85 | high | universal | physics | arxiv | 2511.15978v2 | https://arxiv.org/abs/2511.15978v2 | [
"hep-ex",
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"astro-ph.HE"
] | e4eed8ff5cfbe6874d6d7a80a5d09d4d3bd346b9e929232e031eda7e7f93460f | Extracted from ArXiv paper 2511.15978v2 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:29:42.928770Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123053920634 | Cyg X-1 is observed in a hard state, showing evidence of two Comptonization components with different optical depths. | Cyg X-1 is observed in a hard state, showing evidence of two Comptonization components with different optical depths. | [
"IXPE mission observations",
"Two observation periods: May 15-21 and June 18-20, 2022",
"Total net exposure time: 328 ks"
] | 0.85 | high | universal | physics | arxiv | 2511.16246v1 | https://arxiv.org/abs/2511.16246v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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"astro-ph.HE"
] | 357131ba222f3dbee70fc707809bebcfcd52cd4608a4632dfc955d8c8d919406 | Extracted from ArXiv paper 2511.16246v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.16246v1"
} | science | WO-ARX-01 | 2025-12-07T12:30:53.920634Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123135999439 | Observed polarization properties of Cyg X-1 data suggest a sandwiching slab corona geometry rather than a wedge-shaped corona with truncated disk | Observed polarization properties of Cyg X-1 data suggest a sandwiching slab corona geometry rather than a wedge-shaped corona with truncated disk | [
"IXPE, NuSTAR, and NICER observations in 2022",
"Inner disk temperature estimated to be about 0.15 keV",
"Optical depths of Comptonization components similar to those observed in 2005"
] | 0.85 | high | universal | physics | arxiv | 2511.16246v1 | https://arxiv.org/abs/2511.16246v1 | [
"hep-ex",
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"astro-ph.HE"
] | c859e01626f05b8090160bfc7814d63e53cdf7ad116ec1407f42f2310a8da88f | Extracted from ArXiv paper 2511.16246v1 (chunk 14) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:31:35.999439Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123148038141 | The 95% CL upper limits on the fully degenerate Higgsino production cross section are calculated to be 0.25 pb, with an observed exclusion reaching up to approximately 115 GeV. | The 95% CL upper limits on the fully degenerate Higgsino production cross section are calculated to be 0.25 pb, with an observed exclusion reaching up to approximately 115 GeV. | [
"CMS detector, 137 fb^-1 data sample collected at 13 TeV",
"NLO+NLL precision calculation of theoretical cross section",
"Observed exclusion contour shown with ±1 and ±2 standard deviation experimental uncertainties"
] | 0.85 | high | universal | physics | arxiv | 2511.16394v2 | https://arxiv.org/abs/2511.16394v2 | [
"hep-ex",
"nucl-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | 95ebf639bd6e88f5185976a225226329c1fc0c69f054664f458a3a4ae5eac19a | Extracted from ArXiv paper 2511.16394v2 (chunk 9) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:31:48.038141Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123238585692 | The measurement of the quark-antiquark pair production in association with two Z bosons using the CMS detector at LHC yields a cross-section value of 12.7 fb, with an uncertainty of ±0.3 fb. | The measurement of the quark-antiquark pair production in association with two Z bosons using the CMS detector at LHC yields a cross-section value of 12.7 fb, with an uncertainty of ±0.3 fb. | [
"CMS detector, 2022 LHC run",
"Integrated luminosity: 138.8 fb^-1",
"Z boson pT > 500 GeV"
] | 0.85 | high | universal | physics | arxiv | 2511.16394v2 | https://arxiv.org/abs/2511.16394v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 1bf1f142c5aaea7a0c55b7a3974d3805f0c122800cea4363c92dcdf2463d1a93 | Extracted from ArXiv paper 2511.16394v2 (chunk 28) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 28,
"paper_id": "2511.16394v2"
} | science | WO-ARX-01 | 2025-12-07T12:32:38.586211Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123147185500 | Young's Modulus and Yield Strength of different materials are measured using a tensile test setup with various fixations | Young's Modulus and Yield Strength of different materials are measured using a tensile test setup with various fixations | [
"Load cell, temperature sensors (PT100), National Instruments data acquisition module",
"UTS: 884 MPa for California Fine Wire, 1916.5 MPa for Dahmen material",
"YTS values for different materials and temperatures"
] | 0.85 | medium | universal | physics | arxiv | 2511.16408v1 | https://arxiv.org/abs/2511.16408v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c86915a5670fb82090c13ee1a9969e226e38773161af059bf5d3babad1106603 | Extracted from ArXiv paper 2511.16408v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 6,
"paper_id": "2511.16408v1"
} | science | WO-ARX-01 | 2025-12-07T12:31:47.185500Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123150891803 | Yield tensile strength (YTS) and ultimate tensile strength (UTS) of wire samples measured at various temperatures, with values ranging from 1000-1200 MPa for YTS and up to 1000 MPa for UTS | Yield tensile strength (YTS) and ultimate tensile strength (UTS) of wire samples measured at various temperatures, with values ranging from 1000-1200 MPa for YTS and up to 1000 MPa for UTS | [
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] | 0.85 | medium | universal | physics | arxiv | 2511.16408v1 | https://arxiv.org/abs/2511.16408v1 | [
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w_20251207_123218333097 | The area under the ROC curve (AUC) of the defect detection model is measured to be 0.98, indicating high efficiency in detecting defects. | The area under the ROC curve (AUC) of the defect detection model is measured to be 0.98, indicating high efficiency in detecting defects. | [
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} | science | WO-ARX-01 | 2025-12-07T12:32:18.333097Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123146520056 | Aql X-1 observed with multiple telescopes during the 2024 outburst, providing a comprehensive dataset for studying its properties. | Aql X-1 observed with multiple telescopes during the 2024 outburst, providing a comprehensive dataset for studying its properties. | [
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] | 0.85 | medium | universal | physics | arxiv | 2511.16437v1 | https://arxiv.org/abs/2511.16437v1 | [
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} | science | WO-ARX-01 | 2025-12-07T12:31:46.520056Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123211478892 | X-ray to optical delay in Aql X-1 outburst measured at ≲3 days, consistent with previous observations. | X-ray to optical delay in Aql X-1 outburst measured at ≲3 days, consistent with previous observations. | [
"Belle II detector, 2023 data sample",
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] | 0.85 | medium | universal | physics | arxiv | 2511.16437v1 | https://arxiv.org/abs/2511.16437v1 | [
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] | 31e6d8a8bd7d43d8c6c4af9a56815dc8cbb2ef780d6bc0c7ae005d6f9608d333 | Extracted from ArXiv paper 2511.16437v1 (chunk 13) | [
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} | science | WO-ARX-01 | 2025-12-07T12:32:11.478892Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123148646339 | Residual metallicity from early enrichment population (EEP) needed to reproduce observed galaxy group and cluster metallicity | Residual metallicity from early enrichment population (EEP) needed to reproduce observed galaxy group and cluster metallicity | [
"XMM-Newton data for 26 galaxy groups and clusters",
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] | 0.85 | medium | universal | physics | arxiv | 2511.16448v1 | https://arxiv.org/abs/2511.16448v1 | [
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} | science | WO-ARX-01 | 2025-12-07T12:31:48.646339Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123210414421 | New enrichment model accounting for early, undetectable star populations explains observed metal trends in galaxy clusters. | New enrichment model accounting for early, undetectable star populations explains observed metal trends in galaxy clusters. | [
"Bayesian analysis of 26 galaxy groups and clusters",
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] | 0.85 | high | universal | physics | arxiv | 2511.16448v1 | https://arxiv.org/abs/2511.16448v1 | [
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] | 3369b5c6bc3511d8a6061fe7ef07c7a84ae1d597dc99845309215eef4ece0bbe | Extracted from ArXiv paper 2511.16448v1 (chunk 8) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T12:32:10.414421Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123251796782 | The SABRE South detector is capable of 5σ discovery (3σ exclusion) power to a DAMA-like signal with 2 years of data, given a total experimental background of 0.72 cpd/kg/keVee and a 50 kg target mass | The SABRE South detector is capable of 5σ discovery (3σ exclusion) power to a DAMA-like signal with 2 years of data, given a total experimental background of 0.72 cpd/kg/keVee and a 50 kg target mass | [
"SABRE South Experiment",
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] | 0.85 | high | universal | physics | arxiv | 2511.16451v1 | https://arxiv.org/abs/2511.16451v1 | [
"hep-ex",
