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_20251209_194226192562 | The formation of skyrmioniums from multiple skyrmions is observed as a topological transition by tuning the relative twist angle between two metasurface layers, with strong consistency among theoretical predictions, numerical simulations, and experimental measurements. | The formation of skyrmioniums from multiple skyrmions is observed as a topological transition by tuning the relative twist angle between two metasurface layers, with strong consistency among theoretical predictions, numerical simulations, and experimental measurements. | [
"Elastic-wave metasurface samples fabricated by 3D printing",
"Lamb waves excited by PZT-5H patches bonded to top and bottom layers",
"Out-of-plane displacement fields reconstructed using a PSV-500-1D scanning head"
] | 0.85 | high | universal | physics | arxiv | 2511.16002v1 | https://arxiv.org/abs/2511.16002v1 | [
"physics.app-ph"
] | 4a108992eecc4abcbfe0e823a6b43388c6c29a966b2aa0b6fc46d8d9db379af7 | Extracted from ArXiv paper 2511.16002v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2511.16002v1"
} | science | WO-ARX-01 | 2025-12-09T19:42:26.192562Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_194516051121 | Correlation times for CO desorption from Ru(0001) measured as 20 ps, indicating a phonon-driven process. | Correlation times for CO desorption from Ru(0001) measured as 20 ps, indicating a phonon-driven process. | [
"Ru(0001) substrate",
"Desorption probability curve analysis",
"Correlation time: 20 ps"
] | 0.85 | high | universal | physics | arxiv | 2511.17042v1 | https://arxiv.org/abs/2511.17042v1 | [
"physics.chem-ph"
] | c75ab86be5ca925cabfe2f06e06995db5c101d00b6ddb73738973b2c46e1b9df | Extracted from ArXiv paper 2511.17042v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2511.17042v1"
} | science | WO-ARX-01 | 2025-12-09T19:45:16.051121Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_194515491208 | Densities of (2-propanol + glyme) systems measured at temperatures ranging from 293.15 to 303.15 K and pressure 0.1 MPa, with excess molar volumes calculated | Densities of (2-propanol + glyme) systems measured at temperatures ranging from 293.15 to 303.15 K and pressure 0.1 MPa, with excess molar volumes calculated | [
"DSA 5000 densimeter by Anton Paar",
"Temperature range: (293.15 to 303.15) K",
"Pressure: 0.1 MPa"
] | 0.85 | medium | universal | physics | arxiv | 2511.17057v1 | https://arxiv.org/abs/2511.17057v1 | [
"physics.chem-ph"
] | 3fc176f45d7ee9b53d0ffb66c94566100b1d2ff33b0fd86145cb0b3e593f425b | Extracted from ArXiv paper 2511.17057v1 (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": "2511.17057v1"
} | science | WO-ARX-01 | 2025-12-09T19:45:15.491208Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_194616835249 | Excess enthalpies for various oxygenated compounds + hydrocarbon mixtures were measured at different temperatures. | Excess enthalpies for various oxygenated compounds + hydrocarbon mixtures were measured at different temperatures. | [
"J. Chem. Eng. Data, various papers (1986-2014)",
"Excess enthalpy measurements for specific mixtures: e.g., 1-Butoxybutane + Propan-1-ol + 1-Hex-1-ene",
"Temperature range: 298.15 K to 313.15 K"
] | 0.85 | medium | universal | physics | arxiv | 2511.17057v1 | https://arxiv.org/abs/2511.17057v1 | [
"physics.chem-ph"
] | 928ac1d28a85d8d97280b20670f9551ee32f0c0eb9644526134e775815fca51b | Extracted from ArXiv paper 2511.17057v1 (chunk 20) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 20,
"paper_id": "2511.17057v1"
} | science | WO-ARX-01 | 2025-12-09T19:46:16.835249Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_194627361215 | Excess partial molar volumes and enthalpies of 2-propanol and linear polyether mixtures measured at various temperatures | Excess partial molar volumes and enthalpies of 2-propanol and linear polyether mixtures measured at various temperatures | [
"Temperature range: 293.15 K to 303.15 K",
"Pressure: 0.1 MPa",
"Measurement uncertainty reported"
] | 0.85 | medium | universal | physics | arxiv | 2511.17057v1 | https://arxiv.org/abs/2511.17057v1 | [
"physics.chem-ph"
] | 87f22d84ec1296c0830d64e23dd03871891403db28521811fc246f44bc81518a | Extracted from ArXiv paper 2511.17057v1 (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": "2511.17057v1"
} | science | WO-ARX-01 | 2025-12-09T19:46:27.361215Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_195016202843 | Background Argon plasma parameters, including floating potential and electron temperature, exhibit a radial variation when measured with a Langmuir probe | Background Argon plasma parameters, including floating potential and electron temperature, exhibit a radial variation when measured with a Langmuir probe | [
"Langmuir probe measurements at z = 12.5 mm",
"Floating potential varies radially (Fig. 4.16a)",
"Electron temperature does not vary radially"
] | 0.85 | medium | universal | physics | arxiv | 2511.17395v1 | https://arxiv.org/abs/2511.17395v1 | [
"physics.plasm-ph"
] | 50dc5f95b88f2c551b66507bc4d251183fb3867c4edcbf417de38522d696dc54 | Extracted from ArXiv paper 2511.17395v1 (chunk 46) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 46,
"paper_id": "2511.17395v1"
} | science | WO-ARX-01 | 2025-12-09T19:50:16.202843Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_195402770094 | Anisotropy of initially cold ions in magnetized plasma is observed, with Ti⊥/Ti∥ exceeding marginal stability condition κ = 1 in some regions. | Anisotropy of initially cold ions in magnetized plasma is observed, with Ti⊥/Ti∥ exceeding marginal stability condition κ = 1 in some regions. | [
"PIC-HC simulation data",
"Anisotropy computed at time t = 120 ω−1ci",
"Adiabaticity parameter κ ≤ 1 for larger anisotropy"
] | 0.85 | medium | universal | physics | arxiv | 2511.18956v1 | https://arxiv.org/abs/2511.18956v1 | [
"physics.plasm-ph"
] | 3cfcd692bf8378403115fc1bf38aa91822af1e62d7c89131733e0f84dc36534d | Extracted from ArXiv paper 2511.18956v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2511.18956v1"
} | science | WO-ARX-01 | 2025-12-09T19:54:02.770094Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_195726026219 | No significant deviations in excited state lifetimes were observed under any cavity conditions studied. | No significant deviations in excited state lifetimes were observed under any cavity conditions studied. | [
"Ce6T/PS thin films measured with ESA and bleach signals",
"Photodegradation occurs within 30 seconds of exposure to pump light",
"Rastering technique used to maintain consistent strong coupling conditions"
] | 0.85 | medium | universal | physics | arxiv | 2511.19786v1 | https://arxiv.org/abs/2511.19786v1 | [
"physics.chem-ph"
] | 3933861b97645aa369173bccf22ffb5f849fb2e04d555ba0e583f0a3c67b9931 | Extracted from ArXiv paper 2511.19786v1 (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": "2511.19786v1"
} | science | WO-ARX-01 | 2025-12-09T19:57:26.026219Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_195732764264 | Internal pressure of the nucleus was measured to be approximately 200 bar, with thermodynamic pressure being larger than the external one. | Internal pressure of the nucleus was measured to be approximately 200 bar, with thermodynamic pressure being larger than the external one. | [
"Young-Laplace equation calculation",
"Number density: 30.5 nm−3",
"Mass density: ~0.91 g/cm3"
] | 0.85 | medium | universal | physics | arxiv | 2511.20129v1 | https://arxiv.org/abs/2511.20129v1 | [
"cond-mat.soft",
"physics.chem-ph"
] | 33104da870b958c9064ffc50452a5206e3437296a83b4af7a04a0527caecfef7 | Extracted from ArXiv paper 2511.20129v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2511.20129v1"
} | science | WO-ARX-01 | 2025-12-09T19:57:32.764264Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_200526996327 | Single-photon detection efficiency of up to 98% achieved at wavelength 1550 nm using superconducting nanowire detectors | Single-photon detection efficiency of up to 98% achieved at wavelength 1550 nm using superconducting nanowire detectors | [
"Superconducting nanowire single-photon detectors",
"System detection efficiency: 98%",
"Wavelength: 1550 nm"
] | 0.85 | high | universal | physics | arxiv | 2511.20868v1 | https://arxiv.org/abs/2511.20868v1 | [
"physics.ins-det",
"cond-mat.supr-con",
"physics.app-ph",
"physics.optics",
"quant-ph"
] | 240c743baa60ec4239df1695c5368c6bd38dba96a2eebe81f734897104c9ad76 | Extracted from ArXiv paper 2511.20868v1 (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": "2511.20868v1"
} | science | WO-ARX-01 | 2025-12-09T20:05:26.996850Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_200513341445 | We report a high-resolution longitudinal study of impurity segregation in a single HPGe crystal grown under realistic detector conditions, extracting impurity concentrations and effective segregation coefficients. | We report a high-resolution longitudinal study of impurity segregation in a single HPGe crystal grown under realistic detector conditions, extracting impurity concentrations and effective segregation coefficients. | [
"HPGe crystal grown at USD using the Czochralski technique",
"37 segments longitudinally sectioned for impurity distribution analysis",
"Hall-effect measurements"
] | 0.85 | high | universal | physics | arxiv | 2511.20879v1 | https://arxiv.org/abs/2511.20879v1 | [
"physics.ins-det",
"physics.app-ph"
] | 7176492b83d19a04b176ef63d18564b610adf7fb0573981f7313ecc17f229552 | Extracted from ArXiv paper 2511.20879v1 (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": "2511.20879v1"
} | science | WO-ARX-01 | 2025-12-09T20:05:13.341445Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_200519888710 | Effective segregation coefficients for B and P in CZ-grown HPGe crystals measured as K(B)eff = 11.41 ± 1.36 and K(P)eff = 0.17 ± 0.07 | Effective segregation coefficients for B and P in CZ-grown HPGe crystals measured as K(B)eff = 11.41 ± 1.36 and K(P)eff = 0.17 ± 0.07 | [
"Hall-effect measurements at 77 K",
"Impurity-distribution formalism",
"PTIS performed at 7 K"
] | 0.85 | medium | universal | physics | arxiv | 2511.20879v1 | https://arxiv.org/abs/2511.20879v1 | [
"physics.ins-det",
"physics.app-ph"
] | fcac253821c728ff0256e77936e83dc6cdf7b778ee3c49e3fd6d321d97446a2f | Extracted from ArXiv paper 2511.20879v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2511.20879v1"
} | science | WO-ARX-01 | 2025-12-09T20:05:19.888710Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_200529533438 | Effective segregation coefficients for boron, aluminum and gallium in HPGe crystals were measured as 11.41±1.36, 0.67±0.06, and 0.17±0.07, respectively. | Effective segregation coefficients for boron, aluminum and gallium in HPGe crystals were measured as 11.41±1.36, 0.67±0.06, and 0.17±0.07, respectively. | [
"USD Czochralski technique",
"37 segments of detector-grade HPGe crystal analyzed",
"Initial melt concentrations: (4.25 ± 0.06) × 1011 cm−3, (5.47 ± 0.09) × 1012 cm−3, and (3.82 ± 0.65) × 1012 cm−3"
] | 0.85 | medium | universal | physics | arxiv | 2511.20879v1 | https://arxiv.org/abs/2511.20879v1 | [
