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value | pack_id
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value |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
w_20251209_173722870021
|
Penetration height of liquid jet in supersonic crossflow measured at various fuel mass flow rates and temperatures, with agreement to established correlations for lower temperature conditions
|
Penetration height of liquid jet in supersonic crossflow measured at various fuel mass flow rates and temperatures, with agreement to established correlations for lower temperature conditions
|
[
"Time-averaged schlieren images",
"Shadowgraph images, Fig.8, scaled to match schlieren image resolution",
"Penetration height y/dj calculated from binarized images using Image J algorithm"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.18537v1
|
https://arxiv.org/abs/2510.18537v1
|
[
"physics.flu-dyn",
"physics.app-ph"
] |
bca2502a0727ac3194890afa9bce1d8664528027c107cfe3590c73f04369a461
|
Extracted from ArXiv paper 2510.18537v1 (chunk 10)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 10,
"paper_id": "2510.18537v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:37:22.870021Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_173910188091
|
Variability in wind speed and direction increases with wind speed, with minimal variability observed at around 35 degrees.
|
Variability in wind speed and direction increases with wind speed, with minimal variability observed at around 35 degrees.
|
[
"Wind variability study using data from an unknown location",
"Linear correlation between variability in wind speed (ξv) and speed itself (top left of Figure 7)",
"Plateau value of relative variability (ξv/vmax) reached at larger wind speeds"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.19433v1
|
https://arxiv.org/abs/2510.19433v1
|
[
"physics.app-ph",
"cs.CE",
"physics.ao-ph"
] |
f8d31ebf9846247b0acfcb5924095143399b24ab3ff92df96ea742105053dd59
|
Extracted from ArXiv paper 2510.19433v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.19433v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:39:10.188091Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_173921184886
|
Microturbulence in W7-X stellarator plasma is dominated by microtearing modes, reproducing experimentally observed heat and particle fluxes.
|
Microturbulence in W7-X stellarator plasma is dominated by microtearing modes, reproducing experimentally observed heat and particle fluxes.
|
[
"W7-X tokamak discharge #20181009.034",
"Total injected power P ≈3.7 MW",
"Collisionality and electromagnetic fluctuations key physical effects included in simulations"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19543v1
|
https://arxiv.org/abs/2510.19543v1
|
[
"physics.plasm-ph"
] |
dc2660783dc3f5607b38e962f17d68bb03124a70b3b63864bde8af7a55ec999b
|
Extracted from ArXiv paper 2510.19543v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.19543v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:39:21.184886Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_173936607896
|
Microtearing mode turbulence was observed in W7-X stellarator, driven by moderate collisionality and low magnetic shear.
|
Microtearing mode turbulence was observed in W7-X stellarator, driven by moderate collisionality and low magnetic shear.
|
[
"W7-X stellarator experiment",
"Density gradient: sufficiently large",
"Moderate temperature gradients"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.19543v1
|
https://arxiv.org/abs/2510.19543v1
|
[
"physics.plasm-ph"
] |
ee015b7353dc4b3b493d7e9264786c29a7ef5ef2612b4e62973c7ece9214bbc4
|
Extracted from ArXiv paper 2510.19543v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.19543v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:39:36.608436Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174224350222
|
The Advanced Virgo thermal compensation system achieves a 30% reduction in thermal noise over the full detector bandwidth.
|
The Advanced Virgo thermal compensation system achieves a 30% reduction in thermal noise over the full detector bandwidth.
|
[
"Advanced Virgo gravitational wave detector",
"Thermal noise reduction: 30%",
"Full detector bandwidth"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.20338v1
|
https://arxiv.org/abs/2510.20338v1
|
[
"physics.app-ph",
"astro-ph.IM",
"gr-qc",
"physics.optics"
] |
912620ae256ea94d2aa32947ed07366155bece416e3cfe89def0764e62d4f17f
|
Extracted from ArXiv paper 2510.20338v1 (chunk 13)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2510.20338v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:42:24.350222Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174251059911
|
Quantum coherence of electrons in epitaxial TiN films is measured, revealing moderate surface magnetic disorder leading to a decrease in superconducting critical temperature and phase-breaking scattering rates.
|
Quantum coherence of electrons in epitaxial TiN films is measured, revealing moderate surface magnetic disorder leading to a decrease in superconducting critical temperature and phase-breaking scattering rates.
|
[
"TiN films grown on c-plane sapphire substrate using DC reactive magnetron sputtering",
"Magnetotransport measurements show electron dephasing due to surface magnetic disorder",
"Structural analysis confirms single-crystal homogeneity"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.20576v1
|
https://arxiv.org/abs/2510.20576v1
|
[
"cond-mat.supr-con",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
b70ca72a6c5186366e5d74222cfd65c2067202febe89ee0cfb1f59ff84703879
|
Extracted from ArXiv paper 2510.20576v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2510.20576v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:42:51.060440Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174304823191
|
Electron phase-breaking rate τ−1φ measured in epitaxial TiN films, with values ranging from 0.1 to 10 ns at 10−3 K.