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] | 78b2e9b7e549426dfeaf9d558f97a8b4dbfeea085a04948c8e66103e0626e4d8 | Extracted from ArXiv paper 2511.16451v1 (chunk 4) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:32:51.797300Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123319255991 | Simulations show that thermal evolution curves for observed pulsars require some heating mechanism to explain high temperatures, with neutrino emission and rotochemical heating being primary cooling mechanisms. | Simulations show that thermal evolution curves for observed pulsars require some heating mechanism to explain high temperatures, with neutrino emission and rotochemical heating being primary cooling mechanisms. | [
"Pulsar simulations",
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] | 0.85 | high | universal | physics | arxiv | 2511.16507v1 | https://arxiv.org/abs/2511.16507v1 | [
"hep-ex",
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] | 63740b7721971610e815db06962058d820fa5b8fb84fc62942e3eab909ecafa0 | Extracted from ArXiv paper 2511.16507v1 (chunk 11) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T12:33:19.255991Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123254746427 | Normalised differential decay rate of B+ →J/ψK+ measured as a function of lepton helicity angle using the LHCb Upgrade I experiment | Normalised differential decay rate of B+ →J/ψK+ measured as a function of lepton helicity angle using the LHCb Upgrade I experiment | [
"LHCb Upgrade I detector",
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"hep-ex",
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] | 8cbf045ebc54b0071c47e66346e30efd3d82c74c05f1e3c66634c47668b14492 | Extracted from ArXiv paper 2511.16564v1 (chunk 0) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T12:32:54.746427Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123258341631 | First analysis of b-hadron decay using LHCb Upgrade I detector data presented, measuring angular observables AFB and FH in B+ →J/ψK+ decay. | First analysis of b-hadron decay using LHCb Upgrade I detector data presented, measuring angular observables AFB and FH in B+ →J/ψK+ decay. | [
"LHCb Upgrade I detector",
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"hep-ex",
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} | science | WO-ARX-01 | 2025-12-07T12:32:58.341631Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123320967868 | Measured values of AFB and FH agree with their predictions at the level of 1.2 standard deviations for MagDown data, and at the level of 1.5σ for MagUp data | Measured values of AFB and FH agree with their predictions at the level of 1.2 standard deviations for MagDown data, and at the level of 1.5σ for MagUp data | [
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w_20251207_123327363755 | No significant deviations observed in angular observables AFB and FH from expected values, with statistical and systematic uncertainties contributing roughly equally to the total uncertainty. | No significant deviations observed in angular observables AFB and FH from expected values, with statistical and systematic uncertainties contributing roughly equally to the total uncertainty. | [
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w_20251207_123330388233 | No significant deviation from zero observed in differential measurements of AFB and FH across 17 detector-response and kinematic variables | No significant deviation from zero observed in differential measurements of AFB and FH across 17 detector-response and kinematic variables | [
"LHCb detector, 0.7 fb−1 data sample",
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] | 0.85 | medium | universal | physics | arxiv | 2511.16564v1 | https://arxiv.org/abs/2511.16564v1 | [
"hep-ex",
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} | science | WO-ARX-01 | 2025-12-07T12:33:30.388233Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123333726532 | The upgraded LHCb detector shows excellent performance across varying levels of pile-up conditions, with stable results extracted for the angular distribution in B+ →J/ψK+ decays. | The upgraded LHCb detector shows excellent performance across varying levels of pile-up conditions, with stable results extracted for the angular distribution in B+ →J/ψK+ decays. | [
"LHCb Upgrade I detector, 1.1 fb−1 data collected in October 2024",
"Instantaneous luminosity: 2 × 10^33 cm−2 s−1",
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] | 0.85 | high | universal | physics | arxiv | 2511.16564v1 | https://arxiv.org/abs/2511.16564v1 | [
"hep-ex",
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] | 58a50adaf749acaa68c6e3d028c25af098c964f7027c3f9db672cdf0c2025c70 | Extracted from ArXiv paper 2511.16564v1 (chunk 12) | [
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} | science | WO-ARX-01 | 2025-12-07T12:33:33.726532Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123413220994 | The required detector runtime for a neutrino discovery from binary neutron star mergers is estimated to be around 50 years, but future improvements on the neutrino mass limits may lead to a shorter required detector runtime of 20-30 years. | The required detector runtime for a neutrino discovery from binary neutron star mergers is estimated to be around 50 years, but future improvements on the neutrino mass limits may lead to a shorter required detector runtime of 20-30 years. | [
"5 Mt detector",
"20-year exposure",
"mν = 0 eV case with full background and 0.6 s emission time"
] | 0.85 | high | universal | physics | arxiv | 2511.16658v1 | https://arxiv.org/abs/2511.16658v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | faf944c078faab520bff597dcfbd6567c96b39a51f667cc03001b45c98328580 | Extracted from ArXiv paper 2511.16658v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 10,
"paper_id": "2511.16658v1"
} | science | WO-ARX-01 | 2025-12-07T12:34:13.220994Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123347558518 | Neutron beta decay electron-neutrino correlation measured with goal sensitivity of ∆λ/|λ| = 0.04% by the Nab experiment | Neutron beta decay electron-neutrino correlation measured with goal sensitivity of ∆λ/|λ| = 0.04% by the Nab experiment | [
"Nab asymmetric magnetic spectrometer",
"Commissioning data collected in 2023",
"Tight kinematic constraints enabled new experimental limits on an excited state of the neutron"
] | 0.85 | high | universal | physics | arxiv | 2511.16678v1 | https://arxiv.org/abs/2511.16678v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d1f495cb68df04c51c0049a2bfcefb386f21493d79d4b12f2174e701db4b0506 | Extracted from ArXiv paper 2511.16678v1 (chunk 1) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:33:47.558518Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123404058614 | Researchers design a high-resolution particle detector using scintillating fibers and SPAD sensors, achieving few hundred picosecond time resolution. | Researchers design a high-resolution particle detector using scintillating fibers and SPAD sensors, achieving few hundred picosecond time resolution. | [
"SPAD sensor with large-format array of 110-nm CIS technology",
"Time resolution: hundreds of picoseconds",
"Optimized for noise rejection by signal coincidence"
] | 0.85 | medium | universal | physics | arxiv | 2511.16684v1 | https://arxiv.org/abs/2511.16684v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c64f8fda2050aaa42679c89142513c1ab4ed379611430f57e4bcf392974b0ef2 | Extracted from ArXiv paper 2511.16684v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.16684v1"
} | science | WO-ARX-01 | 2025-12-07T12:34:04.058614Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123644067461 | Folding Iteration with Compton Subtraction (FICS) reintroduces noise in the unfolded spectrum, preserving high-frequency fluctuations present in the observed data. | Folding Iteration with Compton Subtraction (FICS) reintroduces noise in the unfolded spectrum, preserving high-frequency fluctuations present in the observed data. | [
"Observed spectrum y",
"Noise model as in Sec. II D",
"Unfolding equation: ˆusol = Rˆu(k) + δ"
] | 0.85 | medium | universal | physics | arxiv | 2511.16687v1 | https://arxiv.org/abs/2511.16687v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 1994da40b063bcf153ffa552b01b93de315d3be4166e59fddc144c209831b6e5 | Extracted from ArXiv paper 2511.16687v1 (chunk 49) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 49,
"paper_id": "2511.16687v1"
} | science | WO-ARX-01 | 2025-12-07T12:36:44.067461Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123431014274 | Neutron detection efficiency for the miniBELEN detector was optimized using a novel composition method, reducing computation time and increasing design efficiency | Neutron detection efficiency for the miniBELEN detector was optimized using a novel composition method, reducing computation time and increasing design efficiency | [
"Particle Counter Monte Carlo simulations",
"Geant4 toolkit version 10.01 (patch 3)",
"Set of discrete neutron energies from 0.0001 to 10 MeV"
] | 0.85 | medium | universal | physics | arxiv | 2511.16692v1 | https://arxiv.org/abs/2511.16692v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | a2a3c75a141afd0c06859aec75c936f8d002e1ee9384189ac637797f09570a30 | Extracted from ArXiv paper 2511.16692v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.16692v1"
} | science | WO-ARX-01 | 2025-12-07T12:34:31.014274Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123542397234 | The resummed-expanded differential cross sections for DY and gluon fusion Higgs production show good agreement with fixed-order results at NNLO, with minor deviations in the convergence rate due to power corrections. | The resummed-expanded differential cross sections for DY and gluon fusion Higgs production show good agreement with fixed-order results at NNLO, with minor deviations in the convergence rate due to power corrections. | [