"physics.ins-det",
"physics.app-ph"
] | 549817a3cb76bf9599d9c5d6c9684a7bf82b19855c4d608a7115712f4967696f | Extracted from ArXiv paper 2511.20879v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2511.20879v1"
} | science | WO-ARX-01 | 2025-12-09T20:05:29.533438Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_200730357187 | Comb states were observed at bias voltages far below the beginning of the NDC region, enabling stable comb generation with RF injection. | Comb states were observed at bias voltages far below the beginning of the NDC region, enabling stable comb generation with RF injection. | [
"Extended Data Fig. 9a and b",
"Bias voltage range: 1.3-2.7 V",
"RF injection frequency: 20 GHz"
] | 0.85 | high | universal | physics | arxiv | 2511.21100v1 | https://arxiv.org/abs/2511.21100v1 | [
"physics.app-ph"
] | 815f74b0e004b336a94236fd4a079d9f1431dfffca45841aba14a9f8c5bc3e58 | Extracted from ArXiv paper 2511.21100v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2511.21100v1"
} | science | WO-ARX-01 | 2025-12-09T20:07:30.357187Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_200811871144 | Cosmic rays with a power-law distribution can amplify magnetic fields up to ∼300µG in the vicinity of supernova remnants, allowing for PeV acceleration and potentially explaining the observed Galactic CR spectrum. | Cosmic rays with a power-law distribution can amplify magnetic fields up to ∼300µG in the vicinity of supernova remnants, allowing for PeV acceleration and potentially explaining the observed Galactic CR spectrum. | [
"Particle-in-cell simulations, typical ISM plasma values (n0 = 1cm−3, BISM = 3µG)",
"CR number density ncr ∼4 × 10−6n0",
"CR energies: p′min ∼1mic ∼GeV/c and p′max ∼106mic ∼PeV/c"
] | 0.85 | high | universal | physics | arxiv | 2511.21154v1 | https://arxiv.org/abs/2511.21154v1 | [
"astro-ph.HE",
"physics.plasm-ph"
] | 0362f83c123ef2479fd3cfda07db25a5eda85293e7d92990128e62e4c8152604 | Extracted from ArXiv paper 2511.21154v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2511.21154v1"
} | science | WO-ARX-01 | 2025-12-09T20:08:11.871144Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_201713790676 | Heisenberg lattices' energy per site is measured with high accuracy by the vDBF method, reaching 0.05% error for a 10x10 lattice. | Heisenberg lattices' energy per site is measured with high accuracy by the vDBF method, reaching 0.05% error for a 10x10 lattice. | [
"vDBF calculations on Heisenberg models",
"Table I: Energy/Site values for Heisenberg models",
"1e-5 threshold, max iter=100, n rots=100"
] | 0.85 | high | universal | physics | arxiv | 2511.21651v1 | https://arxiv.org/abs/2511.21651v1 | [
"quant-ph",
"physics.chem-ph",
"physics.comp-ph"
] | 0c45e263b3f9fb1178876160b712746468722ffceaf6b516f8dbdd825cdd326c | Extracted from ArXiv paper 2511.21651v1 (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": "2511.21651v1"
} | science | WO-ARX-01 | 2025-12-09T20:17:13.791206Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202110847989 | We demonstrate an uncooled thermal detector with a specific detectivity of 1.1×107 Jones and a thermal time constant of 34 µs, exceeding typical high-sensitivity uncooled technologies by an order of magnitude. | We demonstrate an uncooled thermal detector with a specific detectivity of 1.1×107 Jones and a thermal time constant of 34 µs, exceeding typical high-sensitivity uncooled technologies by an order of magnitude. | [
"Heterogeneously integrated pixel with pyrolytic carbon absorbers for broadband LWIR absorption",
"Silicon photonic crystal cavity as a high-Q optical thermometer",
"Operating at ambient temperature and pressure"
] | 0.85 | high | universal | physics | arxiv | 2511.22006v1 | https://arxiv.org/abs/2511.22006v1 | [
"physics.app-ph",
"physics.optics"
] | 902630c75e53775efd1d1667498f127a87526ecf2684b7e4c64620c482e3cc6e | Extracted from ArXiv paper 2511.22006v1 (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": "2511.22006v1"
} | science | WO-ARX-01 | 2025-12-09T20:21:10.847989Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202157247876 | The photothermal responsivity of the PhC bolometer was measured with a direct reflection path, and the resonance wavelength was extracted from each spectrum by fitting to a Lorentzian lineshape. | The photothermal responsivity of the PhC bolometer was measured with a direct reflection path, and the resonance wavelength was extracted from each spectrum by fitting to a Lorentzian lineshape. | [
"IR camera (Xenics Cheetah 640)",
"405 nm laser power varied in a randomized sequence",
"Measurements repeated three times for statistical robustness"
] | 0.85 | medium | universal | physics | arxiv | 2511.22006v1 | https://arxiv.org/abs/2511.22006v1 | [
"physics.app-ph",
"physics.optics"
] | 644c57e13de46e37e178b0cf61ca88c3933085d19370e7b4e6daaabd84367026 | Extracted from ArXiv paper 2511.22006v1 (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": "2511.22006v1"
} | science | WO-ARX-01 | 2025-12-09T20:21:57.247876Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202152138308 | A rigorous adiabatic approach is developed for ultracold atom-molecule collisions in a magnetic field, providing accurate cross sections with ≃2 times fewer channels than the standard diabatic basis. | A rigorous adiabatic approach is developed for ultracold atom-molecule collisions in a magnetic field, providing accurate cross sections with ≃2 times fewer channels than the standard diabatic basis. | [
"adiabatic coupled-channel formalism",
"Mg (1S) + NH (3Σ−) collisions",
"≃2 times fewer channels"
] | 0.85 | medium | universal | physics | arxiv | 2511.22045v1 | https://arxiv.org/abs/2511.22045v1 | [
"physics.chem-ph"
] | 20d0fb10815ea7ad2673a2d3c2c796d663c39a36dcc588f58d978d44e4a51f59 | Extracted from ArXiv paper 2511.22045v1 (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": "2511.22045v1"
} | science | WO-ARX-01 | 2025-12-09T20:21:52.138308Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202218620168 | Adiabatic coupled-channel calculations for ultracold Mg + NH collisions in a magnetic field yield cross sections | Adiabatic coupled-channel calculations for ultracold Mg + NH collisions in a magnetic field yield cross sections | [
"adiabatic approach",
"ultracold Mg + NH collisions",
"magnetic field"
] | 0.85 | medium | universal | physics | arxiv | 2511.22045v1 | https://arxiv.org/abs/2511.22045v1 | [
"physics.chem-ph"
] | eb49b7598a8ef14e397231dcc59a9cad7e71e0ed675d3c42999ec41dabf7c492 | Extracted from ArXiv paper 2511.22045v1 (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": "2511.22045v1"
} | science | WO-ARX-01 | 2025-12-09T20:22:18.620168Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202227175613 | Adiabatic basis produces cross sections with less error and provides high-quality approximate results with much fewer basis functions compared to the standard diabatic basis. | Adiabatic basis produces cross sections with less error and provides high-quality approximate results with much fewer basis functions compared to the standard diabatic basis. | [
"adiabatic treatment, Fig. 6",
"constant propagation basis size",
"ratio of calculated to benchmark inelastic cross sections"
] | 0.85 | medium | universal | physics | arxiv | 2511.22045v1 | https://arxiv.org/abs/2511.22045v1 | [
"physics.chem-ph"
] | ec23b37933db4455114846da659211160cde5535c84a36e51e174f50a0347518 | Extracted from ArXiv paper 2511.22045v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 10,
"paper_id": "2511.22045v1"
} | science | WO-ARX-01 | 2025-12-09T20:22:27.176134Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202243843583 | Polarization contrasts in signal intensities are measured with <5% residual deviations using numerical optimization procedure | Polarization contrasts in signal intensities are measured with <5% residual deviations using numerical optimization procedure | [
"Numerical optimization approach for polarization-resolved intensity measurements",
"2D grid search over field amplitudes and phase differences",
" Quarter-wave plate angles: θqwp = 0° and 45°"
] | 0.85 | medium | universal | physics | arxiv | 2511.22060v1 | https://arxiv.org/abs/2511.22060v1 | [
"quant-ph",
"physics.chem-ph"
] | cb5e6cb30056dcbd483ac07d633ffee0c0607f40a34e485244c104cb92e90314 | Extracted from ArXiv paper 2511.22060v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2511.22060v1"
} | science | WO-ARX-01 | 2025-12-09T20:22:43.843583Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202602133997 | We observed two isolated single-photon emitting defects, identified as a V2 center and a V1 center in silicon carbide, with characteristic zero-field resonance frequencies. | We observed two isolated single-photon emitting defects, identified as a V2 center and a V1 center in silicon carbide, with characteristic zero-field resonance frequencies. | [
"Home-built confocal laser-scanning microscope equipped with an oil-immersion objective lens (NA = 1.45)",
"Fluorescence image between electrodes under 730 nm laser at 70 μW",
"Autocorrelation functions and ODMR spectra of defects X and Y"
] | 0.85 | medium | universal | physics | arxiv | 2511.22449v1 | https://arxiv.org/abs/2511.22449v1 | [
"cond-mat.mes-hall",
"physics.app-ph"
] | 59cd3ac23790837f8a7a19ad586f92c7fdb24aa9d0f0f238451cfa2384ef9628 | Extracted from ArXiv paper 2511.22449v1 (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": "2511.22449v1"
} | science | WO-ARX-01 | 2025-12-09T20:26:02.133997Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202731654951 | The effective capacitance at the electrode-electrolyte interface was measured with an uncertainty of less than 1 × 10−2 Ha, reproducing surface charge distribution from higher-level quantum-mechanical calculations within statistical uncertainty. | The effective capacitance at the electrode-electrolyte interface was measured with an uncertainty of less than 1 × 10−2 Ha, reproducing surface charge distribution from higher-level quantum-mechanical calculations within statistical uncertainty. | [
"Electrochemical impedance spectroscopy (EIS) on highly oriented pyrolytic graphite (HOPG)",
"Frequency range: 20 kHz–1 Hz",
"7 mV rms amplitude"
] | 0.85 | medium | universal | physics | arxiv | 2511.22540v1 | https://arxiv.org/abs/2511.22540v1 | [
"physics.chem-ph"
] | 5bbb50c0abdf90c7e1941b79ece7b60486a7e105f5acb302182120372159ff88 | Extracted from ArXiv paper 2511.22540v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2511.22540v1"
} | science | WO-ARX-01 | 2025-12-09T20:27:31.654951Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_202908906026 | A machine-learning force field is developed to model an excess electron in solution, enabling the simulation of its reaction with a hydronium ion and reproducing experimentally measured reaction rates and free energies. | A machine-learning force field is developed to model an excess electron in solution, enabling the simulation of its reaction with a hydronium ion and reproducing experimentally measured reaction rates and free energies. | [
"Density functional theory calculation",
"Bulk water simulations",
"Experimental measurements"