|
Electron phase-breaking rate τ−1φ measured in epitaxial TiN films, with values ranging from 0.1 to 10 ns at 10−3 K.
|
[
"MR1-MR4 samples",
"Estimated spin-flip scattering rate τs: 2.3-13.2 ps for MR1-MR4",
"NM < 0.03%"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.20576v1
|
https://arxiv.org/abs/2510.20576v1
|
[
"cond-mat.supr-con",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
3226c1c3fdd6aff36f861e00f6186bbd54b06fd2747ef448a067d4acd37821a8
|
Extracted from ArXiv paper 2510.20576v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.20576v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:43:04.823191Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174527073038
|
Blobs' dynamics in the plasma edge show increased burst rate, lifetime, radial propagation speed, characteristic length, and experimental measured power scrape-off widths for higher SOL collisionality.
|
Blobs' dynamics in the plasma edge show increased burst rate, lifetime, radial propagation speed, characteristic length, and experimental measured power scrape-off widths for higher SOL collisionality.
|
[
"Comparison of blobs' dynamics with lower (ν∗SOL,e ∼33) and higher (ν∗SOL,e ∼92) SOL collisionality",
"Table 1: Correlation between blobs' dynamics and power scrape-off widths λq",
"Experimental measured power scrape-off width increase by 1.7 times"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.21170v1
|
https://arxiv.org/abs/2510.21170v1
|
[
"physics.plasm-ph"
] |
bae21704a41d14252a29b250b471e605ec6ee8b93d1f87c1dc5508c2180196b5
|
Extracted from ArXiv paper 2510.21170v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.21170v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:45:27.073038Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174543805819
|
Radial corrugation of electron temperature was measured in KSTAR L-mode plasmas, appearing as concentric jet-like patterns.
|
Radial corrugation of electron temperature was measured in KSTAR L-mode plasmas, appearing as concentric jet-like patterns.
|
[
"KSTAR experiment",
"Two-dimensional radial measurement",
"Temperature corrugation observed with suppressed MHD instabilities"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21170v1
|
https://arxiv.org/abs/2510.21170v1
|
[
"physics.plasm-ph"
] |
af28cbce3fc8c3e797863a55624af41af74a7dbd8f0d9aaf93749daf85acfd92
|
Extracted from ArXiv paper 2510.21170v1 (chunk 9)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2510.21170v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:45:43.805819Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174754541621
|
We measured power fluctuation statistics in four experimental sets to quantify turbulence-induced statistical deviations and compensation efficacy.
|
We measured power fluctuation statistics in four experimental sets to quantify turbulence-induced statistical deviations and compensation efficacy.
|
[
"Four experimental sets were recorded (Set 1: free-space baseline; Set 2: raw turbulence; Set 3: single PMMA rod; Set 4: double PMMA rods)",
"200 frames were recorded for each set, with a reference frame established for pairwise scintillation indices computation",
"Power fluctuation analysis and kernel density estimation were used to compare turbulence-induced statistical deviations"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21225v1
|
https://arxiv.org/abs/2510.21225v1
|
[
"physics.optics",
"physics.app-ph"
] |
469992868788cf41ca7ec0e64994fe7b0aeed55bfa04d81149df5ef3b2491cf8
|
Extracted from ArXiv paper 2510.21225v1 (chunk 23)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 23,
"paper_id": "2510.21225v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:47:54.541621Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174930642663
|
Two distinct spectral modes, high and low, are observed in simulations S1-S4, with the low mode exhibiting a unique behavior in both electric fields Ex and Ey.
|
Two distinct spectral modes, high and low, are observed in simulations S1-S4, with the low mode exhibiting a unique behavior in both electric fields Ex and Ey.
|
[
"S4 simulation data",
"ω frequency range: 0-140ωp",
"Modes identified through spectral analysis"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21666v1
|
https://arxiv.org/abs/2510.21666v1
|
[
"physics.plasm-ph"
] |
2473cfaa4c555dccb5046e6cc3c63581c46355ca26e79ff2301920e30654e0a6
|
Extracted from ArXiv paper 2510.21666v1 (chunk 12)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 12,
"paper_id": "2510.21666v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:49:30.642663Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_174938071663
|
Weibel instability is observed to generate a small-scale quasi-static magnetic field in the collision of electron-positron plasma clouds.
|
Weibel instability is observed to generate a small-scale quasi-static magnetic field in the collision of electron-positron plasma clouds.
|
[
"Collision of electron-positron plasma clouds",
"Small-scale quasi-static magnetic field generation",
"Fast particle acceleration"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.21675v1
|
https://arxiv.org/abs/2510.21675v1
|
[
"physics.plasm-ph"
] |
a670ff344631abe1b231700e33481ea80efc0533d7925cb7004a923eb954c7d5
|
Extracted from ArXiv paper 2510.21675v1 (chunk 11)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2510.21675v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:49:38.071663Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_175823258855
|
A single detector polarimeter using a dithered orthogonally polarized two-pulse source can accurately measure the local magnetic field B||*(s) in real-time for plasma control.
|
A single detector polarimeter using a dithered orthogonally polarized two-pulse source can accurately measure the local magnetic field B||*(s) in real-time for plasma control.