"Event2 [116] (fixed-order reference), disorder [116–118], Matrix [119] (fixed-order reference)",
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"Statistical uncertainty bands shown in Fig. 4"
] | 0.85 | medium | universal | physics | arxiv | 2511.16723v1 | https://arxiv.org/abs/2511.16723v1 | [
"hep-ex",
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] | 2b32658b7dd0ce221537dafa0193cf8ef8e53fd7510ffcfb7ecfc80ca0f2d98e | Extracted from ArXiv paper 2511.16723v1 (chunk 16) | [
"experimental_physics",
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"paper_id": "2511.16723v1"
} | science | WO-ARX-01 | 2025-12-07T12:35:42.397234Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123510864765 | Characteristic frequency ν∗ for pulsars measured to be around 558 MHz, indicating a similar feature in spectral turnovers as thermal free-free absorption. | Characteristic frequency ν∗ for pulsars measured to be around 558 MHz, indicating a similar feature in spectral turnovers as thermal free-free absorption. | [
"Compiled radio flux density measurements from K17, J18, K21, and S22 subsamples",
"Fitting parameters already published by the authors of each subsample",
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] | 0.85 | high | universal | physics | arxiv | 2511.16728v1 | https://arxiv.org/abs/2511.16728v1 | [
"hep-ex",
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] | 19158d3ae58d8b2002d8610b9d64d74770377858c6c4e8cfc8d17fa9ef49d877 | Extracted from ArXiv paper 2511.16728v1 (chunk 3) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T12:35:10.864765Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123805275969 | The cross section for virtual photoproduction d𝜎𝛾∗/dΩCM 𝜂′ is measured and expanded depending on the polarization of the virtual photons and the azimuthal angle 𝜙𝜂′ | The cross section for virtual photoproduction d𝜎𝛾∗/dΩCM 𝜂′ is measured and expanded depending on the polarization of the virtual photons and the azimuthal angle 𝜙𝜂′ | [
"JLab E12-17-003 experiment",
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"2.9 × 10^19 electrons irradiated"
] | 0.85 | medium | universal | physics | arxiv | 2511.17030v1 | https://arxiv.org/abs/2511.17030v1 | [
"hep-ex",
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] | b4e2d41e97cc051c14fa857495b9c507a2e8447c917502e7bd9d39eb5ba2ce2c | Extracted from ArXiv paper 2511.17030v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:38:05.275969Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123820850898 | Differential cross section for 1H (γ∗, p) η' reaction measured as 4.4 ± 0.8 (stat.) ± 0.4 (sys.) [nb/sr]. | Differential cross section for 1H (γ∗, p) η' reaction measured as 4.4 ± 0.8 (stat.) ± 0.4 (sys.) [nb/sr]. | [
"HRS detector data",
"Missing mass spectrum analysis",
"Statistical uncertainty: 18%"
] | 0.85 | medium | universal | physics | arxiv | 2511.17030v1 | https://arxiv.org/abs/2511.17030v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 561bcd2a31832f9a3c6d2bbc51d5698042b6c8ee8bfd371fc589ce95df40aa76 | Extracted from ArXiv paper 2511.17030v1 (chunk 9) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:38:20.850898Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123840267117 | The differential cross section of the γ* + p → η' + p reaction at W = 2130 MeV is measured to be 4.4 ± 0.8 (stat.) ± 0.4 (sys.) [nb/sr], indicating a significant role played by one or more resonances near W ∼ 2100 MeV. | The differential cross section of the γ* + p → η' + p reaction at W = 2130 MeV is measured to be 4.4 ± 0.8 (stat.) ± 0.4 (sys.) [nb/sr], indicating a significant role played by one or more resonances near W ∼ 2100 MeV. | [
"1H target, Λ hypernuclear spectroscopy experiment at Jefferson Lab",
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"Cos θCM γη' ≈ -1.0 in the One-Photon-Exchange Approximation"
] | 0.85 | high | universal | physics | arxiv | 2511.17030v1 | https://arxiv.org/abs/2511.17030v1 | [
"hep-ex",
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] | 89398eab1e91827277c03dab72a0d6de52e3d52d2ab01d12750bfba3beeabc7c | Extracted from ArXiv paper 2511.17030v1 (chunk 15) | [
"experimental_physics",
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} | science | WO-ARX-01 | 2025-12-07T12:38:40.267117Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123935522938 | The differential cross section for secondary electron ejection is described by a formula with a constant and an energy-dependent term, matching the Rutherford form at high energies but leveling out at low energies. | The differential cross section for secondary electron ejection is described by a formula with a constant and an energy-dependent term, matching the Rutherford form at high energies but leveling out at low energies. | [
"Opal et al. experiment (1971)",
"Secondary electrons up to 200 eV, primaries up to 2 keV",
"Differential cross section formula: σ(E, ϵ) = const(E) × 1/(1 + ϵ/¯E)^2"
] | 0.85 | medium | universal | physics | arxiv | 2511.17084v1 | https://arxiv.org/abs/2511.17084v1 | [
"hep-ex",
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] | f6694d96825dd1ab0388683be106f8982690ee28164e924789fccad422d17a6d | Extracted from ArXiv paper 2511.17084v1 (chunk 31) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.17084v1"
} | science | WO-ARX-01 | 2025-12-07T12:39:35.522938Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123900640180 | AI-Based Support Assistant for the ALICE-FIT detector setup at CERN enhances operational efficiency and safety with context-aware diagnostics and proactive decision support | AI-Based Support Assistant for the ALICE-FIT detector setup at CERN enhances operational efficiency and safety with context-aware diagnostics and proactive decision support | [
"WinCC OA alert panel",
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"Mean Time to Diagnose (MTTD): time measured in minutes"
] | 0.85 | medium | universal | physics | arxiv | 2511.17154v1 | https://arxiv.org/abs/2511.17154v1 | [
"hep-ex",
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] | 1d99c0d1ed22089ae6dd288cc32c68eea21eb7515ec20da6be1a6e16e3ace5f2 | Extracted from ArXiv paper 2511.17154v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:39:00.640180Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_123908649043 | Early-time decay rates of excited state population in subradiant regime measured with good quantitative agreement for Ω/Γ > 1 | Early-time decay rates of excited state population in subradiant regime measured with good quantitative agreement for Ω/Γ > 1 | [
"Imaging technique using absorption images",
"Driving frequency: Ω/Γ ≫1, scattered intensity",
"Experimental setup: gaussian intensity distribution"
] | 0.85 | medium | universal | physics | arxiv | 2511.17187v1 | https://arxiv.org/abs/2511.17187v1 | [
"hep-ex",
"nucl-ex",
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] | 6de477bdd15b3032c63caf7dfb69fc4fbf694a54c0735798d6a03ea9618487d4 | Extracted from ArXiv paper 2511.17187v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.17187v1"
} | science | WO-ARX-01 | 2025-12-07T12:39:08.649043Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124029591450 | No significant excess of events beyond SM expectation is observed, with upper limits determined for three new physics processes | No significant excess of events beyond SM expectation is observed, with upper limits determined for three new physics processes | [
"2017 and 2018 CMS data sets",
"Combined analysis with 2016 data set",
"95% confidence level (CL) upper limits obtained using asymptotic CLs criterion"
] | 0.85 | medium | universal | physics | arxiv | 2511.17310v1 | https://arxiv.org/abs/2511.17310v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | 6b250637491edf4f93f9717aed1a51887dcc603908fdda24cf425d8b03cb140f | Extracted from ArXiv paper 2511.17310v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 11,
"paper_id": "2511.17310v1"
} | science | WO-ARX-01 | 2025-12-07T12:40:29.591450Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124051438975 | Black hole spin measured to be a = 0.99 ± 0.01 with inclination θ = 68◦± 5◦, using NuSTAR data and accounting for narrow Fe Kα emission line | Black hole spin measured to be a = 0.99 ± 0.01 with inclination θ = 68◦± 5◦, using NuSTAR data and accounting for narrow Fe Kα emission line | [
"NuSTAR FPMA&FPMB spectra, simultaneous observation",
"Bh spin: 0.99 ± 0.01",
"Inclination: 68◦± 5◦"
] | 0.85 | high | universal | physics | arxiv | 2511.17338v1 | https://arxiv.org/abs/2511.17338v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 898999d31de32006df0135624a2b6cf33765daff7e9a49e6faee182dd26835b3 | Extracted from ArXiv paper 2511.17338v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 10,
"paper_id": "2511.17338v1"
} | science | WO-ARX-01 | 2025-12-07T12:40:51.438975Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124039381032 | MicroBooNE experiment measures νe CC cross sections on argon as a function of electron energy, total visible energy, and opening angle between the electron and leading proton. | MicroBooNE experiment measures νe CC cross sections on argon as a function of electron energy, total visible energy, and opening angle between the electron and leading proton. | [
"MicroBooNE detector, NuMI data sample",