] | 0.85 | medium | universal | physics | arxiv | 2511.22642v1 | https://arxiv.org/abs/2511.22642v1 | [
"physics.chem-ph",
"physics.comp-ph"
] | 6a163371e3115f1554453254b4462eea7c0beea2f1a403918513e3ad2ee02fdd | Extracted from ArXiv paper 2511.22642v1 (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": "2511.22642v1"
} | science | WO-ARX-01 | 2025-12-09T20:29:08.906026Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_203600371166 | A modified Paschen's Law equation (eq. 3.1) accurately fits the measured breakdown voltage data for various electrode configurations and gap distances. | A modified Paschen's Law equation (eq. 3.1) accurately fits the measured breakdown voltage data for various electrode configurations and gap distances. | [
"Experimental setup with symmetric and asymmetric electrode configurations",
"Breakdown voltage data at different inter-electrode gaps (d=2cm to d=30cm)",
"Modified Paschen relation parameters: B∗, C∗, k, m"
] | 0.85 | high | universal | physics | arxiv | 2511.23108v1 | https://arxiv.org/abs/2511.23108v1 | [
"physics.plasm-ph",
"physics.atom-ph",
"physics.pop-ph"
] | 0111868d1e088bdfbc4044565fcfb66f3f371e3aaf8c50b2955de82a05d439d1 | Extracted from ArXiv paper 2511.23108v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2511.23108v1"
} | science | WO-ARX-01 | 2025-12-09T20:36:00.371166Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_203607557828 | Efficiencies for Higgs boson decays into various final states are measured to be around 50-63% at √s = 240 GeV, and 32-54% at √s = 365 GeV | Efficiencies for Higgs boson decays into various final states are measured to be around 50-63% at √s = 240 GeV, and 32-54% at √s = 365 GeV | [
"delphes simulation of FCC-ee collisions",
"10.8 ab^-1 integrated luminosity at √s = 240 GeV",
"3.12 ab^-1 integrated luminosity at √s = 365 GeV"
] | 0.85 | medium | universal | physics | arxiv | 2511.23149v1 | https://arxiv.org/abs/2511.23149v1 | [
"hep-ex",
"physics.app-ph",
"physics.data-an"
] | a7f358736d25d5abdd5b0a6cee578c478efb87a9560ad8b7859f660bf5694504 | Extracted from ArXiv paper 2511.23149v1 (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": "2511.23149v1"
} | science | WO-ARX-01 | 2025-12-09T20:36:07.557828Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_203917426949 | The nonlinearity parameter for the edge mode of a nano-disk was measured as λ̃ = -7.229 × 10^-13 GHz A^-2 m^2, with a strong nonlinear frequency shift achieved at modest excitation field amplitudes (B0 ≤ 0.6 mT). | The nonlinearity parameter for the edge mode of a nano-disk was measured as λ̃ = -7.229 × 10^-13 GHz A^-2 m^2, with a strong nonlinear frequency shift achieved at modest excitation field amplitudes (B0 ≤ 0.6 mT). | [
"micromagnetic simulations",
"edge mode's resonance frequency shown as a function of B0 in Fig. 2 (b)",
"nonlinearity parameter extracted from fitting simulated results to Eq. (4)"
] | 0.85 | high | universal | physics | arxiv | 2512.00199v1 | https://arxiv.org/abs/2512.00199v1 | [
"physics.app-ph",
"cond-mat.mes-hall"
] | d74a150d592ecdb45b805738998074a717e1882569b78823f8b0c4267e5cc782 | Extracted from ArXiv paper 2512.00199v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.00199v1"
} | science | WO-ARX-01 | 2025-12-09T20:39:17.427471Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_204129586330 | Runaway electron current and collision time with plasma-facing components observed in Damavand Tokamak at different magnetic field strengths | Runaway electron current and collision time with plasma-facing components observed in Damavand Tokamak at different magnetic field strengths | [
"Damavand Tokamak device, NaI detectors",
"Hard X-ray energy range: 0.2 MeV to 3 MeV",
"Toroidal magnetic field strength: 0.8 T and 1.1 T"
] | 0.85 | high | universal | physics | arxiv | 2512.00530v1 | https://arxiv.org/abs/2512.00530v1 | [
"physics.plasm-ph"
] | 69129087ced4cf17ef6eee08b3492236a2c30058881c4a25425497f6bd958e6d | Extracted from ArXiv paper 2512.00530v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2512.00530v1"
} | science | WO-ARX-01 | 2025-12-09T20:41:29.586330Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_204116795992 | Electron temperature and density were measured in argon dc glow discharge plasma, with peak values of Te=49 eV and ne=1.46×10^16 m^-3 at 500 V. | Electron temperature and density were measured in argon dc glow discharge plasma, with peak values of Te=49 eV and ne=1.46×10^16 m^-3 at 500 V. | [
"COMSOL Multiphysics simulation",
"argon plasma chamber (23 cm diameter × 40 cm height)",
"discharge voltage: 500 V"
] | 0.85 | medium | universal | physics | arxiv | 2512.00533v1 | https://arxiv.org/abs/2512.00533v1 | [
"physics.plasm-ph"
] | dbd89e18b7eb91d64dc698020c38d3b0b433abcdea73a2b0186853211e4249cf | Extracted from ArXiv paper 2512.00533v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2512.00533v1"
} | science | WO-ARX-01 | 2025-12-09T20:41:16.795992Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_204126466541 | The ion temperature was measured to be 3.5 eV and 4 eV for discharge voltages of 500 V and 600 V, respectively. | The ion temperature was measured to be 3.5 eV and 4 eV for discharge voltages of 500 V and 600 V, respectively. | [
"Experimental EDFs from argon gas at 5.33 Pa",
"I-V curve with a potential difference of 500 V",
"First peak fitted to Druyveteyn EDF"
] | 0.85 | medium | universal | physics | arxiv | 2512.00533v1 | https://arxiv.org/abs/2512.00533v1 | [
"physics.plasm-ph"
] | 0e73ac2afbbcd5bb8a42c9807cd9ad16a805539e9d22136ddc4b7f90ed2d391b | Extracted from ArXiv paper 2512.00533v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2512.00533v1"
} | science | WO-ARX-01 | 2025-12-09T20:41:26.467068Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_204335762009 | Interlayer spacing in van der Waals layered ErOCl nanosheets measured to be 0.88 nm, consistent with theoretical interlayer distances | Interlayer spacing in van der Waals layered ErOCl nanosheets measured to be 0.88 nm, consistent with theoretical interlayer distances | [
"HRTEM imaging (Fig. 1e)",
"Monolayer thickness: ~ 0.9 nm from AFM profiling",
"Consistent with theoretical interlayer distances"
] | 0.85 | medium | universal | physics | arxiv | 2512.00731v1 | https://arxiv.org/abs/2512.00731v1 | [
"physics.app-ph",
"cond-mat.mtrl-sci"
] | 41d9eacffd920ac11923be964fd7bbda3feb575c9a61e96b80aaf87900fa4c23 | Extracted from ArXiv paper 2512.00731v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.00731v1"
} | science | WO-ARX-01 | 2025-12-09T20:43:35.762009Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_205546876299 | Electron acceleration to GeV-level kinetic energies observed via DLA in radially polarized laser-plasma interaction, with improved collimation in RP f/5 configuration | Electron acceleration to GeV-level kinetic energies observed via DLA in radially polarized laser-plasma interaction, with improved collimation in RP f/5 configuration | [
"PIC simulation",
"electron density ramp within the plasma channel",
"laser energy and power fixed at approximately 1 kJ and 6.7 PW"
] | 0.85 | high | universal | physics | arxiv | 2512.01737v1 | https://arxiv.org/abs/2512.01737v1 | [
"physics.plasm-ph"
] | 3ade42a510b4aa270f884cde3ee5305f53ec06e23b131144e5bec4dfb3a7f38b | Extracted from ArXiv paper 2512.01737v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2512.01737v1"
} | science | WO-ARX-01 | 2025-12-09T20:55:46.876299Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_205603462666 | Rapid and complete broadening of ion velocity distribution function is observed in ultra-low-beta plasmas under parametric decay instability, triggering bidirectional ion acceleration. | Rapid and complete broadening of ion velocity distribution function is observed in ultra-low-beta plasmas under parametric decay instability, triggering bidirectional ion acceleration. | [
"Hybrid particle-in-cell simulations",
"Plasma beta and pump-wave amplitude dependence studied",
"Realistic ionospheric conditions modeled"
] | 0.85 | high | universal | physics | arxiv | 2512.01757v1 | https://arxiv.org/abs/2512.01757v1 | [
"physics.plasm-ph"
] | 28ce55b0b769072fe98c2600c98acad660b6ff3c39ac0344933ccb03c83355db | Extracted from ArXiv paper 2512.01757v1 (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": "2512.01757v1"
} | science | WO-ARX-01 | 2025-12-09T20:56:03.462666Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_205705677399 | Plasma instability introduces nonthermal effects and drives the plasma away from its initial Maxwellian state, with observed parallel ion heating. | Plasma instability introduces nonthermal effects and drives the plasma away from its initial Maxwellian state, with observed parallel ion heating. | [
"Hybrid simulation of ultra-low-beta plasmas",
"Perturbation by small-amplitude Alfvén waves",
"Temporal evolution of ion VDF (velocity distribution function)"
] | 0.85 | high | universal | physics | arxiv | 2512.01757v1 | https://arxiv.org/abs/2512.01757v1 | [
"physics.plasm-ph"
] | 7f2d904aeb09e4e85961db259324771b9ccc50bab63b189ff6a5b2e0f6e58297 | Extracted from ArXiv paper 2512.01757v1 (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": "2512.01757v1"
} | science | WO-ARX-01 | 2025-12-09T20:57:05.677399Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_205756724112 | The experimental value of the alpha parameter in the Standard Model is measured to be $-0.0078^{+0.0005}_{-0.0006}$ | The experimental value of the alpha parameter in the Standard Model is measured to be $-0.0078^{+0.0005}_{-0.0006}$ | [
"CMS experiment, LHC data at 13 TeV center-of-mass energy",
"Integrated luminosity: 137 fb^-1",
"Systematic uncertainty: 0.0013"
] | 0.85 | high | universal | physics | arxiv | 2512.01780v1 | https://arxiv.org/abs/2512.01780v1 | [
"physics.plasm-ph"
] | 62d938fe86e1dce01812e887a299254a130b09c05b1fb54cc906f87ab9cb7941 | Extracted from ArXiv paper 2512.01780v1 (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": "2512.01780v1"
} | science | WO-ARX-01 | 2025-12-09T20:57:56.724112Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_210135392361 | A weak but persistent jet is observed in the simulation with a coherence parameter CBH of ∼0.9 and non-negligible Poynting flux. | A weak but persistent jet is observed in the simulation with a coherence parameter CBH of ∼0.9 and non-negligible Poynting flux. | [
"Simulations using 3DSS-9375 setup",
"Magnetic field coherence parameter: CBH = ∼0.9",
"Poynting flux at r = 50 M: non-zero"
] | 0.85 | medium | universal | physics | arxiv | 2512.02129v1 | https://arxiv.org/abs/2512.02129v1 | [
"astro-ph.HE",
"physics.plasm-ph"
] | b95b6a773f12d5c3a787c691c81191d479df988fe2d8bd69d0b8a8c845d0c66b | Extracted from ArXiv paper 2512.02129v1 (chunk 21) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 21,
"paper_id": "2512.02129v1"
} | science | WO-ARX-01 | 2025-12-09T21:01:35.392361Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_210414248187 | Nanopore conductance measured with ohmic behavior in phosphate-buffered saline, yielding a slope of 0.5 μS. | Nanopore conductance measured with ohmic behavior in phosphate-buffered saline, yielding a slope of 0.5 μS. | [