|
[
"one detector polarimeter",
"dithered orthogonally polarized two-pulse source",
"difference-over-sum intensity method"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.23562v1
|
https://arxiv.org/abs/2510.23562v1
|
[
"physics.plasm-ph",
"physics.acc-ph"
] |
8762af8c0a8d2104843b6b12805de541013b45ab0042b388d0ec0261e2ae51cf
|
Extracted from ArXiv paper 2510.23562v1 (chunk 7)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 7,
"paper_id": "2510.23562v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T17:58:23.258855Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_180206154377
|
Infrared reflectance spectra of the ME-FIRST sensor were measured with a spectral resolution of 4 cm−1 and averaged over 32 scans.
|
Infrared reflectance spectra of the ME-FIRST sensor were measured with a spectral resolution of 4 cm−1 and averaged over 32 scans.
|
[
"Bruker VERTEX 80v Fourier transform infrared spectrometer",
"Wire grid polarizer for polarized incident light",
"Reference gold mirror for calculating reflectance"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24210v1
|
https://arxiv.org/abs/2510.24210v1
|
[
"physics.optics",
"physics.app-ph"
] |
5c7293fbc985b09b48422a7f9bda414f1c106dc9d3c9d2a63bc0aa2a1c89955a
|
Extracted from ArXiv paper 2510.24210v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.24210v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:02:06.154898Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_180403220219
|
Radial bunching appears in the witness beam when propagating through high-density plasma due to betatron radiation losses, with multiple radial spatial bunches observed.
|
Radial bunching appears in the witness beam when propagating through high-density plasma due to betatron radiation losses, with multiple radial spatial bunches observed.
|
[
"FACET-II-like electron beams",
"High-density plasma (n0 = 1.6×1019 cm−3)",
"Betatron cooling"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.24567v1
|
https://arxiv.org/abs/2510.24567v1
|
[
"physics.acc-ph",
"physics.plasm-ph"
] |
4b8f5d91925298ed32756fe081a0e71821dc1b1118922006522d9b8419f4f75f
|
Extracted from ArXiv paper 2510.24567v1 (chunk 4)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 4,
"paper_id": "2510.24567v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:04:03.220219Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_180714305784
|
The magnon dispersion in YIG was measured with a saturation magnetization of 1.409 × 10^5 A/m and a pronounced PSSW band observed.
|
The magnon dispersion in YIG was measured with a saturation magnetization of 1.409 × 10^5 A/m and a pronounced PSSW band observed.
|
[
"Lock-in amplifier measurements, Fig.3(a-c)",
"MW pump pulse (20 ns, 4-GHz) and optical probe pulse widths",
"Kittel mode of YIG with theoretical fitting to the dispersion"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.24964v1
|
https://arxiv.org/abs/2510.24964v1
|
[
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
bd5c82e604dca735f57215272acfcbad01f04ca9d686434e7cfca1900572e523
|
Extracted from ArXiv paper 2510.24964v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.24964v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:07:14.306307Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181241475267
|
GW-BSE formalism accurately reproduces measured absorption spectrum of rectangular nanographenes, with two lowest bright excitations agreeing with experiment within 0.05 eV after finite-size extrapolation.
|
GW-BSE formalism accurately reproduces measured absorption spectrum of rectangular nanographenes, with two lowest bright excitations agreeing with experiment within 0.05 eV after finite-size extrapolation.
|
[
"CP2K package implementation",
"Rectangular nanographenes with fixed width and variable length (up to L = 13)",
"BSE@evGW0@PBE approach"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.25658v1
|
https://arxiv.org/abs/2510.25658v1
|
[
"physics.comp-ph",
"physics.chem-ph"
] |
d0ba3fef27c56e06153d92ea52a606ac24da25f73492d479cf847f3d10f74df6
|
Extracted from ArXiv paper 2510.25658v1 (chunk 9)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2510.25658v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:12:41.475267Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181239470090
|
The measured MTE of inner emission signal is sub-thermal at 6 meV, consistent with direct band to vacuum emission from the Boltzmann tail of thermalized electron distribution in the LCB.
|
The measured MTE of inner emission signal is sub-thermal at 6 meV, consistent with direct band to vacuum emission from the Boltzmann tail of thermalized electron distribution in the LCB.
|
[
"Fe:Ga2O3(010) photocathode characterization system",
"Sub-picosecond tunable UV laser system and 10-20kV DC gun-based setup",
"Electron beam profile measured with microchannel plate/phosphor screen detector"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.25722v1
|
https://arxiv.org/abs/2510.25722v1
|
[
"cond-mat.mtrl-sci",
"physics.acc-ph",
"physics.app-ph"
] |
21ecc22bf0f8a2eb64db6efb08c69775e61df418cc72abe5f82ad3ab702536eb
|
Extracted from ArXiv paper 2510.25722v1 (chunk 3)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 3,
"paper_id": "2510.25722v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:12:39.470090Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181256893487
|
The measured spectral photoemission properties of a Fe-doped β-Ga2O3(010) photocathode display an ultracold 6meV MTE contribution to its photoemission in the long transport regime (αl < 1), due to direct emission from the LCB.