"Flux-integrated differential cross sections extracted using higher-statistics data",
"Signal definition includes one electron with >20 MeV kinetic energy, at least one proton with >40 MeV kinetic energy, zero charged pions with >40 MeV kinetic energy"
] | 0.85 | high | universal | physics | arxiv | 2511.17342v1 | https://arxiv.org/abs/2511.17342v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 4c3f09c3d2a4f2528f500ef3a6bf440e25cb7ed8b27c95ecf19099f5c88823a5 | Extracted from ArXiv paper 2511.17342v1 (chunk 2) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:40:39.381032Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124049413221 | Neutrino event simulation and reconstruction performed in MicroBooNE using GENIE Monte Carlo with custom algorithms for detector effects, achieving high-statistics sample of random events for cosmic-ray background estimation | Neutrino event simulation and reconstruction performed in MicroBooNE using GENIE Monte Carlo with custom algorithms for detector effects, achieving high-statistics sample of random events for cosmic-ray background estimation | [
"MicroBooNE LArTPC detector",
"GENIE v3.0.6 G18 10a 02 11a event generator",
"Independent measurements from T2K experiment"
] | 0.85 | medium | universal | physics | arxiv | 2511.17342v1 | https://arxiv.org/abs/2511.17342v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | e3be0bb4afc8847855f7c36952abdf255551f9fb76459261a3605ebcecfadd55 | Extracted from ArXiv paper 2511.17342v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.17342v1"
} | science | WO-ARX-01 | 2025-12-07T12:40:49.413737Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124134182189 | Background-subtracted event count and unfolded cross-section measured as a function of visible energy, with values ranging from 2.10 to 3.78 × 10^-39 cm^2 / GeV / nucleon | Background-subtracted event count and unfolded cross-section measured as a function of visible energy, with values ranging from 2.10 to 3.78 × 10^-39 cm^2 / GeV / nucleon | [
"T2K experiment, Run 1 FHC data",
"Event count: 42.04 (0.05-0.45 GeV) to 2.44 (∞ GeV)",
"Selection efficiencies and response matrix used for unfolding"
] | 0.85 | medium | universal | physics | arxiv | 2511.17342v1 | https://arxiv.org/abs/2511.17342v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ca62824613ac4fd0c9804f25b5b916ba3392ccc93842f9c8f519288afe6a3c72 | Extracted from ArXiv paper 2511.17342v1 (chunk 22) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 22,
"paper_id": "2511.17342v1"
} | science | WO-ARX-01 | 2025-12-07T12:41:34.182189Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124136980375 | The unfolded cross-section is measured to be 2.36 in units of 10−39 cm / nucleon at a proton multiplicity of 3 | The unfolded cross-section is measured to be 2.36 in units of 10−39 cm / nucleon at a proton multiplicity of 3 | [
"Background-subtracted event count: 44.91",
"Proton multiplicity: 3",
"Unfolded cross section (Table III)"
] | 0.85 | medium | universal | physics | arxiv | 2511.17342v1 | https://arxiv.org/abs/2511.17342v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 576d1dbc8568123f8b2af661b0a861ae3de7754cc9fa0ff585d95c6578a39e37 | Extracted from ArXiv paper 2511.17342v1 (chunk 23) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 23,
"paper_id": "2511.17342v1"
} | science | WO-ARX-01 | 2025-12-07T12:41:36.980375Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124120417783 | LZ detector background rate for beta decays, detector gamma rays, solar neutrino ER, 136Xe 2νββ, and other components measured in WS2022 and WS2024 datasets | LZ detector background rate for beta decays, detector gamma rays, solar neutrino ER, 136Xe 2νββ, and other components measured in WS2022 and WS2024 datasets | [
"WS2022 dataset",
"Table I: pre-fit expectations and background-only fit results for main background components",
"WS2024 dataset"
] | 0.85 | medium | universal | physics | arxiv | 2511.17350v1 | https://arxiv.org/abs/2511.17350v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 338ff70c364508d03669a62baccfc5c9fe229d3097f502fe776e446c09b6ea1a | Extracted from ArXiv paper 2511.17350v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2511.17350v1"
} | science | WO-ARX-01 | 2025-12-07T12:41:20.417783Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124201322186 | Modified electron Hall parameter He′ was measured as a function of magnetic field strength for two experimental pressures. | Modified electron Hall parameter He′ was measured as a function of magnetic field strength for two experimental pressures. | [
"He′ measurements taken using the modified experimental setup",
"Experimental pressures: 2 values (not specified)",
"Magnetic field strength: varied"
] | 0.85 | medium | universal | physics | arxiv | 2511.17395v1 | https://arxiv.org/abs/2511.17395v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | dec23cc61b902b1d63c5cb4a8370921b7fc93bfa0fe279e885a672a30375f585 | Extracted from ArXiv paper 2511.17395v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2511.17395v1"
} | science | WO-ARX-01 | 2025-12-07T12:42:01.322186Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124145543760 | The CLD and IDEA detector concepts are compared in terms of their charged-hadron identification capabilities, using full simulation of the tracking systems. | The CLD and IDEA detector concepts are compared in terms of their charged-hadron identification capabilities, using full simulation of the tracking systems. | [
"CLIC-like detector (CLD) and innovative detector for e+e−accelerators (IDEA)",
"particle-identification algorithm",
"time-of-flight resolution and cluster-counting efficiency"
] | 0.85 | medium | universal | physics | arxiv | 2511.17447v1 | https://arxiv.org/abs/2511.17447v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 70793887765708933795af7b9245f3db7f4d7de602d7d7537810807245a4bea6 | Extracted from ArXiv paper 2511.17447v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2511.17447v1"
} | science | WO-ARX-01 | 2025-12-07T12:41:45.543760Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124210148139 | The time-of-flight resolution of the CLD detector must be better than 30-50 ps to reduce background contamination by at least an order of magnitude. | The time-of-flight resolution of the CLD detector must be better than 30-50 ps to reduce background contamination by at least an order of magnitude. | [
"CLD detector, simulation study",
"Background suppression from 10% to 1%",
"Signal window and background vetoes: ±10 MeV/c2"
] | 0.85 | high | universal | physics | arxiv | 2511.17447v1 | https://arxiv.org/abs/2511.17447v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 89b2bbf31a8db4286050da2bab9c85a6184787781027253b93087a1eb3f3ab3e | Extracted from ArXiv paper 2511.17447v1 (chunk 9) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2511.17447v1"
} | science | WO-ARX-01 | 2025-12-07T12:42:10.148139Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124218755079 | Particle identification in the FCC-ee detector can be achieved with a time-of-flight measurement alone, without dedicated particle-identification detectors, for certain momentum ranges. | Particle identification in the FCC-ee detector can be achieved with a time-of-flight measurement alone, without dedicated particle-identification detectors, for certain momentum ranges. | [
"IDEA detector concept at the FCC-ee",
"Three example physics studies covering low, medium, and high momentum regions",
"Time-of-flight resolution of 30 ps or better required in some cases"
] | 0.85 | medium | universal | physics | arxiv | 2511.17447v1 | https://arxiv.org/abs/2511.17447v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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] | 1d5c57a2d64b96f37dd990ac029c82cbbeaff34028f0707f488b4a5f22472cf3 | Extracted from ArXiv paper 2511.17447v1 (chunk 12) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:42:18.755079Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124227383420 | Measurements of time-of-flight resolution and cluster-counting efficiency for the IDEA detector, with/without silicone-based dE/dx measurement. | Measurements of time-of-flight resolution and cluster-counting efficiency for the IDEA detector, with/without silicone-based dE/dx measurement. | [
"IDEA detector, σToF = 3 ps, εcc = 80%",
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] | 0.85 | medium | universal | physics | arxiv | 2511.17447v1 | https://arxiv.org/abs/2511.17447v1 | [
"hep-ex",
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] | 39a91b1a6715dd8fe18f785fd98f504b0e69747d80f0507efcb60387d379c9a1 | Extracted from ArXiv paper 2511.17447v1 (chunk 15) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:42:27.383420Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124214772665 | A novel quantum sensing technology using microcalorimeter detectors is capable of resolving the hyperfine structure of the weakly populated 2s1/2 →2p3/2 transition in muonic atoms, enabling an improvement of quadrupole moments by an order of magnitude within days of measurement. | A novel quantum sensing technology using microcalorimeter detectors is capable of resolving the hyperfine structure of the weakly populated 2s1/2 →2p3/2 transition in muonic atoms, enabling an improvement of quadrupole moments by an order of magnitude within days of measurement. | [
"Microcalorimeter detectors",
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] | 0.85 | high | universal | physics | arxiv | 2511.17546v1 | https://arxiv.org/abs/2511.17546v1 | [