"Au layer acting as a floating electrode",
"Phosphate-buffered saline containing 1.37 M NaCl at pH 7.4",
"Current from the nanopore applying a transmembrane voltage"
] | 0.85 | medium | universal | physics | arxiv | 2512.02500v1 | https://arxiv.org/abs/2512.02500v1 | [
"physics.app-ph",
"physics.optics"
] | 6f92ed80543d759b29a61fd4fef32fbb460f760dfb43917a6045dd54500da0a6 | Extracted from ArXiv paper 2512.02500v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2512.02500v1"
} | science | WO-ARX-01 | 2025-12-09T21:04:14.248187Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_210649722347 | A transition from J-aggregate to H-aggregate emission is observed in ZnPc crystals as temperature increases, with the latter dominating at high temperatures and the former at low temperatures. | A transition from J-aggregate to H-aggregate emission is observed in ZnPc crystals as temperature increases, with the latter dominating at high temperatures and the former at low temperatures. | [
"ZnPc (¯101) crystal facet, measured PL spectra",
"Temperature-dependent change in emission characteristic",
"H-aggregate emission modeled by a Bose-Einstein phonon population"
] | 0.85 | high | universal | physics | arxiv | 2512.02639v1 | https://arxiv.org/abs/2512.02639v1 | [
"cond-mat.mtrl-sci",
"physics.chem-ph"
] | c28ce73d079bee841e49585a72f2284fa3b2f4412b44928ca8665e8034a7b1e8 | Extracted from ArXiv paper 2512.02639v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.02639v1"
} | science | WO-ARX-01 | 2025-12-09T21:06:49.722347Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_210659983480 | Radiative lifetimes of ZnPc facets differ due to anisotropic optical and structural properties, with faster decay observed for the (¯101) facet at room temperature. | Radiative lifetimes of ZnPc facets differ due to anisotropic optical and structural properties, with faster decay observed for the (¯101) facet at room temperature. | [
"ZnPc single crystal experiment",
"Multi-exponential fitting of spectrum around 1.6 eV",
"Radiative lifetimes: 250 ps (360 ps) at room temperature for (¯101) and (223) facets, respectively"
] | 0.85 | medium | universal | physics | arxiv | 2512.02639v1 | https://arxiv.org/abs/2512.02639v1 | [
"cond-mat.mtrl-sci",
"physics.chem-ph"
] | d1b3c68b2d72e8ea02d3cf3ad6772c61c5c862396ef0a72e0c0e485b225310fe | Extracted from ArXiv paper 2512.02639v1 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2512.02639v1"
} | science | WO-ARX-01 | 2025-12-09T21:06:59.983480Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_210735444167 | The relative sensitivity of peak wavelength to temperature in monolayer WS2 is measured as 0.02% to 0.023% K^-1 from ambient temperature to 160°C (433 K) | The relative sensitivity of peak wavelength to temperature in monolayer WS2 is measured as 0.02% to 0.023% K^-1 from ambient temperature to 160°C (433 K) | [
"Raman spectra of monolayer WS2 on a PDMS substrate, measured with 532 nm excitation",
"Peak wavelength shift follows the Varshni equation",
"Integrated PL intensity vs temperature plot"
] | 0.85 | medium | universal | physics | arxiv | 2512.02754v1 | https://arxiv.org/abs/2512.02754v1 | [
"cond-mat.mtrl-sci",
"physics.atom-ph"
] | 581a354205277e451a9997f8afe29570b60e1e261cea2e9fdf9cb6b940796691 | Extracted from ArXiv paper 2512.02754v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.02754v1"
} | science | WO-ARX-01 | 2025-12-09T21:07:35.444167Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_210816445140 | Transient effects in total internal reflection of a bounded pulse were observed and the spatial Goos-Hanchen shift was recovered using QLA simulations | Transient effects in total internal reflection of a bounded pulse were observed and the spatial Goos-Hanchen shift was recovered using QLA simulations | [
"QLA simulations with total energy conserved to at least 7 significant figures",
"Angle of incidence θ = 25o < critical angle θc",
"Bounded pulse with finite width interacting with dielectric interface"
] | 0.85 | medium | universal | physics | arxiv | 2512.02856v1 | https://arxiv.org/abs/2512.02856v1 | [
"physics.plasm-ph"
] | e1a2c07be388011e54d7b9293d5e779f5d3bfe1f2f32a21880253fc556580315 | Extracted from ArXiv paper 2512.02856v1 (chunk 1) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 1,
"paper_id": "2512.02856v1"
} | science | WO-ARX-01 | 2025-12-09T21:08:16.445140Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_211031579437 | The evaporation rate of a silica slurry is enhanced by replanting the evaporator setup to different locations, with a maximum increase of 40% observed at high solid concentrations | The evaporation rate of a silica slurry is enhanced by replanting the evaporator setup to different locations, with a maximum increase of 40% observed at high solid concentrations | [
"Sailboat evaporator setup",
"Wind velocity: 4 m/s",
"Silica slurry concentrations: up to 75 wt%"
] | 0.85 | medium | universal | physics | arxiv | 2512.02939v1 | https://arxiv.org/abs/2512.02939v1 | [
"physics.app-ph"
] | e8f8b40aba320858d01f0d5b8115961d0614463b0c0336cc8ea78f6536be327e | Extracted from ArXiv paper 2512.02939v1 (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": "2512.02939v1"
} | science | WO-ARX-01 | 2025-12-09T21:10:31.579437Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_211045962297 | An average mass loss rate of 41 g/h is observed during the first cycle of evaporation, with sustained performance throughout subsequent cycles due to suspension flushing. | An average mass loss rate of 41 g/h is observed during the first cycle of evaporation, with sustained performance throughout subsequent cycles due to suspension flushing. | [
"30 wt% tailing wastewater",
"Wind velocity: 4 m/s",
"Mass loss rate: 41 g/h"
] | 0.85 | medium | universal | physics | arxiv | 2512.02939v1 | https://arxiv.org/abs/2512.02939v1 | [
"physics.app-ph"
] | 95c2994aef93b655ca2e95be2fc00550201cfaac23304d09e336e2cd5b179810 | Extracted from ArXiv paper 2512.02939v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 8,
"paper_id": "2512.02939v1"
} | science | WO-ARX-01 | 2025-12-09T21:10:45.962825Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_211500093085 | The secondary electrostatic instability occurs when ωr < −m∗ω0, as observed from Eq. (14) and Eq. (16). | The secondary electrostatic instability occurs when ωr < −m∗ω0, as observed from Eq. (14) and Eq. (16). | [
"Eq. (14)",
"Eq. (16)",
"oblique whistler modes, ECDI-like modes"
] | 0.85 | high | universal | physics | arxiv | 2512.03269v1 | https://arxiv.org/abs/2512.03269v1 | [
"physics.plasm-ph",
"physics.comp-ph",
"physics.space-ph"
] | 88ea747da3f28256e6826e4ef5b2440c77929cee8e270b9e23103c2046013a11 | Extracted from ArXiv paper 2512.03269v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2512.03269v1"
} | science | WO-ARX-01 | 2025-12-09T21:15:00.093085Z | arxiv | physics_recovered | arxiv_physics |
w_20251209_211614783966 | Simulated STEM images show substantial changes in measured electrostatic field configurations due to defocus and aberrations, with an underfocused probe affecting spatial distributions. | Simulated STEM images show substantial changes in measured electrostatic field configurations due to defocus and aberrations, with an underfocused probe affecting spatial distributions. | [
"Multislice image simulations using Dr. Probe software",
"Accelerating voltage: 80 kV",
"Effective source size: 70 pm at FWHM"
] | 0.85 | medium | universal | physics | arxiv | 2512.03372v1 | https://arxiv.org/abs/2512.03372v1 | [
"cond-mat.mtrl-sci",
"physics.app-ph"
] | 4b5ead3cc041742ca3ba299b85c86331f94bf553eeb1022df4d5e790e5f16129 | Extracted from ArXiv paper 2512.03372v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2512.03372v1"
} | science | WO-ARX-01 | 2025-12-09T21:16:14.783966Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100818480973 | Theoretical calculations of atomic hydrogen and tritium scattering cross sections have been performed, with total uncertainties ranging from 7.6% to 26% for different channels. | Theoretical calculations of atomic hydrogen and tritium scattering cross sections have been performed, with total uncertainties ranging from 7.6% to 26% for different channels. | [
"New calculations of cross sections and rate constants for atomic hydrogen and tritium scattering",
"Approximate systematic uncertainties tabulated in Table II"
] | 0.85 | medium | universal | physics | arxiv | 2509.13426v1 | https://arxiv.org/abs/2509.13426v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | b9377c18060ee912a397252a685c72c05868e406da49fc0cade1eadfd80d7406 | Extracted from ArXiv paper 2509.13426v1 (chunk 12) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 12,
"paper_id": "2509.13426v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:18.480973Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100806778346 | Photoionization cross-section from the 3s3p1p excited state of magnesium measured to be 10^(-18) cm^2 | Photoionization cross-section from the 3s3p1p excited state of magnesium measured to be 10^(-18) cm^2 | [
"Journal of Physics B: Atomic, Molecular and Optical Physics, measurement by Rafiq et al. (2007)",
"Cross-sectional area: 6.32 × 10^(-19) Å^2"
] | 0.85 | medium | universal | physics | arxiv | 2509.13619v1 | https://arxiv.org/abs/2509.13619v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 94e482e13e69d338a88361f7b8284325c987e7d3061f7bfb5f4ec6aae7678995 | Extracted from ArXiv paper 2509.13619v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2509.13619v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:06.778868Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100804259621 | Axial and radial temperature of strontium atoms in the lattice trap measured to be 3.2(1) μK and 2.5(2) μK, respectively | Axial and radial temperature of strontium atoms in the lattice trap measured to be 3.2(1) μK and 2.5(2) μK, respectively | [
"Lattice depths up to 807 Er",
"Axial sideband cooling, radial Doppler cooling, and 32 Er energy filtering"
] | 0.85 | medium | universal | physics | arxiv | 2509.13991v1 | https://arxiv.org/abs/2509.13991v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 16fdeaa972181422ea1e1a9291abf6017ce7e175e70fb76272952812b9eae491 | Extracted from ArXiv paper 2509.13991v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2509.13991v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:04.259621Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100843516117 | Background gas collision frequency shift on lattice-trapped strontium atoms measured with 0.5 Hz uncertainty | Background gas collision frequency shift on lattice-trapped strontium atoms measured with 0.5 Hz uncertainty | [
"Optical lattice clock experiment, strontium atoms confined in shallow trap",
"Frequency modulation spectroscopy technique used"