|
The measured spectral photoemission properties of a Fe-doped β-Ga2O3(010) photocathode display an ultracold 6meV MTE contribution to its photoemission in the long transport regime (αl < 1), due to direct emission from the LCB.
|
[
"Fe:Ga2O3(010) photocathode",
"Spectral dependence of the QE for this photocathode at 300K",
"Electron energy kBTe ≈ 27meV, consistent with theoretical expectations"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.25722v1
|
https://arxiv.org/abs/2510.25722v1
|
[
"cond-mat.mtrl-sci",
"physics.acc-ph",
"physics.app-ph"
] |
4fd8efaff5424f270a34e89c91b07ed3668da6f8c9087dbd7400c9ea5ccad11c
|
Extracted from ArXiv paper 2510.25722v1 (chunk 8)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 8,
"paper_id": "2510.25722v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:12:56.893487Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181502231560
|
A Langmuir probe system measured broad low-frequency fluctuations in a collision-dominated plasma jet, with notable peaks at ∼2.5 kHz and ∼15 kHz.
|
A Langmuir probe system measured broad low-frequency fluctuations in a collision-dominated plasma jet, with notable peaks at ∼2.5 kHz and ∼15 kHz.
|
[
"Langmuir probe system",
"Sweeping frequency: 100 kHz",
"Voltage range: -40 V to 40 V"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26162v1
|
https://arxiv.org/abs/2510.26162v1
|
[
"physics.plasm-ph"
] |
5d3056d92b18845c85f9160a37ec57142ba514448a46a0733059055bde3b7f29
|
Extracted from ArXiv paper 2510.26162v1 (chunk 5)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 5,
"paper_id": "2510.26162v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:15:02.231560Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181520192568
|
Electron temperature measured at approximately 8 eV near the centerline of the nozzle, with a semi-linear increase in electron density towards the centerline.
|
Electron temperature measured at approximately 8 eV near the centerline of the nozzle, with a semi-linear increase in electron density towards the centerline.
|
[
"Langmuir probe diagnostics on Runs 029 and 030",
"Electron temperature calculation using OML theory (Eq. 5)",
"Average ion saturation current Ii calculated from the characteristic I–V curve"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.26162v1
|
https://arxiv.org/abs/2510.26162v1
|
[
"physics.plasm-ph"
] |
f99f81cda1d128e003040fba622b40b6f248ca1b0732bfbad3934b5248dc8fea
|
Extracted from ArXiv paper 2510.26162v1 (chunk 9)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 9,
"paper_id": "2510.26162v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:15:20.192568Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181542449254
|
Hot spot evolution in inertial confinement fusion plasmas measured using high-resolution x-ray spectroscopy at the National Ignition Facility.
|
Hot spot evolution in inertial confinement fusion plasmas measured using high-resolution x-ray spectroscopy at the National Ignition Facility.
|
[
"National Ignition Facility, W. Hill et al.",
"High-resolution x-ray spectroscopy",
"Hot spot temperature: not explicitly stated"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26162v1
|
https://arxiv.org/abs/2510.26162v1
|
[
"physics.plasm-ph"
] |
f709b7f859f784565b171ce0837c7152c39ea8fbf963ece054a178b68c5230d0
|
Extracted from ArXiv paper 2510.26162v1 (chunk 13)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2510.26162v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:15:42.449789Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_181853318247
|
Higher hydrogen peroxide yields observed in conventional dose-rate irradiations compared to ultra-high dose rate irradiations, except when hydrated electron scavengers are present.
|
Higher hydrogen peroxide yields observed in conventional dose-rate irradiations compared to ultra-high dose rate irradiations, except when hydrated electron scavengers are present.
|
[
"Amplex Red assay",
"6MeV electrons, 4% O2, pH7 under conventional DR vs UHDR",
"Variation of dose rates and instantaneous dose rates in different experiments"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.26928v1
|
https://arxiv.org/abs/2510.26928v1
|
[
"physics.med-ph",
"physics.app-ph",
"physics.bio-ph",
"physics.chem-ph"
] |
042dfd54bdf46d741becd876ab7d1c437b963e7c341c20f766e608981830edd5
|
Extracted from ArXiv paper 2510.26928v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2510.26928v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:18:53.318247Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_182034496379
|
A two-stage nature of a solar flare was observed, with quasi-parallel and semi-circular ribbons exhibiting distinct brightening patterns.
|
A two-stage nature of a solar flare was observed, with quasi-parallel and semi-circular ribbons exhibiting distinct brightening patterns.
|
[
"Multi-wavelength observations from tandem instruments",
"M8.2-class flare on 2023 September 20",
"Two major peaks in the hard X-ray (HXR) light curve"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.27162v1
|
https://arxiv.org/abs/2510.27162v1
|
[
"astro-ph.SR",
"physics.plasm-ph",
"physics.space-ph"
] |
ec7aad6ccb22991ff0727432b8bb46c9accd6547fe981b7c5285378811b3d77e
|
Extracted from ArXiv paper 2510.27162v1 (chunk 0)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 0,
"paper_id": "2510.27162v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:20:34.496379Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_182121141730
|
Relativistic self-focusing and temporal compression of a laser-plasma pulse are observed, leading to a predicted collapse point within the simulated propagation range.