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] | d92732f83e7c18c3daa3d1d24b201f710f0a8ec673182ead60e5260f58fdd9f7 | Extracted from ArXiv paper 2511.17546v1 (chunk 7) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:42:14.772665Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124230205290 | Proper motions for 46 filaments in Tycho's supernova remnant have been measured with greater precision, consistent with previous measurements but with improved accuracy. | Proper motions for 46 filaments in Tycho's supernova remnant have been measured with greater precision, consistent with previous measurements but with improved accuracy. | [
"Optical images from eight epochs between 1986 and 2016",
"Matched continuum images revealed faint emission, including a network of optical knots and filaments",
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] | 0.85 | medium | universal | physics | arxiv | 2511.17763v1 | https://arxiv.org/abs/2511.17763v1 | [
"hep-ex",
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] | 623d50d33fe863a2584464e0553b497361ee7e7e4f6b23eabb593b318d8a7556 | Extracted from ArXiv paper 2511.17763v1 (chunk 0) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:42:30.205290Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124512892508 | A fast-simulation framework, Delphes, is used to emulate the behavior of a realistic CMS detector setup, allowing for controlled emulation of potential readout failures. | A fast-simulation framework, Delphes, is used to emulate the behavior of a realistic CMS detector setup, allowing for controlled emulation of potential readout failures. | [
"Delphes simulation tool",
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] | 0.85 | medium | universal | physics | arxiv | 2511.18172v1 | https://arxiv.org/abs/2511.18172v1 | [
"hep-ex",
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] | 5c8065000681065f9276fb869d0b01d9f5774ad3a99a02d58955772a75af5bb0 | Extracted from ArXiv paper 2511.18172v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:45:12.892508Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124533614210 | MEDIC, a novel end-to-end network, successfully detects and classifies detector glitches with strong discriminative power | MEDIC, a novel end-to-end network, successfully detects and classifies detector glitches with strong discriminative power | [
"Delphes simulation data",
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"Training on particle-level kinematics"
] | 0.85 | medium | universal | physics | arxiv | 2511.18172v1 | https://arxiv.org/abs/2511.18172v1 | [
"hep-ex",
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"astro-ph.HE"
] | 6756dddb05c952e424a1d05ff6bf840d2c50559e6cf2e2634df91f4467120f31 | Extracted from ArXiv paper 2511.18172v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.18172v1"
} | science | WO-ARX-01 | 2025-12-07T12:45:33.614210Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124716458361 | Detection horizon for ORCA24 detector reaches 11.2 kpc, while ARCA29 and ARCA230 detectors reach 10.0 kpc and 19.6 kpc respectively. | Detection horizon for ORCA24 detector reaches 11.2 kpc, while ARCA29 and ARCA230 detectors reach 10.0 kpc and 19.6 kpc respectively. | [
"ORCA24 detector configuration",
"5σ CCSN detection horizons evaluated separately for each detector",
"ARCA29 and ARCA230 configurations show similar performances"
] | 0.85 | high | universal | physics | arxiv | 2511.18565v1 | https://arxiv.org/abs/2511.18565v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 518b8603e8e2b4e489595176fab9dd9a116bff76f9fd9ffd580e90e6356209cd | Extracted from ArXiv paper 2511.18565v1 (chunk 14) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:47:16.458361Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124717108422 | A new kind of nucleosynthesis process, driven by high-entropy conditions and neutron-to-seed ratio drops, is observed to produce p-isotopes up to 92Mo | A new kind of nucleosynthesis process, driven by high-entropy conditions and neutron-to-seed ratio drops, is observed to produce p-isotopes up to 92Mo | [
"track 146 simulation data",
"neutron density low and r-process path closer to stability",
"(γ,n) and (p,n) reactions drive composition toward stability"
] | 0.85 | high | universal | physics | arxiv | 2511.18584v1 | https://arxiv.org/abs/2511.18584v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | 76d2c8e01d5828a0778967f59cac642392c1d61eb2653513ae06308086829f42 | Extracted from ArXiv paper 2511.18584v1 (chunk 12) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:47:17.108422Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124700324862 | Two new highly segmented HA-TPCs in the ND280 detector achieved spatial resolution better than 800 µm and dE/dx resolution better than 10% across all incident angles and drift distances | Two new highly segmented HA-TPCs in the ND280 detector achieved spatial resolution better than 800 µm and dE/dx resolution better than 10% across all incident angles and drift distances | [
"HA-TPC readout system utilizing resistive Micromegas technology",
"Spatial resolution: < 800 µm, dE/dx resolution: < 10%",
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] | 0.85 | medium | universal | physics | arxiv | 2511.18650v1 | https://arxiv.org/abs/2511.18650v1 | [
"hep-ex",
"nucl-ex",
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] | 34416346069abf2a284882a3f52e79533128247ed73ef62f15f4ec910532df2c | Extracted from ArXiv paper 2511.18650v1 (chunk 2) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:47:00.324862Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124712350136 | ERAM detectors exhibit gain and RC values with distinct production trends, influenced by mechanical imprints, gap thickness, and surface resistivity. | ERAM detectors exhibit gain and RC values with distinct production trends, influenced by mechanical imprints, gap thickness, and surface resistivity. | [
"Dedicated X-ray test bench for pad-by-pad scan",
"12 parameters (RC) for each module analyzed using physical model [4]",
"15% systematic uncertainty in gain and 13% in RC due to electronics model choices"
] | 0.85 | medium | universal | physics | arxiv | 2511.18650v1 | https://arxiv.org/abs/2511.18650v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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"astro-ph.HE"
] | 298e29fdd90796f58dbbba9252d8a9c80c2f3ffca4043fa1e7427cdfc1ab6d08 | Extracted from ArXiv paper 2511.18650v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:47:12.350660Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124746489274 | Momentum resolution for vertical tracks in HA-TPCs reaches slightly less than 10% at 1 GeV/c, with some bias observed due to E × B effects | Momentum resolution for vertical tracks in HA-TPCs reaches slightly less than 10% at 1 GeV/c, with some bias observed due to E × B effects | [
"Belle II detector, 2023 data sample",
"362 million B-meson pairs analyzed",
"Systematic uncertainty: 0.008"
] | 0.85 | medium | universal | physics | arxiv | 2511.18650v1 | https://arxiv.org/abs/2511.18650v1 | [
"hep-ex",
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"physics.plasm-ph",
"astro-ph.HE"
] | 73c10c4ae50bb0be7ec1be810103473d9bc3c84d8d53b47ed8bf3850a42b19d9 | Extracted from ArXiv paper 2511.18650v1 (chunk 17) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 17,
"paper_id": "2511.18650v1"
} | science | WO-ARX-01 | 2025-12-07T12:47:46.489274Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124817554929 | RELICS detector prototype demonstrates efficient data processing and signal classification, achieving high accuracy in separating physical signals from background features. | RELICS detector prototype demonstrates efficient data processing and signal classification, achieving high accuracy in separating physical signals from background features. | [
"Dual-phase xenon time projection chamber (TPC) experiment",
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"Identification of distinct signal types: S1, S2, DE, Muon Tracks, Lone Hits / Single Photoelectrons"
] | 0.85 | high | universal | physics | arxiv | 2511.18693v1 | https://arxiv.org/abs/2511.18693v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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"astro-ph.HE"
] | 683514cdafe2c714e74117748bc00b55dc76f19fcf6c8e36009d44ed8063b126 | Extracted from ArXiv paper 2511.18693v1 (chunk 13) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.18693v1"
} | science | WO-ARX-01 | 2025-12-07T12:48:17.554929Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124849807975 | The first indication of solar 8B neutrinos is observed through coherent elastic neutrino-nucleus scattering in PandaX-4T. | The first indication of solar 8B neutrinos is observed through coherent elastic neutrino-nucleus scattering in PandaX-4T. | [
"PandaX-4T detector, data from 2024",
"Observed event rate: 0.15 events/kg/ day",
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] | 0.85 | high | universal | physics | arxiv | 2511.18693v1 | https://arxiv.org/abs/2511.18693v1 | [
"hep-ex",
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"astro-ph.HE"
] | a8ca0717edd47ebf5c42596aac9f46fe77fdef0b0ddc8d3988ff136d14980dc5 | Extracted from ArXiv paper 2511.18693v1 (chunk 23) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 23,
"paper_id": "2511.18693v1"
} | science | WO-ARX-01 | 2025-12-07T12:48:49.807975Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124828259800 | Up to six-fold ionization of Ar was observed in collisions with carbon ions, and recoil ion yield showed a different distribution for single capture events compared to ionization. | Up to six-fold ionization of Ar was observed in collisions with carbon ions, and recoil ion yield showed a different distribution for single capture events compared to ionization. | [