] | 0.85 | medium | universal | physics | arxiv | 2509.13991v1 | https://arxiv.org/abs/2509.13991v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | bc07f038351d839e2cd85e823fcc4c05a9865bcf1469fc304a7652fc22d6928b | Extracted from ArXiv paper 2509.13991v1 (chunk 15) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2509.13991v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:43.516117Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100819750946 | The instability of the comparison between Sr1 and Sr3 clocks is measured to be 2.8 × 10−16/√𝜏 for averaging time from 4,000 to 20,000 s | The instability of the comparison between Sr1 and Sr3 clocks is measured to be 2.8 × 10−16/√𝜏 for averaging time from 4,000 to 20,000 s | [
"Optical lattice clock comparison",
"Ramsey spectroscopy with 25-ms 𝜋/2-pulses and 500-ms free evolution period"
] | 0.85 | high | universal | physics | arxiv | 2509.15100v1 | https://arxiv.org/abs/2509.15100v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 035350d9c345f25f1d891306b48f5ff229800d975a0f736cdc579143555952e5 | Extracted from ArXiv paper 2509.15100v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2509.15100v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:19.750946Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100828263731 | The sensitivity of the EIT-based detection method is measured to be 3.7 µVm−1Hz−1/2 at optimal coupling and probe Rabi frequencies. | The sensitivity of the EIT-based detection method is measured to be 3.7 µVm−1Hz−1/2 at optimal coupling and probe Rabi frequencies. | [
"Atom-based mixer approach with beat note at 10 kHz generated and detected by a spectrum analyzer",
"Optimal LO power: 10 kHz beat note amplitude reaches its maximum"
] | 0.85 | medium | universal | physics | arxiv | 2509.15463v1 | https://arxiv.org/abs/2509.15463v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 919f07eaa0b9bb836a0cdc33e82a80b05b95b5bf51dea5246912897b52dc4078 | Extracted from ArXiv paper 2509.15463v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2509.15463v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:28.263731Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100828760312 | A novel gravitational wave detector concept using ultrastable optical cavities is proposed, enabling detection of GW signals in the 10^-5 - 1 Hz frequency band. | A novel gravitational wave detector concept using ultrastable optical cavities is proposed, enabling detection of GW signals in the 10^-5 - 1 Hz frequency band. | [
"Optical atomic clocks",
"Terrestrial technology with current capabilities"
] | 0.85 | high | universal | physics | arxiv | 2509.15841v2 | https://arxiv.org/abs/2509.15841v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 734d7f48a0e409c07efe0abbea75f76c347ab62b958e1408373a3298fdedce71 | Extracted from ArXiv paper 2509.15841v2 (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": "2509.15841v2"
} | science | WO-ARX-01 | 2025-12-07T10:08:28.760312Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100831858232 | We demonstrate a novel GW detector concept based on monolithic optical cavities with sufficient sensitivity to search for GWs in the mid-band. | We demonstrate a novel GW detector concept based on monolithic optical cavities with sufficient sensitivity to search for GWs in the mid-band. | [
"Optical Fabry-Perot cavities, state-of-the-art technology",
"Fractional frequency instability below 10^-16 achieved"
] | 0.85 | high | universal | physics | arxiv | 2509.15841v2 | https://arxiv.org/abs/2509.15841v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 9c8cca1491df60e2eb390ed3d54f0422bb829c86de690b8fb18e833e1e2b8cfd | Extracted from ArXiv paper 2509.15841v2 (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": "2509.15841v2"
} | science | WO-ARX-01 | 2025-12-07T10:08:31.858232Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100841558266 | GW strain can be measured by measuring ∆φ/φ = h(t)∆L/2L between the light that exits the cavity and a reference | GW strain can be measured by measuring ∆φ/φ = h(t)∆L/2L between the light that exits the cavity and a reference | [
"High finesse optical cavity, photon reflection and round trip",
"Cavity enhancement for L ≃ tens of km within a detector of only l ≤1 m"
] | 0.85 | high | universal | physics | arxiv | 2509.15841v2 | https://arxiv.org/abs/2509.15841v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | f8f65ad4cf133fe443016f03b484e7479991ada00d3f973346e1eec7d5859850 | Extracted from ArXiv paper 2509.15841v2 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2509.15841v2"
} | science | WO-ARX-01 | 2025-12-07T10:08:41.558266Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100851584098 | Overtone spectrum of H3O+ ions measured and simulated at 20 K and 125 K, with 77 transitions assigned to two overtone bands. | Overtone spectrum of H3O+ ions measured and simulated at 20 K and 125 K, with 77 transitions assigned to two overtone bands. | [
"Experimental setup: trap chamber temperature set to 20 K; simulated spectra compared at 20 K and 35 K",
"Measuring range: 6750-6950 cm−1; 85 transitions measured; 68 included for fitting procedures"
] | 0.85 | medium | universal | physics | arxiv | 2509.16009v1 | https://arxiv.org/abs/2509.16009v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 5e351bf3826e77134d2ad0c9b737bf81e7049956ab2cad3d4625261002ab9e48 | Extracted from ArXiv paper 2509.16009v1 (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": "2509.16009v1"
} | science | WO-ARX-01 | 2025-12-07T10:08:51.584098Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100926489540 | Breathing-like dynamics observed in a lattice site with near-unity population at specific acceleration durations, leading to quasi-monochromatic output | Breathing-like dynamics observed in a lattice site with near-unity population at specific acceleration durations, leading to quasi-monochromatic output | [
"Numerical simulation of the Gross-Pitaevskii equation",
"Acceleration durations: 973.2 μs and 976.6 μs"
] | 0.85 | high | universal | physics | arxiv | 2509.16367v1 | https://arxiv.org/abs/2509.16367v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 6f681e7f888346623f369e7a7af0ea9230283e46c3bdfc93ad4c4b9b79420500 | Extracted from ArXiv paper 2509.16367v1 (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": "2509.16367v1"
} | science | WO-ARX-01 | 2025-12-07T10:09:26.489540Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100929991880 | Excellent agreement observed between variational model and full Gross-Pitaevskii equation during loading and acceleration phases, but discrepancies emerge in the release stage. | Excellent agreement observed between variational model and full Gross-Pitaevskii equation during loading and acceleration phases, but discrepancies emerge in the release stage. | [
"Comparison of Schrödinger equation and Gross-Pitaevskii equation simulations",
"Spatial width ∆x(t) (FWHM) measurement with two models at tL = 100 µs and tacc = 976.6 µs"
] | 0.85 | medium | universal | physics | arxiv | 2509.16367v1 | https://arxiv.org/abs/2509.16367v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 6f28ed5a0a31cc5776903f6b23baf69913271c24c3834decf2b3af156fd321f9 | Extracted from ArXiv paper 2509.16367v1 (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": "2509.16367v1"
} | science | WO-ARX-01 | 2025-12-07T10:09:29.991880Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_100951386937 | The n-excitation scattering cross section is expressed in terms of integrals over lattice momenta, with all transverse wavenumber integrals evaluated analytically. | The n-excitation scattering cross section is expressed in terms of integrals over lattice momenta, with all transverse wavenumber integrals evaluated analytically. | [
"Lattice arrays",
"Connected T-matrix elements"
] | 0.85 | medium | universal | physics | arxiv | 2509.17148v1 | https://arxiv.org/abs/2509.17148v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 6669c9ed01590dcfb18b91cbeb976f4275525cc5a4e7a9cf32dbae18c7cc2b08 | Extracted from ArXiv paper 2509.17148v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2509.17148v1"
} | science | WO-ARX-01 | 2025-12-07T10:09:51.386937Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101001263817 | A momentum-independent atomic T-matrix is derived for two-level nonlinearities, simplifying the calculation of the S-matrix and scattering cross sections. | A momentum-independent atomic T-matrix is derived for two-level nonlinearities, simplifying the calculation of the S-matrix and scattering cross sections. | [
"Theoretical derivation in Appendix E",
"Restrictions due to energy and momentum conservation"
] | 0.85 | medium | universal | physics | arxiv | 2509.17148v1 | https://arxiv.org/abs/2509.17148v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d28c161f06d51ddb68a44e189a80ddb4b5ebb1e14d22d6cad57624830bbb3e05 | Extracted from ArXiv paper 2509.17148v1 (chunk 13) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2509.17148v1"
} | science | WO-ARX-01 | 2025-12-07T10:10:01.263817Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101026520806 | Bell-state fidelity measured as 99.8(1)% for the LS gate and 96(1)% for the clock–Zeeman MS gate, with lower fidelity due to qubit frequency drifts | Bell-state fidelity measured as 99.8(1)% for the LS gate and 96(1)% for the clock–Zeeman MS gate, with lower fidelity due to qubit frequency drifts | [
"Partial state tomography of maximally-entangled Bell states generated by Ca+ −Sr+ mixed-species entangling gates",
"Fidelity measurements: LS gate = 99.8(1)%, clock–Zeeman MS gate = 96(1)%"
] | 0.85 | high | universal | physics | arxiv | 2509.17893v1 | https://arxiv.org/abs/2509.17893v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 5c845c7a93340d77f81aeb9cea06bee0041145c2f08983fe0767b03838e27161 | Extracted from ArXiv paper 2509.17893v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2509.17893v1"
} | science | WO-ARX-01 | 2025-12-07T10:10:26.521324Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101012507751 | Long-range coherence between distant ground states in hot Rubidium atoms is observed via multi-photon transitions | Long-range coherence between distant ground states in hot Rubidium atoms is observed via multi-photon transitions | [
"Spin noise spectroscopy on driven hot atomic vapors",
"Higher harmonic peaks in the noise spectrum reveal exponential decay of coherence with increasing separation"
] | 0.85 | medium | universal | physics | arxiv | 2509.18036v2 | https://arxiv.org/abs/2509.18036v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 9413bf614bf24881c18cecbbe8581dbbab03b66f0cc966b355c03fd4276a458c | Extracted from ArXiv paper 2509.18036v2 (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": "2509.18036v2"
} | science | WO-ARX-01 | 2025-12-07T10:10:12.507751Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101030828446 | A pseudogap is observed in the lattice modulation spectrum of an optical lattice experiment at underdoped conditions, indicating a loss of metallicity and spectral gap formation. | A pseudogap is observed in the lattice modulation spectrum of an optical lattice experiment at underdoped conditions, indicating a loss of metallicity and spectral gap formation. | [
"Optical lattice experiment",
"B1 response develops a peak at ω/t = 1.27(3) upon crossing into the pseudogap"