|
Relativistic self-focusing and temporal compression of a laser-plasma pulse are observed, leading to a predicted collapse point within the simulated propagation range.
|
[
"High-intensity laser setup",
"Strong magnetic field with cyclotron resonance",
"Simulated beam width parameter (rf) exhibits nonlinear decent"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2510.27239v2
|
https://arxiv.org/abs/2510.27239v2
|
[
"physics.plasm-ph"
] |
a8254e6c968dbc215f13449867527cd3b11f33a28cfb1133cb0459e500b04ae0
|
Extracted from ArXiv paper 2510.27239v2 (chunk 11)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 11,
"paper_id": "2510.27239v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:21:21.141730Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_182151012897
|
The handedness of tellurium crystals can be determined by the shift in E modes under opposite circularly polarized incident light, with a larger shift observed for the E1 mode.
|
The handedness of tellurium crystals can be determined by the shift in E modes under opposite circularly polarized incident light, with a larger shift observed for the E1 mode.
|
[
"Circularly polarized Raman spectroscopy on three crystal faces",
"Shifts observed in E1 and E2 modes under left- and right-handed light excitation",
"Replicability across different crystals"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2510.27341v1
|
https://arxiv.org/abs/2510.27341v1
|
[
"cond-mat.mtrl-sci",
"cond-mat.mes-hall",
"physics.chem-ph",
"physics.optics"
] |
613535d5b9be9e418127016ed457284db858bb15b89d4f18a41223135807051f
|
Extracted from ArXiv paper 2510.27341v1 (chunk 6)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 6,
"paper_id": "2510.27341v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:21:51.012897Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_182418004877
|
Electrode erosion in Z-pinch device is dominated by sublimation of graphite, with peak pinch current concurrent with high measured carbon erosion.
|
Electrode erosion in Z-pinch device is dominated by sublimation of graphite, with peak pinch current concurrent with high measured carbon erosion.
|
[
"ZaP-HD sheared-flow-stabilized Z-pinch device",
"Campaign-averaged pinch current and erosion measurements at z = 10 cm probe array",
"Sublimation flux calculations: heat flux, surface binding energy (7.4 eV for graphite)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00354v1
|
https://arxiv.org/abs/2511.00354v1
|
[
"physics.plasm-ph"
] |
d102a6eb3e60f526562987d40def6385258dcb38075aa9c9d296e92ff30053ab
|
Extracted from ArXiv paper 2511.00354v1 (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": "2511.00354v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:24:18.004877Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_182420845036
|
Erosion fluxes are at least two orders of magnitude larger than the maximum theoretical sputtered flux, suggesting sublimation is primarily responsible for measured gross electrode erosion.
|
Erosion fluxes are at least two orders of magnitude larger than the maximum theoretical sputtered flux, suggesting sublimation is primarily responsible for measured gross electrode erosion.
|
[
"ZaP-HD sheared-flow-stabilized Z-pinch device",
"Particle flux: 10^22 m^-2s^-1",
"Theoretical sputtered flux limit: 10^19 m^-2s^-1"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.00354v1
|
https://arxiv.org/abs/2511.00354v1
|
[
"physics.plasm-ph"
] |
810c4a07a88f0557a0d74feb1aae45ea8e40e31329e3565cf539f1ed2567cc4f
|
Extracted from ArXiv paper 2511.00354v1 (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": "2511.00354v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:24:20.845036Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_182919641207
|
The accuracy of the OIM remains almost unchanged from 2×2 MIMO up to 90 × 90 MIMO, with some performance drop observed for 100 × 100 MIMO.
|
The accuracy of the OIM remains almost unchanged from 2×2 MIMO up to 90 × 90 MIMO, with some performance drop observed for 100 × 100 MIMO.
|
[
"Fig. 4a (Euclidean distance), Fig. 4b (BER), and Fig. 4c (SP)",
"Conductance range: 1 µS to 60 µS",
"MIMO size: up to 90 × 90"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00479v1
|
https://arxiv.org/abs/2511.00479v1
|
[
"physics.app-ph",
"eess.SY"
] |
2c6017a3906095fb9d60457b7064408cb9a0802b659d05ea179592742dba8060
|
Extracted from ArXiv paper 2511.00479v1 (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": "2511.00479v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:29:19.641733Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_183105871950
|
The measured responsivity of the GeSn photodetector integrated with metasurface is 1.02 mA/W at a wavelength of 1.55 μm and 2.01 mA/W at 2.2 μm
|
The measured responsivity of the GeSn photodetector integrated with metasurface is 1.02 mA/W at a wavelength of 1.55 μm and 2.01 mA/W at 2.2 μm
|
[
"GeSn membrane photodetector, measurement setup in Figure S3",
"Optical power: 1.26 mW",
"Bias voltage: 30 mV"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.00771v2
|
https://arxiv.org/abs/2511.00771v2
|
[
"physics.app-ph",
"physics.optics"
] |
f82e6e564478e21330e1920ee85ea82e09e2dd8546adff6894e991dc11c8c1c9
|
Extracted from ArXiv paper 2511.00771v2 (chunk 15)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2511.00771v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:31:05.871950Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_183735090540
|
Dynamic viscosity of 1-iodonaphthalene + n-alkane mixtures measured at various temperatures with deviations in absolute viscosity determined.