"RIMS + CSA experimental setup",
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] | 0.85 | medium | universal | physics | arxiv | 2511.18707v1 | https://arxiv.org/abs/2511.18707v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 91c5fa397e79749e5ae69878aad1abb275e34a4fae74a51e6306fc0ce9669b56 | Extracted from ArXiv paper 2511.18707v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 7,
"paper_id": "2511.18707v1"
} | science | WO-ARX-01 | 2025-12-07T12:48:28.260331Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124852231757 | Magneto-optical resonances observed in cesium vapor cell with electromagnetically induced transparency and absorption | Magneto-optical resonances observed in cesium vapor cell with electromagnetically induced transparency and absorption | [
"cesium vapor cell, balanced photodetector used for pump and probe wave transmission",
"pump intensity: P ≈400 µW (Fig. 6(a)), P ≈1000 µW (Fig. 6(d))",
"magnetic field scanning"
] | 0.85 | medium | universal | physics | arxiv | 2511.18710v1 | https://arxiv.org/abs/2511.18710v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 69179e7f7d0a19683ff06dbbe89caf3b939bd57dd506eb278c6d2615edc10d5a | Extracted from ArXiv paper 2511.18710v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2511.18710v1"
} | science | WO-ARX-01 | 2025-12-07T12:48:52.231757Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124851462330 | A hierarchical Bayesian scheme is developed for inferring pulsar braking indices and timing residual root-mean-square from TOA data, with the model successfully reproducing observed pulse shapes and times of arrival. | A hierarchical Bayesian scheme is developed for inferring pulsar braking indices and timing residual root-mean-square from TOA data, with the model successfully reproducing observed pulse shapes and times of arrival. | [
"TOA (Time Of Arrival) data",
"Pulsar timing residuals",
"Hierarchical Bayesian inference"
] | 0.85 | medium | universal | physics | arxiv | 2511.18744v1 | https://arxiv.org/abs/2511.18744v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 59d2f4985f96645463fa8b3718c1f0d3216be2b051c02dee79c3baca800ad9a9 | Extracted from ArXiv paper 2511.18744v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2511.18744v1"
} | science | WO-ARX-01 | 2025-12-07T12:48:51.462330Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124914275979 | The capture rates of φ's were evaluated for different scattering cross sections and lifetimes, reaching a maximum value at IceCube for certain values of the parameters. | The capture rates of φ's were evaluated for different scattering cross sections and lifetimes, reaching a maximum value at IceCube for certain values of the parameters. | [
"IceCube data",
"Scattering cross section: σφN = 10−44 cm2",
"Lifetime: τφ = 1018 s"
] | 0.85 | medium | universal | physics | arxiv | 2511.18881v2 | https://arxiv.org/abs/2511.18881v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 2309312931238e711760233d968ae717a39d9142264481de6d033a1823faaa65 | Extracted from ArXiv paper 2511.18881v2 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2511.18881v2"
} | science | WO-ARX-01 | 2025-12-07T12:49:14.275979Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_124922513634 | Blazars show variability across the electromagnetic spectrum, with flux and spectral variations observed on various time scales. | Blazars show variability across the electromagnetic spectrum, with flux and spectral variations observed on various time scales. | [
"blazar observations",
"jet precession",
"twisting jets"
] | 0.85 | medium | universal | physics | arxiv | 2511.18975v1 | https://arxiv.org/abs/2511.18975v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | da54be8258287e5bb7a7a4d88b0d7dacb29730c547821e30e5e28404ba660bb7 | Extracted from ArXiv paper 2511.18975v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.18975v1"
} | science | WO-ARX-01 | 2025-12-07T12:49:22.513634Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125051559454 | Polarisation degree of jet radiation measured in BL Lacs, with P ranging from 60% to 82%, depending on the magnetic field properties | Polarisation degree of jet radiation measured in BL Lacs, with P ranging from 60% to 82%, depending on the magnetic field properties | [
"ArXiv paper 2511.18975v1",
"Theory of synchrotron radiation by Rybicki and Lightman (1979)",
"Observed polarisation degree in BL Lacs, with maximum P observed lower than expected"
] | 0.85 | medium | universal | physics | arxiv | 2511.18975v1 | https://arxiv.org/abs/2511.18975v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 0052865f88e9eeb7f712954df909d67bd8eaf26be0b2305d3a9378b96be642fa | Extracted from ArXiv paper 2511.18975v1 (chunk 31) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 31,
"paper_id": "2511.18975v1"
} | science | WO-ARX-01 | 2025-12-07T12:50:51.559454Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125102296123 | Breakdown voltage and quenching resistor of FBK NUV-HD-Cryo 3T SiPMs measured at room and LN2 temperatures, with 33.0±0.1 V and 560±10 kΩ at 300 K, decreasing to 27.08±0.03 V and 2640±70 kΩ at 77 K | Breakdown voltage and quenching resistor of FBK NUV-HD-Cryo 3T SiPMs measured at room and LN2 temperatures, with 33.0±0.1 V and 560±10 kΩ at 300 K, decreasing to 27.08±0.03 V and 2640±70 kΩ at 77 K | [
"IV curve measurements",
"Breakdown voltage: 33.0±0.1 V at room temperature, decreasing to 27.08±0.03 V at LN2 temperature",
"Quenching resistor: 560±10 kΩ at room temperature, increasing to 2640±70 kΩ at LN2 temperature"
] | 0.85 | medium | universal | physics | arxiv | 2511.19095v1 | https://arxiv.org/abs/2511.19095v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 4dac15c3e43368910483c7e172576f13093f054c7e104dd7ef4c1afcb3babefd | Extracted from ArXiv paper 2511.19095v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19095v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:02.296650Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125122072833 | Breakdown voltage of ion-ion plasma measured at -5.9 ± 0.05 kV and +7.65 ± 0.05 kV for a 500 ns time window | Breakdown voltage of ion-ion plasma measured at -5.9 ± 0.05 kV and +7.65 ± 0.05 kV for a 500 ns time window | [
"Experimental measurement, Fig. 2(f)",
"Ion accumulation stage with electrons forming a negative ion region",
"Space charge field aligning with the negative applied field"
] | 0.85 | high | universal | physics | arxiv | 2511.19136v1 | https://arxiv.org/abs/2511.19136v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c4fe684734c92423119b5be4b3cc36d0dd5fad83fa81722193787d329ef6c12f | Extracted from ArXiv paper 2511.19136v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19136v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:22.072833Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125113898748 | Only a fraction as small as ∼10−3 of Luminous Red Novae correspond to gravitational-wave observed binary neutron star and neutron star-black hole mergers. | Only a fraction as small as ∼10−3 of Luminous Red Novae correspond to gravitational-wave observed binary neutron star and neutron star-black hole mergers. | [
"Zwicky Transient Facility (ZTF) observations",
"Fourth Gravitational Wave transient catalog (GWTC-4)",
"Delay time distribution models for compact binaries"
] | 0.85 | high | universal | physics | arxiv | 2511.19243v1 | https://arxiv.org/abs/2511.19243v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 1d14c20682c670e32ba869ac788dd6f1162b7aac8e3f20e3b235ceea93a057a2 | Extracted from ArXiv paper 2511.19243v1 (chunk 0) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19243v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:13.898748Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125145751217 | Apparent jet speeds in XRBs are significantly lower than those of blazars, with observed speeds up to 5.3. | Apparent jet speeds in XRBs are significantly lower than those of blazars, with observed speeds up to 5.3. | [
"ThunderKAT program and GRS 1915+105 measurements",
"4U 1543-47 jets show 𝛽app ∼5.3",
"AGN and blazars have apparent speeds up to 𝛽app ∼50"
] | 0.85 | medium | universal | physics | arxiv | 2511.19362v1 | https://arxiv.org/abs/2511.19362v1 | [
"hep-ex",
"nucl-ex",
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"astro-ph.HE"
] | b446fe661d535b98e7e5f91f0d8e3e66d0b1250c8e8174b49b157cfd0815aa65 | Extracted from ArXiv paper 2511.19362v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19362v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:45.751217Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125148494046 | The apparent speed of XRB jets is limited by inclination and sample size, with speeds up to 5, much lower than those observed in AGN. | The apparent speed of XRB jets is limited by inclination and sample size, with speeds up to 5, much lower than those observed in AGN. | [
"XRB jet speed sample compiled by Fender & Motta (2025)",
"Estimated apparent speed from proper motion data",
"Significant uncertainty in inclination measurement"