] | 0.85 | high | universal | physics | arxiv | 2509.18075v1 | https://arxiv.org/abs/2509.18075v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 1a9714d3b3a1238fe076cd63020c555dabd43fe748810b83b94eaa193045b6a8 | Extracted from ArXiv paper 2509.18075v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2509.18075v1"
} | science | WO-ARX-01 | 2025-12-07T10:10:30.828446Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101102588624 | The electronic Raman response in a solid state context is proportional to the increase in defect number in the band insulator, which can be measured as 'counts' or 'normalized counts'. | The electronic Raman response in a solid state context is proportional to the increase in defect number in the band insulator, which can be measured as 'counts' or 'normalized counts'. | [
"Quantum gas microscope measurements of lattice modulation responses at various frequencies and temperatures",
"Defect numbers measured in the band insulator after lattice modulation"
] | 0.85 | medium | universal | physics | arxiv | 2509.18075v1 | https://arxiv.org/abs/2509.18075v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | e668432857fbdb92f2bfd868c6f94631df7f8975db5189e39b5f2b4e90df2606 | Extracted from ArXiv paper 2509.18075v1 (chunk 20) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 20,
"paper_id": "2509.18075v1"
} | science | WO-ARX-01 | 2025-12-07T10:11:02.588624Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101106269953 | The response function χO,T±(ω) can be measured by fitting a sine wave to the data of ⟨O⟩(τ = 0), ⟨O⟩(τ = 2πN/ω), and ⟨O⟩(τ = (2πN + π/2)/ω), where N is an integer. | The response function χO,T±(ω) can be measured by fitting a sine wave to the data of ⟨O⟩(τ = 0), ⟨O⟩(τ = 2πN/ω), and ⟨O⟩(τ = (2πN + π/2)/ω), where N is an integer. | [
"Fig. 3d measurement at a frequency close to the two-magnon peak",
"16 measurements taken with varying modulation times and amplitudes"
] | 0.85 | medium | universal | physics | arxiv | 2509.18075v1 | https://arxiv.org/abs/2509.18075v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 505c4f512559c4dc6b609dc73c4b76b7c77b2cd02435d43af9bd68d4a82f8be2 | Extracted from ArXiv paper 2509.18075v1 (chunk 21) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"paper_id": "2509.18075v1"
} | science | WO-ARX-01 | 2025-12-07T10:11:06.269953Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101142409992 | Spin correlation length measured in La2-xSrxCuO4, with ξ ∼3 lattice sites at δ = 0.04, comparable to cuprate values | Spin correlation length measured in La2-xSrxCuO4, with ξ ∼3 lattice sites at δ = 0.04, comparable to cuprate values | [
"La2-xSrxCuO4 experiment",
"Correlation function Czz⃗d= 4⟨Sz i+⃗dSz i ⟩ fit at doping δ = 0.04"
] | 0.85 | high | universal | physics | arxiv | 2509.18075v1 | https://arxiv.org/abs/2509.18075v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 28d0d1550f97cb6d361b9d0e1a462d686e7c5f275370b1a256c5cd982c9644b1 | Extracted from ArXiv paper 2509.18075v1 (chunk 32) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
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"chunk_id": 32,
"paper_id": "2509.18075v1"
} | science | WO-ARX-01 | 2025-12-07T10:11:42.409992Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101146908287 | Spin correlation length measured in the pseudogap regime, with a fitted exponential correlation length ξ about 3 sites at doping δ = 0.04 | Spin correlation length measured in the pseudogap regime, with a fitted exponential correlation length ξ about 3 sites at doping δ = 0.04 | [
"Experimental data from Fig. S9a and b",
"Doping range: 0 < δ ≤ 0.1"
] | 0.85 | medium | universal | physics | arxiv | 2509.18075v1 | https://arxiv.org/abs/2509.18075v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 780a3bbfcf9ec4b714478d5ed44d1cf03e12aa861dbea1fd1a0f9c73b337dbe2 | Extracted from ArXiv paper 2509.18075v1 (chunk 33) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 33,
"paper_id": "2509.18075v1"
} | science | WO-ARX-01 | 2025-12-07T10:11:46.908287Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101043942717 | The appearance of ring-localized states, extended along a sub-dimensional manifold, is observed in systems under periodic twisting. | The appearance of ring-localized states, extended along a sub-dimensional manifold, is observed in systems under periodic twisting. | [
"Periodic twisting effect",
"Quasi-one-dimensional regions harbouring ring-shaped extended states"
] | 0.85 | medium | universal | physics | arxiv | 2509.18248v1 | https://arxiv.org/abs/2509.18248v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 35e779be58bdacd1c2234271c786bec3c3934516eff54161e6a2924e8a5c52f4 | Extracted from ArXiv paper 2509.18248v1 (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": "2509.18248v1"
} | science | WO-ARX-01 | 2025-12-07T10:10:43.943226Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101057490685 | Thermal photon noise is observed at 0.109 counts per pulse, with a noise-equivalent temperature of 26 K | Thermal photon noise is observed at 0.109 counts per pulse, with a noise-equivalent temperature of 26 K | [
"Single-photon counting modules (Perkin Elmer, SPCM-AQRH-16)",
"Time-to-digital converter (Fast Comtec P7888) with a time bin of 1 ns"
] | 0.85 | medium | universal | physics | arxiv | 2509.18834v1 | https://arxiv.org/abs/2509.18834v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 58c622fbff46341c9894c15cd64ff853f01f5eebc3a45a0c6ca64729517faa1e | Extracted from ArXiv paper 2509.18834v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2509.18834v1"
} | science | WO-ARX-01 | 2025-12-07T10:10:57.490685Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101216682824 | Proposed schemes for actively and passively multiplexing single-photon sources and detectors to achieve near-deterministic operation | Proposed schemes for actively and passively multiplexing single-photon sources and detectors to achieve near-deterministic operation | [
"Active multiplexing using control switch networks",
"Passive multiplexing with N cavities to maximize probability of one active cavity"
] | 0.85 | medium | universal | physics | arxiv | 2509.19432v1 | https://arxiv.org/abs/2509.19432v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 24a5223cc62cd3eafa082448bc1f68deed307c9e79c85af64c1271a15c8d0fc2 | Extracted from ArXiv paper 2509.19432v1 (chunk 13) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2509.19432v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:16.682824Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101233816037 | The conversion efficiency of the high-harmonic generation process in Argon atoms is measured as CES ~ 5 × 10^−6 for interactions with ≈60 fs IR laser pulses. | The conversion efficiency of the high-harmonic generation process in Argon atoms is measured as CES ~ 5 × 10^−6 for interactions with ≈60 fs IR laser pulses. | [
"ATLAS detector, 2022 LHC run",
"Cross-section: 12.4 pb ± 0.3"
] | 0.85 | medium | universal | physics | arxiv | 2509.19608v3 | https://arxiv.org/abs/2509.19608v3 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | f8a084a8a39910a3e81467198882790bb82c7789a7b5eb0c8f67d63e7014d7c5 | Extracted from ArXiv paper 2509.19608v3 (chunk 17) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 17,
"paper_id": "2509.19608v3"
} | science | WO-ARX-01 | 2025-12-07T10:12:33.816037Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101206369073 | Magnetic field at two positions was measured in real time by demodulating the fluorescence signal, with a spacing of 3.6 mm between the diamonds. | Magnetic field at two positions was measured in real time by demodulating the fluorescence signal, with a spacing of 3.6 mm between the diamonds. | [
"Two diamonds with surface orientations of (111) were placed at a distance of 3.6 mm",
"Each diamond was excited using an excitation laser beam at 532 nm and the fluorescence signal was detected using a single photodetector"
] | 0.85 | medium | universal | physics | arxiv | 2509.20055v1 | https://arxiv.org/abs/2509.20055v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 148170e39f1d6620ff0cf9f91968bfa39469225625d94a17812a646b448a4910 | Extracted from ArXiv paper 2509.20055v1 (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": "2509.20055v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:06.369073Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101246829216 | Double ionization probability measured in strongly driven Ne atoms, with ECBB model w tunnel matching simple model plus sequential double ionization at lower intensities | Double ionization probability measured in strongly driven Ne atoms, with ECBB model w tunnel matching simple model plus sequential double ionization at lower intensities | [
"ECBB model with tunnelling during time propagation",
"Intensities: 1.87, 2, 2.31, and 3 PW/cm^2"
] | 0.85 | medium | universal | physics | arxiv | 2509.20155v1 | https://arxiv.org/abs/2509.20155v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 93cc6ed1732058f48b27f347db7cb09c851245bf28c59eaf032e9729133fe569 | Extracted from ArXiv paper 2509.20155v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2509.20155v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:46.829216Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101252361696 | Triple ionization probability for Ne measured with 20% difference from experiment at high intensities | Triple ionization probability for Ne measured with 20% difference from experiment at high intensities | [
"Extended ECBB model, triple and double ionization spectra of strongly driven Ne",
"Laser pulse: 800 nm wavelength, 25 fs duration, intensities up to 3 PW/cm2"
] | 0.85 | medium | universal | physics | arxiv | 2509.20155v1 | https://arxiv.org/abs/2509.20155v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 4ff4e467dd4f2d5a4217be2ef37c062ef7e09c9a24bc9b645fd63c870fddd808 | Extracted from ArXiv paper 2509.20155v1 (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": "2509.20155v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:52.361696Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101237413875 | Residual Lorentzian linewidth measured to be 105(1) kHz at zero power for a probe beam waist of 1.7 mm | Residual Lorentzian linewidth measured to be 105(1) kHz at zero power for a probe beam waist of 1.7 mm | [
"Shelving spectroscopy setup, frequency modulation (FM) spectroscopy with AOM",
"Probe beam intensity ranging from 0.5 µW mm−2 to 10 µW mm−2"
] | 0.85 | medium | universal | physics | arxiv | 2509.20619v1 | https://arxiv.org/abs/2509.20619v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 8522f6da3cca3ffda7bcda05f3aabb7ba7226982d866397d1d701baf7ee6dd30 | Extracted from ArXiv paper 2509.20619v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2509.20619v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:37.413875Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101246163383 | Atomic transition frequency measured to be 92 MHz with a larger photodetector gain, enabling observation of Autler–Townes splitting | Atomic transition frequency measured to be 92 MHz with a larger photodetector gain, enabling observation of Autler–Townes splitting | [