|
Dynamic viscosity of 1-iodonaphthalene + n-alkane mixtures measured at various temperatures with deviations in absolute viscosity determined.
|
[
"Table S2 contains values of density and kinematic viscosity",
"Table 3 lists results on excess molar volumes (E_m_V) and dynamic viscosities (η)",
"Deviations calculated using equation (7)"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.01714v1
|
https://arxiv.org/abs/2511.01714v1
|
[
"physics.chem-ph"
] |
fa66d89686860564981950c9273ab3a0fdd5e6ba9593954c0b147e9775d3007f
|
Extracted from ArXiv paper 2511.01714v1 (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": "2511.01714v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:37:35.090540Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_183947392309
|
The plasma expansion wave in regime(V) can be observed with a characteristic scale of ∆Le,i(t) = λs(t) = Cs0 / γ exp(γt), where λs is the correlation distance and γ is the growth rate.
|
The plasma expansion wave in regime(V) can be observed with a characteristic scale of ∆Le,i(t) = λs(t) = Cs0 / γ exp(γt), where λs is the correlation distance and γ is the growth rate.
|
[
"Eqs.(53) and (54)",
"Profiles for η values of 100 and 900 are plotted in Fig.7",
"The mean solutions obtained by solving Eqs.(53) and (54) are also shown"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02028v1
|
https://arxiv.org/abs/2511.02028v1
|
[
"physics.plasm-ph",
"physics.acc-ph",
"physics.flu-dyn"
] |
c28a9aa5d2ebcc7429c9a5e813397571295092af83029836e49445658e3e5741
|
Extracted from ArXiv paper 2511.02028v1 (chunk 17)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 17,
"paper_id": "2511.02028v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:39:47.392309Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_183914996116
|
The isotope effect in turbulent transport control by GAMs is observed and modeled using gyrokinetic simulations.
|
The isotope effect in turbulent transport control by GAMs is observed and modeled using gyrokinetic simulations.
|
[
"Gyrokinetic simulations, observation in TJ-II stellarator",
"Isotopic scaling laws are broken in turbulent regimes",
"Multi-scale study of the isotope effect"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02070v1
|
https://arxiv.org/abs/2511.02070v1
|
[
"physics.plasm-ph"
] |
2eb2916fd1e101cc9a6eed698516b317f8668f7b133b819105a3f99742f383d7
|
Extracted from ArXiv paper 2511.02070v1 (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": "2511.02070v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:39:14.996116Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_183921817336
|
Nonlinear coupling between small-poloidal wave-number potential fluctuations and turbulent potential fluctuations observed in ohmically heated plasmas
|
Nonlinear coupling between small-poloidal wave-number potential fluctuations and turbulent potential fluctuations observed in ohmically heated plasmas
|
[
"JFT-2M tokamak experiment",
"Ohmically heated plasmas",
"Small-poloidal wave-number potential fluctuations"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.02070v1
|
https://arxiv.org/abs/2511.02070v1
|
[
"physics.plasm-ph"
] |
b896c11bb8f9226e211ce0fbc783be2019296bcffdd01d9a7b5c10a6c04530ac
|
Extracted from ArXiv paper 2511.02070v1 (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": "2511.02070v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:39:21.817336Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184030559994
|
Shearless phase-space transport barriers are observed to survive in high-fidelity gyrokinetic simulations, suppressing radial dispersion across the torus.
|
Shearless phase-space transport barriers are observed to survive in high-fidelity gyrokinetic simulations, suppressing radial dispersion across the torus.
|
[
"gyrokinetic simulations",
"high-fidelity data",
"radial dispersion suppression"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02075v1
|
https://arxiv.org/abs/2511.02075v1
|
[
"physics.plasm-ph"
] |
f9fa4808c8c555105cc168640d54d8ec893566b18994fb664f8fb162f8b2337a
|
Extracted from ArXiv paper 2511.02075v1 (chunk 18)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 18,
"paper_id": "2511.02075v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:40:30.559994Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184306030109
|
Corrected phase noise measured as -102 dBc/Hz at a temperature of 25 °C and offset frequency of 100 kHz
|
Corrected phase noise measured as -102 dBc/Hz at a temperature of 25 °C and offset frequency of 100 kHz
|
[
"NS-132 spectrum analyzer, NEX1 Future",
"Resolution bandwidth: 1 kHz",
"IF amplifier error correction"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02724v1
|
https://arxiv.org/abs/2511.02724v1
|
[
"physics.app-ph",
"eess.SY",
"physics.ins-det"
] |
2a6eb1db67bda385db1d7bf0e447c17154f3ffdc44bfeadd6c3b218e3e1a0de0
|
Extracted from ArXiv paper 2511.02724v1 (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": "2511.02724v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:43:06.030109Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184400995416
|
We developed a suite of codes called FitAik to accurately reproduce and predict measured Einstein coefficients for atomic transitions in lanthanide atoms.