] | 0.85 | medium | universal | physics | arxiv | 2511.19362v1 | https://arxiv.org/abs/2511.19362v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ed49d8e8f3f834852c6cfc5cfc8072c60c32ea1864f40df9ff46571345713cb2 | Extracted from ArXiv paper 2511.19362v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19362v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:48.494596Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125155057441 | The observed apparent speed distribution of X-ray binaries (XRBs) is largely unaffected by changes in intrinsic Lorentz factor due to their high inclination angles, while active galactic nuclei (AGN) show a peak at low inclination angles. | The observed apparent speed distribution of X-ray binaries (XRBs) is largely unaffected by changes in intrinsic Lorentz factor due to their high inclination angles, while active galactic nuclei (AGN) show a peak at low inclination angles. | [
"Sample of XRBs and AGN",
"Inclination angle distributions",
"Apparent speed distribution"
] | 0.85 | medium | universal | physics | arxiv | 2511.19362v1 | https://arxiv.org/abs/2511.19362v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c4c400dee777962e2f43ccb4e7915784c11ba1716883e553bb00d9fbf06acc1c | Extracted from ArXiv paper 2511.19362v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19362v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:55.057441Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125158476137 | The IceCube detector collected ∼1.67 million low-energy neutrino events between 2011 and 2017, comprising ∼2600 days of detector livetime. | The IceCube detector collected ∼1.67 million low-energy neutrino events between 2011 and 2017, comprising ∼2600 days of detector livetime. | [
"IceCube in-ice Cherenkov detector",
"∼2600 days of detector livetime",
"0.5 ≲log(Eν/GeV) ≲2.5"
] | 0.85 | medium | universal | physics | arxiv | 2511.19385v1 | https://arxiv.org/abs/2511.19385v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 5cc84796387cab3bf0e77bda7815562dedca55d02ef16280300aef20cc4eac1e | Extracted from ArXiv paper 2511.19385v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 5,
"paper_id": "2511.19385v1"
} | science | WO-ARX-01 | 2025-12-07T12:51:58.476137Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125224682883 | JUNO experiment measured sin^2 θ12 to unprecedented precision, reducing relative uncertainty by a factor of 1.6 | JUNO experiment measured sin^2 θ12 to unprecedented precision, reducing relative uncertainty by a factor of 1.6 | [
"JUNO experiment",
"sin^2 θ12 = 0.3092 ± 0.0087",
"∆m^2_21 = (7.50 ± 0.12) × 10^-5 eV^2"
] | 0.85 | high | universal | physics | arxiv | 2511.19408v1 | https://arxiv.org/abs/2511.19408v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | eb58f85d08b19d5cfee5740e4db59d4300cb5fe1bc6ca6a56e3929cec9f6938c | Extracted from ArXiv paper 2511.19408v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 0,
"paper_id": "2511.19408v1"
} | science | WO-ARX-01 | 2025-12-07T12:52:24.683398Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125332183582 | XMM-Newton observed five INS candidates, removing high background flaring periods and refining astrometry using optical sources in the Guide Star Catalogue | XMM-Newton observed five INS candidates, removing high background flaring periods and refining astrometry using optical sources in the Guide Star Catalogue | [
"XMM-Newton observations, 50 - 80 ks each between May 2023 and April 2024",
"EPIC-pn and MOS detectors, applying FLAG = 0 and PATTERN ≤12",
"Background regions defined on same chip or neighboring chip"
] | 0.85 | medium | universal | physics | arxiv | 2511.19591v1 | https://arxiv.org/abs/2511.19591v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 87ce4ec6198f3d5519a684717ea8fd5306a4ecc09c18f12b884360448f55589e | Extracted from ArXiv paper 2511.19591v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 2,
"paper_id": "2511.19591v1"
} | science | WO-ARX-01 | 2025-12-07T12:53:32.183582Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125414279029 | Obscuration of X-ray detected sources in C iv and [Ne v] samples measured, with 48 out of 84 sources obscured (N_H >= 10^22 cm^-2) and 37 extremely obscured (N_H > 10^23 cm^-2) | Obscuration of X-ray detected sources in C iv and [Ne v] samples measured, with 48 out of 84 sources obscured (N_H >= 10^22 cm^-2) and 37 extremely obscured (N_H > 10^23 cm^-2) | [
"X-ray detected sources in the C iv and [Ne v] samples",
"Obscuration measured via power-law model with fixed photon index Γ = 1.8 plus an absorption component",
"Median spectral properties reported in Table 3"
] | 0.85 | high | universal | physics | arxiv | 2511.19602v1 | https://arxiv.org/abs/2511.19602v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ac0b2e16bc72563b4c4b7add1bf9daefe549bfe622ef44b2ad7f922b334aaedb | Extracted from ArXiv paper 2511.19602v1 (chunk 9) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 9,
"paper_id": "2511.19602v1"
} | science | WO-ARX-01 | 2025-12-07T12:54:14.279029Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125438389388 | The eccentric gravitational-wave model developed in this work is equally applicable to Galactic stellar-mass binaries, such as white dwarfs, neutron stars, and black holes, that will be observed by LISA. | The eccentric gravitational-wave model developed in this work is equally applicable to Galactic stellar-mass binaries, such as white dwarfs, neutron stars, and black holes, that will be observed by LISA. | [
"LISA (Laser Interferometer Space Antenna)",
"Galactic stellar-mass binaries",
"White dwarfs, neutron stars, and black holes"
] | 0.85 | high | universal | physics | arxiv | 2511.19611v1 | https://arxiv.org/abs/2511.19611v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c3b57f5a9ae6621a4acb3a02fd15671a8781e2bb72809498e08bd6c65fbb374a | Extracted from ArXiv paper 2511.19611v1 (chunk 12) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 12,
"paper_id": "2511.19611v1"
} | science | WO-ARX-01 | 2025-12-07T12:54:38.389388Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125510280131 | New mass values for neutron-rich tin and antimony isotopes near 132Sn were measured with a Penning trap mass spectrometer. | New mass values for neutron-rich tin and antimony isotopes near 132Sn were measured with a Penning trap mass spectrometer. | [
"Canadian Penning Trap mass spectrometer (CPT)",
"CARIBU facility at Argonne National Laboratory",
"Beam production from a 252Cf source"
] | 0.85 | medium | universal | physics | arxiv | 2511.19673v2 | https://arxiv.org/abs/2511.19673v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c5ec20ebc4c9792ae7725973d8a504c80fada67351fb3b207ba3f977ac752a91 | Extracted from ArXiv paper 2511.19673v2 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 1,
"paper_id": "2511.19673v2"
} | science | WO-ARX-01 | 2025-12-07T12:55:10.280131Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125513874191 | The cyclotron frequency of ions in a Penning trap is measured using the Phase-Imaging Ion-Cyclotron-Resonance technique, with an uncertainty of less than part in 10^9. | The cyclotron frequency of ions in a Penning trap is measured using the Phase-Imaging Ion-Cyclotron-Resonance technique, with an uncertainty of less than part in 10^9. | [
"CPT’s Stable Ion Source",
"133Cs+ calibrant mass used for calibration",
"MCP position sensitive detector"
] | 0.85 | medium | universal | physics | arxiv | 2511.19673v2 | https://arxiv.org/abs/2511.19673v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | bc751ff2ad54998e2d09c54a20987e7e9b080b14dcdddbf4d89098427c4e5ca5 | Extracted from ArXiv paper 2511.19673v2 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2511.19673v2"
} | science | WO-ARX-01 | 2025-12-07T12:55:13.874191Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125534861620 | Effective single-photon absorption probability measured with cat state spectroscopy, reaching a maximum value of 0.12(1) after applying 34 laser pulses | Effective single-photon absorption probability measured with cat state spectroscopy, reaching a maximum value of 0.12(1) after applying 34 laser pulses | [
"Femtosecond laser pulses with center frequency of 3703.3(2) cm^-1",
"Photon absorption signal S = 0.12(1)",
"Comparison with simple theoretical model"
] | 0.85 | medium | universal | physics | arxiv | 2511.19687v1 | https://arxiv.org/abs/2511.19687v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 78fac9d800411d83852273d4dcfe488855ae69714ca41605af99b3cd740caec6 | Extracted from ArXiv paper 2511.19687v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.19687v1"
} | science | WO-ARX-01 | 2025-12-07T12:55:34.861620Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125647498159 | Leading-order photoproduction cross sections for γN →γM N′ are calculated with quark GPD contributions, showing strong sensitivity to pion distribution amplitude and gluon content. | Leading-order photoproduction cross sections for γN →γM N′ are calculated with quark GPD contributions, showing strong sensitivity to pion distribution amplitude and gluon content. | [
"pseudoscalar channels M ∈{π±, π0, η, η′}",
"leading-twist and leading-order in perturbative QCD",
"renormalization scale dependence highlighted"
] | 0.85 | medium | universal | physics | arxiv | 2511.19720v1 | https://arxiv.org/abs/2511.19720v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | a449d6aefbb03b1fe1c3f78b7267efb537da06a1c0e95978c83e08dd5963c6f5 | Extracted from ArXiv paper 2511.19720v1 (chunk 22) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 22,
"paper_id": "2511.19720v1"
} | science | WO-ARX-01 | 2025-12-07T12:56:47.498159Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125659677959 | Fully differential cross-section for γN →γM N′ measured, with significant pion-pole contribution at small ξ values | Fully differential cross-section for γN →γM N′ measured, with significant pion-pole contribution at small ξ values | [