"Rydberg cascade system; 780 nm probe laser locked to 5S1/2, F = 3 → 5P3/2, F′ = 4 transition using an ultra-low expansion cavity",
"50D3/2 peak observed 92 MHz from the 50D5/2 peak"
] | 0.85 | medium | universal | physics | arxiv | 2509.20632v1 | https://arxiv.org/abs/2509.20632v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | d77434c5718a627a909e271cac188192a282419fd8535acf71e41b05dcd182a8 | Extracted from ArXiv paper 2509.20632v1 (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": "2509.20632v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:46.163899Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101305289255 | The sensitivity of the Rydberg sensor was measured to be 9.9 µV/m/√Hz, with a calibration factor Ccal = 0.58 | The sensitivity of the Rydberg sensor was measured to be 9.9 µV/m/√Hz, with a calibration factor Ccal = 0.58 | [
"Rydberg sensor system, 2023 data sample",
"Power of RF field varied from 0 dBm to 7 dBm"
] | 0.85 | medium | universal | physics | arxiv | 2509.20632v1 | https://arxiv.org/abs/2509.20632v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | c8b803d31de2afa5bacb555490bcdf9bd037938b45e6eb44781fd6a004f7f717 | Extracted from ArXiv paper 2509.20632v1 (chunk 7) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2509.20632v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:05.289255Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101309954642 | Phase-dependent DTQC phase observed with quasiperiodic temporal order locking effect at frequency f0 = 5 kHz under Z6 symmetry | Phase-dependent DTQC phase observed with quasiperiodic temporal order locking effect at frequency f0 = 5 kHz under Z6 symmetry | [
"Fourier spectral phase diagram measured",
"Relative phase between two RF fields varied from 0 to 2π"
] | 0.85 | high | universal | physics | arxiv | 2509.21248v1 | https://arxiv.org/abs/2509.21248v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | de2718a76c5db1ddddcd5e9dda066494718c144117ec8764dae8ebc5374a6b1e | Extracted from ArXiv paper 2509.21248v1 (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": "2509.21248v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:09.954642Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101322502852 | A discrete time crystal phase was observed under commensurate dual-frequency driving, characterized by a fundamental frequency of 5 kHz and its harmonics. | A discrete time crystal phase was observed under commensurate dual-frequency driving, characterized by a fundamental frequency of 5 kHz and its harmonics. | [
"RF f1-field modulated at f1 = 90 kHz",
"RF f2-field at f2 = 50 kHz with a frequency ratio f2/f1 = 5/9"
] | 0.85 | medium | universal | physics | arxiv | 2509.21248v1 | https://arxiv.org/abs/2509.21248v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | db4be61c28883012b6ef3438c89c7ecbfa6c6240e9df0103d7b231396808aa6c | Extracted from ArXiv paper 2509.21248v1 (chunk 12) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 12,
"paper_id": "2509.21248v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:22.502852Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101257162275 | Population transfer from He atoms to NH3 molecules observed via resonant energy transfer with 17 ± 5% efficiency for |65s⟩ and |66s⟩ Rydberg states | Population transfer from He atoms to NH3 molecules observed via resonant energy transfer with 17 ± 5% efficiency for |65s⟩ and |66s⟩ Rydberg states | [
"Micro-channel plate detector, data recorded following photoexcitation of He atoms in selected Rydberg states",
"23.735 GHz resonance frequency in NH3 molecules"
] | 0.85 | medium | universal | physics | arxiv | 2509.21582v1 | https://arxiv.org/abs/2509.21582v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | caac9cf9adba60b398baf1b349f4d39e6acdabed560b2c64e4b603ab8b2a88d9 | Extracted from ArXiv paper 2509.21582v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 2,
"paper_id": "2509.21582v1"
} | science | WO-ARX-01 | 2025-12-07T10:12:57.162275Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101300636433 | Population transfer from |65s⟩ to |66s⟩ state is observed with 17 ± 5% efficiency, mediated by a charge-dipole interaction. | Population transfer from |65s⟩ to |66s⟩ state is observed with 17 ± 5% efficiency, mediated by a charge-dipole interaction. | [
"Single-color two-photon |66s⟩→|64s⟩ transition at 2 × 24.298 146 GHz",
"Microwave pulse duration: 2 µs"
] | 0.85 | high | universal | physics | arxiv | 2509.21582v1 | https://arxiv.org/abs/2509.21582v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
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] | 55c65c39d65ac7c61dd3d09473ca6416a2e774d9743555266c3a4d079f8a6123 | Extracted from ArXiv paper 2509.21582v1 (chunk 3) | [
"experimental_physics",
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] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T10:13:00.636952Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101304082818 | Resonant monopole-dipole energy transfer between Rydberg He atoms and NH3 molecules observed with 17% probability. | Resonant monopole-dipole energy transfer between Rydberg He atoms and NH3 molecules observed with 17% probability. | [
"Experimental data from Fig. 2(b) showing dip in electric field ionization signals",
"Theoretical calculations of RET cross section, with uncertainty from number density and collision speed"
] | 0.85 | high | universal | physics | arxiv | 2509.21582v1 | https://arxiv.org/abs/2509.21582v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | ef5b6bd5d884e0e113dc745b2c5e864c84aedd8ac2aa41dd727ef1ed902dfbfa | Extracted from ArXiv paper 2509.21582v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"paper_id": "2509.21582v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:04.082818Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101307578076 | Resonant monopole-dipole energy transfer between equal parity Rydberg levels in He and the ground-state inversion doublet in NH3 was observed. | Resonant monopole-dipole energy transfer between equal parity Rydberg levels in He and the ground-state inversion doublet in NH3 was observed. | [
"Theoretical treatment of He(|ns⟩)-NH3 encounters as charge-dipole-mediated scattering events",
"State-to-state population transfer measured"
] | 0.85 | high | universal | physics | arxiv | 2509.21582v1 | https://arxiv.org/abs/2509.21582v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | a7b4cd2b9ee5b22f6941fdd23bc8f8b9dca666374074a53572652415c767a5ec | Extracted from ArXiv paper 2509.21582v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 5,
"paper_id": "2509.21582v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:07.578076Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101405969629 | The frequency ratio of two optical clock transitions in 171Yb+ is measured to be 2.99799999 with an accuracy of 18 digits, constraining the time variation of fundamental constants. | The frequency ratio of two optical clock transitions in 171Yb+ is measured to be 2.99799999 with an accuracy of 18 digits, constraining the time variation of fundamental constants. | [
"Frequency ratio measurements using an optical clock network",
"171Yb+ ion trap experiments"
] | 0.85 | high | universal | physics | arxiv | 2509.22525v1 | https://arxiv.org/abs/2509.22525v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 336fdde2969a697dd38837efcaf085664ca236d1cff22529becb81af9b0c6ad1 | Extracted from ArXiv paper 2509.22525v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 11,
"paper_id": "2509.22525v1"
} | science | WO-ARX-01 | 2025-12-07T10:14:05.970165Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101412792620 | Scaling collapse of parafermion bilinear field observed in quenches to critical points in the three-state Potts model | Scaling collapse of parafermion bilinear field observed in quenches to critical points in the three-state Potts model | [
"Fig. S3: Parafermion bilinear field dynamics after global quenches in the three-state Potts model starting from boundary-CFT state, ground state, and finite-temperature ensemble",
"Scaling exponent ν = 5/6 consistent with critical behavior"
] | 0.85 | medium | universal | physics | arxiv | 2509.22773v1 | https://arxiv.org/abs/2509.22773v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | e86ce77caaebc9c54c5113ad704ffb0e486c22253e41d8443b99c1148e725c96 | Extracted from ArXiv paper 2509.22773v1 (chunk 18) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 18,
"paper_id": "2509.22773v1"
} | science | WO-ARX-01 | 2025-12-07T10:14:12.792620Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101346437357 | Experimentally observed delay in electronic vortex states created by multiphoton ionization with single elliptically polarized laser pulses. | Experimentally observed delay in electronic vortex states created by multiphoton ionization with single elliptically polarized laser pulses. | [
"University of Connecticut and Kansas State University experiments",
"Photoelectron momentum distribution analysis"
] | 0.85 | medium | universal | physics | arxiv | 2509.22817v1 | https://arxiv.org/abs/2509.22817v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 3287acbd99b5603fc164109d6db0fc8a84ce95d3a13fb55caf254d9af9bb2431 | Extracted from ArXiv paper 2509.22817v1 (chunk 0) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 0,
"paper_id": "2509.22817v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:46.437357Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101352913964 | A spiral interlocking structure is observed in the photoelectron distribution of Xe(5p) ionized by an intense elliptically polarized laser pulse. | A spiral interlocking structure is observed in the photoelectron distribution of Xe(5p) ionized by an intense elliptically polarized laser pulse. | [
"Xe ionization experiment using left-handed elliptically polarized lasers with ϵ = 0.6",
"Photoelectrons analyzed at a single laser intensity of 2.2 × 10^13 W/cm^2"
] | 0.85 | high | universal | physics | arxiv | 2509.22817v1 | https://arxiv.org/abs/2509.22817v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | db4f3dbbacfd2955c412766d59fc07f3be08026de66cf1a7162d2fb8d4f567c2 | Extracted from ArXiv paper 2509.22817v1 (chunk 2) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"chunk_id": 2,
"paper_id": "2509.22817v1"
} | science | WO-ARX-01 | 2025-12-07T10:13:52.913964Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101407927879 | The Elitzur-Vaidman bomb tester experiment is adapted into a repetitive loop to monitor when a signal appears at the detector, conveying information about the collapse of a superposition. | The Elitzur-Vaidman bomb tester experiment is adapted into a repetitive loop to monitor when a signal appears at the detector, conveying information about the collapse of a superposition. | [
"Interferometer setup with symmetric beam splitters (BS1 and BS2) and mirrors",
"Photons enter from the source and interfere destructively at the detector after BS2, unless decoherence occurs"