|
We developed a suite of codes called FitAik to accurately reproduce and predict measured Einstein coefficients for atomic transitions in lanthanide atoms.
|
[
"Cowan's suite of codes",
"FitAik interfaced with Cowan codes",
"400 experimental Einstein coefficients from J. E. Lawler’s group"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"cond-mat.quant-gas",
"physics.atom-ph",
"physics.chem-ph",
"physics.optics",
"quant-ph"
] |
85ef71a9da2a4044027d927a5966a1c191a54d004920275d38b045a9173b0923
|
Extracted from ArXiv paper 2511.02890v2 (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": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:44:00.995416Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184548487798
|
Polarizability of Erbium measured with 3-35% uncertainty at three wavelengths (532.26 nm, 1064.5 nm, and 1570.0 nm)
|
Polarizability of Erbium measured with 3-35% uncertainty at three wavelengths (532.26 nm, 1064.5 nm, and 1570.0 nm)
|
[
"Crossed-beam optical dipole trap, focused beam waists from 18 µm to 46 µm",
"Trapping frequencies measured with 1% uncertainty, systematic errors up to 35%",
"Trap frequencies fitted to Eq. (6) for αtot as a function of P and λ"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"cond-mat.quant-gas",
"physics.atom-ph",
"physics.chem-ph",
"physics.optics",
"quant-ph"
] |
6f20fabcb2d30698480d7910dd6fcdb4e3653aba76aa10b39fbdbc631d7fb530
|
Extracted from ArXiv paper 2511.02890v2 (chunk 45)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 45,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:45:48.487798Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184551869776
|
The tensor-to-scalar polarizability ratio of Er atoms in the ground state is measured with a relative change of the light shift at 532.26 nm and 1064.5 nm.
|
The tensor-to-scalar polarizability ratio of Er atoms in the ground state is measured with a relative change of the light shift at 532.26 nm and 1064.5 nm.
|
[
" Ultra-cold Er sample prepared in the lowest Zeeman sublevel (mj = -6)",
" Trap frequencies measured for different values of θp",
" Statistical uncertainties from trapping-frequency measurements"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"cond-mat.quant-gas",
"physics.atom-ph",
"physics.chem-ph",
"physics.optics",
"quant-ph"
] |
410345c176ee5a044eb8d72d25ee1ef5a35b3e7832a453649b474539c7c35519
|
Extracted from ArXiv paper 2511.02890v2 (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": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:45:51.869776Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184600844312
|
The excited-state polarizability of Er atoms in the 583 nm-excited state was measured to be positive for 1064.5 nm and negative for 1570 nm, with a large anisotropy due to the highly anisotropic electronic configuration around the core.
|
The excited-state polarizability of Er atoms in the 583 nm-excited state was measured to be positive for 1064.5 nm and negative for 1570 nm, with a large anisotropy due to the highly anisotropic electronic configuration around the core.
|
[
"Optical dipole trap measurement",
"Resonance frequency shift extracted from data",
"Tensor polarizability coefficients measured for three wavelengths"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"cond-mat.quant-gas",
"physics.atom-ph",
"physics.chem-ph",
"physics.optics",
"quant-ph"
] |
befd8c8359d59ea0a18f44799732866c7843248f2c7db97c3f58ba2639dc1934
|
Extracted from ArXiv paper 2511.02890v2 (chunk 48)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 48,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:46:00.844312Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185017570516
|
Collision rates for two-photon resonance in 23Na39K molecules measured as function of Rabi frequencies and detunings, with largest γ-value of 0.33 at certain conditions.
|
Collision rates for two-photon resonance in 23Na39K molecules measured as function of Rabi frequencies and detunings, with largest γ-value of 0.33 at certain conditions.
|
[
"Ph.D work by Charbel Karam",
"Two-photon resonances at δ = 0 and ∆= 1 GHz",
"Rabi frequencies Ω1 and Ω2 up to 200 MHz"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.02890v2
|
https://arxiv.org/abs/2511.02890v2
|
[
"cond-mat.quant-gas",
"physics.atom-ph",
"physics.chem-ph",
"physics.optics",
"quant-ph"
] |
ab3e79f6674ccdea6b352579759981fadb78616153dae697122185dfe527b144
|
Extracted from ArXiv paper 2511.02890v2 (chunk 126)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 126,
"paper_id": "2511.02890v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:50:17.570516Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184350480039
|
Modulational instability and Alfvén wave packet formation observed in a strong magnetic field, enabling electron acceleration via gyroresonant surfing acceleration.
|
Modulational instability and Alfvén wave packet formation observed in a strong magnetic field, enabling electron acceleration via gyroresonant surfing acceleration.