"Figs. 5-9: numerical results for fully differential cross-section",
"Kinematics varied across Figs.: SγN = 20 GeV2, s' = 4 GeV2, (−t) = (−t0)",
"Different mesons represented by different line styles"
] | 0.85 | medium | universal | physics | arxiv | 2511.19720v1 | https://arxiv.org/abs/2511.19720v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 4c41aa46efeccbf811d187ae787b38b916ede34fea60f7ad7ab38201fb418276 | Extracted from ArXiv paper 2511.19720v1 (chunk 26) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 26,
"paper_id": "2511.19720v1"
} | science | WO-ARX-01 | 2025-12-07T12:56:59.677959Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125555830397 | Channeling efficiencies exceeding 50% were measured in bent silicon crystals at low energy, with a record at sub-GeV domain. | Channeling efficiencies exceeding 50% were measured in bent silicon crystals at low energy, with a record at sub-GeV domain. | [
"855 MeV electron beam at Mainz Microtron (MAMI)",
"15 µm-thick crystal bent along (111) planes",
"Measured channeling efficiencies"
] | 0.85 | high | universal | physics | arxiv | 2511.19807v1 | https://arxiv.org/abs/2511.19807v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | dd27e811b6cfb8dbdd1ad81ca18d22177e839010fc440331904ea512425a12ed | Extracted from ArXiv paper 2511.19807v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2511.19807v1"
} | science | WO-ARX-01 | 2025-12-07T12:55:55.830397Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125615106511 | The dechanneling length was measured to be 21 µm at 855 MeV, decreasing to 14 µm at 600 MeV and 9.4 µm at 300 MeV. | The dechanneling length was measured to be 21 µm at 855 MeV, decreasing to 14 µm at 600 MeV and 9.4 µm at 300 MeV. | [
"Bent crystals with varying lengths were simulated",
"Exponential decay fit: Nch(ℓ) = N0 exp(−ℓ/Ld)",
"NaI(Tl) detector placed at L = 8.627 m"
] | 0.85 | medium | universal | physics | arxiv | 2511.19807v1 | https://arxiv.org/abs/2511.19807v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | b4930c1e6a4632d15fcc921e1068044b252236dd13e8877c726cb1b19818e5db | Extracted from ArXiv paper 2511.19807v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2511.19807v1"
} | science | WO-ARX-01 | 2025-12-07T12:56:15.106511Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125635560312 | The bunch duration of relativistic electron beams is measured to be approximately 4 fs using momentum spectra measurements. | The bunch duration of relativistic electron beams is measured to be approximately 4 fs using momentum spectra measurements. | [
"Phys. Rev. Accel. Beams, 27, 2024.",
"Sparc lab experiments",
"Momentum spectra analysis"
] | 0.85 | medium | universal | physics | arxiv | 2511.19807v1 | https://arxiv.org/abs/2511.19807v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 2087adeaaef985dc270c141545996ba8349497b439b0a8911566479ba0f17f84 | Extracted from ArXiv paper 2511.19807v1 (chunk 14) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 14,
"paper_id": "2511.19807v1"
} | science | WO-ARX-01 | 2025-12-07T12:56:35.560832Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125649938172 | The SBC 10 kg liquid argon detector has a potential for world leading sensitivity to O(GeV/c^2) mass dark matter and to perform a high statistics reactor CEνNS measurement. | The SBC 10 kg liquid argon detector has a potential for world leading sensitivity to O(GeV/c^2) mass dark matter and to perform a high statistics reactor CEνNS measurement. | [
"SBC 10 kg liquid argon detector",
"Calibration campaign with systematic uncertainties comparable to other recent bubble chamber calibrations",
"Simulations at four thresholds from 80 to 400 eV"
] | 0.85 | high | universal | physics | arxiv | 2511.19817v1 | https://arxiv.org/abs/2511.19817v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ad4cd602c776c3fe9260d7c074f11f49f09ed83ebffc9748aabf72928c0540bc | Extracted from ArXiv paper 2511.19817v1 (chunk 16) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 16,
"paper_id": "2511.19817v1"
} | science | WO-ARX-01 | 2025-12-07T12:56:49.938172Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125718511797 | The Kasen effect, a sudden brightening after a supernova explosion due to a red giant companion, is not observed in six normal SNIa, contradicting expectations. | The Kasen effect, a sudden brightening after a supernova explosion due to a red giant companion, is not observed in six normal SNIa, contradicting expectations. | [
"TESS full-frame data for 307 SNIa",
"No prominent Kasen peaks detected in light curves",
"Weak signals in residuals plots"
] | 0.85 | high | universal | physics | arxiv | 2511.19948v1 | https://arxiv.org/abs/2511.19948v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d3a900e36e52121f6e9dc114fd396507c238fe53f30c114aa2b29d340e9435f2 | Extracted from ArXiv paper 2511.19948v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.19948v1"
} | science | WO-ARX-01 | 2025-12-07T12:57:18.511797Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125740268662 | Cross-section values for 𝜒0~2𝜒±~1, 𝜒0~2𝜒0~1, 𝜒0~1𝜒±~1, and 𝜒+~1𝜒−~1 production are measured as 5.3 ± 0.2 pb, 3.2 ± 0.1 pb, 5.5 ± 0.2 pb, and 2.9 ± 0.1 pb respectively, using ATLAS detector | Cross-section values for 𝜒0~2𝜒±~1, 𝜒0~2𝜒0~1, 𝜒0~1𝜒±~1, and 𝜒+~1𝜒−~1 production are measured as 5.3 ± 0.2 pb, 3.2 ± 0.1 pb, 5.5 ± 0.2 pb, and 2.9 ± 0.1 pb respectively, using ATLAS detector | [
"ATLAS detector",
"Resummino 2.0.1 at NLO+NLL precision",
"CTEQ6.6 [76] and MSTW2008nlo90cl [77] PDF sets"
] | 0.85 | medium | universal | physics | arxiv | 2511.20042v1 | https://arxiv.org/abs/2511.20042v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | e170c36a529885ec4aa0d58cec5e6c9848df335ec8c88e923f159d22033897ff | Extracted from ArXiv paper 2511.20042v1 (chunk 7) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T12:57:40.268662Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125747052985 | Low- pT lepton-track identification methods developed to distinguish leptons from hadrons and fake combinatorial tracks in the inner detector, with dedicated optimisations for electron-tracks and muon-tracks | Low- pT lepton-track identification methods developed to distinguish leptons from hadrons and fake combinatorial tracks in the inner detector, with dedicated optimisations for electron-tracks and muon-tracks | [
"Tight Primary working point defined in Ref. [117]",
"Preselected tracks with pT > 500 MeV and |η| < 2.5",
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] | 0.85 | medium | universal | physics | arxiv | 2511.20042v1 | https://arxiv.org/abs/2511.20042v1 | [
"hep-ex",
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"astro-ph.HE"
] | 1ce441cf284e716355008d1b1a25e0c49d7138caf853af73724cdba2249511a4 | Extracted from ArXiv paper 2511.20042v1 (chunk 9) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.20042v1"
} | science | WO-ARX-01 | 2025-12-07T12:57:47.053496Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125817128006 | Normalisation factors for Z+jets and diboson processes measured as 1.29 ± 0.01 and 1.4 ± 0.2, respectively | Normalisation factors for Z+jets and diboson processes measured as 1.29 ± 0.01 and 1.4 ± 0.2, respectively | [
"ATLAS detector",
"2022 LHC run data",
"Normalisation factor for W±(→τ± hadντ)+jets processes: 1.37 ± 0.04"
] | 0.85 | medium | universal | physics | arxiv | 2511.20042v1 | https://arxiv.org/abs/2511.20042v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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"astro-ph.HE"
] | 7be6d816885db44fa429d0880f37c067f1ea08772a522c82cdfc4d005a580814 | Extracted from ArXiv paper 2511.20042v1 (chunk 18) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 18,
"paper_id": "2511.20042v1"
} | science | WO-ARX-01 | 2025-12-07T12:58:17.128006Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125835610852 | The ATLAS detector observes good agreement between data and predicted background event yields in validation regions, with deviations below 2σ. | The ATLAS detector observes good agreement between data and predicted background event yields in validation regions, with deviations below 2σ. | [
"ATLAS detector",
"14 TeV, 140 fb−1 collision data",
"good agreement observed in all VRs for both displaced track and 1ℓ1T searches"
] | 0.85 | medium | universal | physics | arxiv | 2511.20042v1 | https://arxiv.org/abs/2511.20042v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 00247bdd11b30fae1da04ea9bb0fae1ba04c6df18daab4d9c1fcb9678d0440ec | Extracted from ArXiv paper 2511.20042v1 (chunk 24) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 24,
"paper_id": "2511.20042v1"
} | science | WO-ARX-01 | 2025-12-07T12:58:35.610852Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_125842287449 | The ATLAS collaboration observed a significance of up to 5.8 sigma in the pNN-θ=4 GeV slice for SR-1ℓ1T. | The ATLAS collaboration observed a significance of up to 5.8 sigma in the pNN-θ=4 GeV slice for SR-1ℓ1T. | [
"ATLAS detector, 13 TeV collision data",
"Observed yield: 7 events",
"Fitted SM background: 10.0 ± 2.4"
] | 0.85 | high | universal | physics | arxiv | 2511.20042v1 | https://arxiv.org/abs/2511.20042v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | fc1d79901d0c08cb7fdcd24d4242f59a43a4227b33a7cd91037a7409d0e9e248 | Extracted from ArXiv paper 2511.20042v1 (chunk 26) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 26,
"paper_id": "2511.20042v1"
} | science | WO-ARX-01 | 2025-12-07T12:58:42.287449Z | arxiv | physics_recovered | arxiv_physics |
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