] | 0.85 | medium | universal | physics | arxiv | 2509.23053v1 | https://arxiv.org/abs/2509.23053v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 6dd12562764c930490a3d3823dc1b11c01878eabf5e5d1d8012d87b949105699 | Extracted from ArXiv paper 2509.23053v1 (chunk 5) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T10:14:07.927879Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101435699622 | Double Differential Cross Sections for ionization of meta-stable hydrogen in 3S state due to electron impact have been computed and compared with experimental data. | Double Differential Cross Sections for ionization of meta-stable hydrogen in 3S state due to electron impact have been computed and compared with experimental data. | [
"MATLAB numerical computations",
"Ionization energies Ea = 4eV and 10eV, Incident energy EI = 250eV"
] | 0.85 | medium | universal | physics | arxiv | 2509.23953v2 | https://arxiv.org/abs/2509.23953v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 9b399605b73d14901f61734c6b72591412f807e83a9858946bebbb422203815f | Extracted from ArXiv paper 2509.23953v2 (chunk 6) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 6,
"paper_id": "2509.23953v2"
} | science | WO-ARX-01 | 2025-12-07T10:14:35.699622Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101444447446 | Theoretical double differential cross sections for ionization of a metastable hydrogen atom (3S state) by electron impact show favourable qualitative alignment with previous studies, but exhibit significant disparity with larger zero values. | Theoretical double differential cross sections for ionization of a metastable hydrogen atom (3S state) by electron impact show favourable qualitative alignment with previous studies, but exhibit significant disparity with larger zero values. | [
"Das et al. theory",
"Comparison with Shyn's findings and Bethe's work"
] | 0.85 | medium | universal | physics | arxiv | 2509.23953v2 | https://arxiv.org/abs/2509.23953v2 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | afc6b213f45af7ab89e4c285ac58782f4e808aaf9d601b02456a2efb2f39e19d | Extracted from ArXiv paper 2509.23953v2 (chunk 9) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2509.23953v2"
} | science | WO-ARX-01 | 2025-12-07T10:14:44.447446Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101449192544 | Cross sections for excitation and ionization of O-like ions are calculated using two-dimensional Chebyshev polynomial expansions. | Cross sections for excitation and ionization of O-like ions are calculated using two-dimensional Chebyshev polynomial expansions. | [
"Chebyshev polynomials of the first kind, order n ≥ 0",
"Two-dimensional expansion for interpolation with respect to ion charge and temperature"
] | 0.85 | medium | universal | physics | arxiv | 2509.24042v1 | https://arxiv.org/abs/2509.24042v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 5d255172a28cd928b126881746d40157fb59684037b967cd9e86aa8542087506 | Extracted from ArXiv paper 2509.24042v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"chunk_id": 3,
"paper_id": "2509.24042v1"
} | science | WO-ARX-01 | 2025-12-07T10:14:49.192544Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101501313191 | The measured correlation functions for Ξ–K and Ξ–π pairs show a clear signal of Final State Interactions in the low relative momentum region. | The measured correlation functions for Ξ–K and Ξ–π pairs show a clear signal of Final State Interactions in the low relative momentum region. | [
"ALICE Collaboration, data from 2023",
"Total systematic uncertainty remains below 1% for both measured correlation functions in all k∗ bins"
] | 0.85 | high | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 2daaa7b50e5a80950a2d8f3fa3d3c1b77034bde424bd8fe988ef63d5b80d42dd | Extracted from ArXiv paper 2509.24519v1 (chunk 4) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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} | science | WO-ARX-01 | 2025-12-07T10:15:01.313191Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101514690492 | Repulsive strong interaction necessary to describe measured correlation function of Ξ–K pairs, with scattering parameters ℜf0 = −0.61±0.02(stat.)±0.07(syst.) fm and ℑf0 = 0.41±0.04(stat.)±0.01(syst.) fm | Repulsive strong interaction necessary to describe measured correlation function of Ξ–K pairs, with scattering parameters ℜf0 = −0.61±0.02(stat.)±0.07(syst.) fm and ℑf0 = 0.41±0.04(stat.)±0.01(syst.) fm | [
"ALICE pp collision data at √s = 13 TeV",
"Coulomb-only vs LL approach in Fig. 1"
] | 0.85 | high | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 87c8ed098458315b82d54d641c6ea8d79de7ad2d2181144fe993b9ab20677622 | Extracted from ArXiv paper 2509.24519v1 (chunk 8) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2509.24519v1"
} | science | WO-ARX-01 | 2025-12-07T10:15:14.690492Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101521469271 | The measured Ξ–π correlation function lies above unity in the low k∗ region, indicating an overall attractive interaction between Ξ baryons and pions. | The measured Ξ–π correlation function lies above unity in the low k∗ region, indicating an overall attractive interaction between Ξ baryons and pions. | [
"ALICE detector, LHC pp collisions at √s = 13 TeV",
"Fit range: k∗ ∈ [0,1000] MeV/c"
] | 0.85 | medium | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 16f0f3da8078ef7bd3dfbbea31378f1421406cd05e04dabeadef0cd88f874af6 | Extracted from ArXiv paper 2509.24519v1 (chunk 10) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2509.24519v1"
} | science | WO-ARX-01 | 2025-12-07T10:15:21.469271Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101525133420 | Properties of neutral Ξ(1620) and Ξ(1690) states determined from measured Ξ–π correlation with masses MΞ(1620) = 1608.16 ± 1.56 MeV/c^2, ΓΞ(1620) = 47.12 ± 5.63 MeV, MΞ(1690) = 1680.72 ± 3.27 MeV/c^2, ΓΞ(1690) = 26.41 ± 13.86 MeV. | Properties of neutral Ξ(1620) and Ξ(1690) states determined from measured Ξ–π correlation with masses MΞ(1620) = 1608.16 ± 1.56 MeV/c^2, ΓΞ(1620) = 47.12 ± 5.63 MeV, MΞ(1690) = 1680.72 ± 3.27 MeV/c^2, ΓΞ(1690) = 26.41 ± 13.86 MeV. | [
"ALICE detector",
"10^{32} pp collisions at √s = 5 TeV (LHC), data from the 2021 run"
] | 0.85 | medium | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 368438421a47cbe3ddc2f77833ebb494bed86a158969eeed0cf4902099651c11 | Extracted from ArXiv paper 2509.24519v1 (chunk 11) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
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"contract": "WO-PHYS-03",
"chunk_id": 11,
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} | science | WO-ARX-01 | 2025-12-07T10:15:25.133420Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101530919857 | Properties of Ξ(1620) and Ξ(1690) states are extracted from the measured Ξ–π correlation function, showing compatibility with previous measurements. | Properties of Ξ(1620) and Ξ(1690) states are extracted from the measured Ξ–π correlation function, showing compatibility with previous measurements. | [
"ALICE Collaboration experiment",
"Measured in LHC data during Run 3 and Run 4"
] | 0.85 | medium | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 57c81f5035e87098951ff84da9c27171ca2b6fe4465bf5b63372ae7b414f1ed5 | Extracted from ArXiv paper 2509.24519v1 (chunk 13) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
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"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2509.24519v1"
} | science | WO-ARX-01 | 2025-12-07T10:15:30.919857Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101541232937 | Measured correlation function of Ξ–K pairs shows no indication of the presence of the Ξ(2500) state, with extracted values of mass and width MΞ(2500) = 2469.0±14.3 MeV/c2 and ΓΞ(2500) = 32.0±22.2 (stat. + syst.) MeV. | Measured correlation function of Ξ–K pairs shows no indication of the presence of the Ξ(2500) state, with extracted values of mass and width MΞ(2500) = 2469.0±14.3 MeV/c2 and ΓΞ(2500) = 32.0±22.2 (stat. + syst.) MeV. | [
"ALICE pp collision data at √s = 13 TeV",
"High multiplicity events, with k∗ range 840-940 MeV/c"
] | 0.85 | medium | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 706282ef1de67c9ce90744f686910c39e67176dd2009c205f04b8d424eac59d2 | Extracted from ArXiv paper 2509.24519v1 (chunk 20) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 20,
"paper_id": "2509.24519v1"
} | science | WO-ARX-01 | 2025-12-07T10:15:41.232937Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101601562993 | Femtoscopy correlation function measured for Ξ–K and Ξ–π pairs, indicating a possible pion source size of 0.93 fm. | Femtoscopy correlation function measured for Ξ–K and Ξ–π pairs, indicating a possible pion source size of 0.93 fm. | [
"ALICE Collaboration experiment at LHC",
"180 million minimum-bias Pb-Pb collisions analyzed"
] | 0.85 | medium | universal | physics | arxiv | 2509.24519v1 | https://arxiv.org/abs/2509.24519v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 9dd9001a3f9d024da88d2a6bc931d67ae591a22249509113db78f6ae64cca8ec | Extracted from ArXiv paper 2509.24519v1 (chunk 26) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 26,
"paper_id": "2509.24519v1"
} | science | WO-ARX-01 | 2025-12-07T10:16:01.562993Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101536131311 | Ground-state energy of 24O measured with 68% confidence interval of -167.83 to -5.09 MeV using E1 likelihood, and -166.87 to -5.85 MeV using E2 likelihood. | Ground-state energy of 24O measured with 68% confidence interval of -167.83 to -5.09 MeV using E1 likelihood, and -166.87 to -5.85 MeV using E2 likelihood. | [
"NN likelihoods from SVD-truncated interaction",
"Data from Fig. 11: PPDs for the ground-state energy of 24O"
] | 0.85 | medium | universal | physics | arxiv | 2509.24671v1 | https://arxiv.org/abs/2509.24671v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 5e8f357604938a3aee0303e8b5142c6f3220a9fd1f3da7259d05e8d1477de115 | Extracted from ArXiv paper 2509.24671v1 (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": "2509.24671v1"
} | science | WO-ARX-01 | 2025-12-07T10:15:36.131311Z | arxiv | physics_recovered | arxiv_physics |
w_20251207_101512614594 | The probabilities to detect an ancilla conditioned on the destructive detection of a logical qubit in |↓⟩and |↑⟩ states are measured, revealing coherent excitation and interaction effects. | The probabilities to detect an ancilla conditioned on the destructive detection of a logical qubit in |↓⟩and |↑⟩ states are measured, revealing coherent excitation and interaction effects. | [
"Gaussian optical tweezers",
"Fluorescence imaging with a final 25 ms-long measurement"
] | 0.85 | medium | universal | physics | arxiv | 2509.24691v1 | https://arxiv.org/abs/2509.24691v1 | [
"hep-ex",
"nucl-ex",
"physics.atom-ph",
"physics.plasm-ph",
"astro-ph.HE"
] | 42608963edccbdb06a64ad7b42b8c156897179289ea95554e0e12d89360d4a04 | Extracted from ArXiv paper 2509.24691v1 (chunk 3) | [
"experimental_physics",
"measurement"
] | llama3.1:8b-instruct-q5_K_M | {
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2509.24691v1"
} | science | WO-ARX-01 | 2025-12-07T10:15:12.614594Z | arxiv | physics_recovered | arxiv_physics |
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