|
[
"1D PIC simulation of a right-hand circularly polarized wave",
"System size: Lx/(c/ωpe) = 1832",
"Magnetization parameter σ0 = Ω2ce/ω2pe = 6.4 × 103"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03069v1
|
https://arxiv.org/abs/2511.03069v1
|
[
"physics.plasm-ph",
"astro-ph.HE"
] |
d497332e53ef4f87a49ab4a27fdd71c877f63035551957afc39318678409a683
|
Extracted from ArXiv paper 2511.03069v1 (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": "2511.03069v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:43:50.480559Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184447401217
|
Cross-beam energy transfer was observed in direct-drive inertial confinement fusion implosions, achieving 30% reduction in cross-beam energy transfer
|
Cross-beam energy transfer was observed in direct-drive inertial confinement fusion implosions, achieving 30% reduction in cross-beam energy transfer
|
[
"National Ignition Facility, experiments on Direct-Drive ICF",
"Reduction of cross-beam energy transfer: 30%",
"Saturation achieved with wavelength detuning"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03090v1
|
https://arxiv.org/abs/2511.03090v1
|
[
"physics.plasm-ph"
] |
e164839342fd70192b92babc0a4f115572ef06133c886de9e0c64365495e261c
|
Extracted from ArXiv paper 2511.03090v1 (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": "2511.03090v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:44:47.401217Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184549185846
|
Graphene-enabled on-chip THz detector-interferometer achieved sub-wavelength thickness accuracy of ∼5 µm and record-high external responsivity of 73 mA/W
|
Graphene-enabled on-chip THz detector-interferometer achieved sub-wavelength thickness accuracy of ∼5 µm and record-high external responsivity of 73 mA/W
|
[
"Catalan Institute of Nanoscience and Nanotechnology (ICN2) detector",
"Thin films placed in front of the detector-interferometer",
"Predicted thickness accuracy: 10 nm"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03308v1
|
https://arxiv.org/abs/2511.03308v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
e26d73041b586ee7353d187f5971e9dfc344e20d4e65b327a28c851ab8d29ae6
|
Extracted from ArXiv paper 2511.03308v1 (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": "2511.03308v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:45:49.185846Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184557917941
|
A strong photocurrent peak is observed at fpeak = 89 GHz due to positive interference at the graphene location, corresponding to a THz refractive index of nTHz = 3.1.
|
A strong photocurrent peak is observed at fpeak = 89 GHz due to positive interference at the graphene location, corresponding to a THz refractive index of nTHz = 3.1.
|
[
"commercial continuous-wave THz setup",
"free-space wavelength: 3.35 mm",
"cavity length: λ0/4nTHz"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03308v1
|
https://arxiv.org/abs/2511.03308v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
7acc8bd9a24d43efec12219de4dd9790738f30b01e5f6b300dfba7be5ca781b5
|
Extracted from ArXiv paper 2511.03308v1 (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": "2511.03308v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:45:57.917941Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184601646550
|
We observe periodic peaks in photocurrent due to interference effects caused by an external cavity between the detector and THz source, with a periodicity matching λ0/2.
|
We observe periodic peaks in photocurrent due to interference effects caused by an external cavity between the detector and THz source, with a periodicity matching λ0/2.
|
[
"Periodic peaks observed around central frequency",
"Periodicity: 1.79 mm for 89 GHz light, 0.98 mm for 160 GHz light (close to λ0/2)",
"Interference pattern matches intensity of electric field at graphene position"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03308v1
|
https://arxiv.org/abs/2511.03308v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
f462645d5828e93c95f99187f16309f5b6c3aed1b8f7032b4d17d46c9e8be740
|
Extracted from ArXiv paper 2511.03308v1 (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": "2511.03308v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:46:01.646550Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184609580876
|
THz detector-interferometer measures thicknesses of materials with ±10% accuracy using phase sensitivity
|
THz detector-interferometer measures thicknesses of materials with ±10% accuracy using phase sensitivity
|
[
"THz source and detector, graphene channel",
"Photocurrent interference patterns vs position x",
"Refractive indices: Si ≈3.5, paper ≈1.6, Kapton ≈1.8"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.03308v1
|
https://arxiv.org/abs/2511.03308v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
2dcfb0f3fc9244fde1c7f456bb13d275f6d8c2a3bd09949b4679d20dc5ea4663
|
Extracted from ArXiv paper 2511.03308v1 (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": "2511.03308v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:46:09.580876Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184612612848
|
The thickness accuracy of thin films measured with deep sub-wavelength precision using a graphene-based detector-interferometer, achieving the highest accuracy for silicon with a few micrometers.
|
The thickness accuracy of thin films measured with deep sub-wavelength precision using a graphene-based detector-interferometer, achieving the highest accuracy for silicon with a few micrometers.
|
[
"Graphene-based detector-interferometer, THz dipolar antenna, and vertical optical cavity",
"Thickness accuracy: a few micrometers",
"Refractive index dependent thickness error bars"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03308v1
|
https://arxiv.org/abs/2511.03308v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
b4260d72c1bd027bc3eb2da015e92b7524f5005ec4997c4cfa29fd982466025a
|
Extracted from ArXiv paper 2511.03308v1 (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": "2511.03308v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:46:12.612848Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184615993076
|
We measure the detector responsivity for our experimental THz spot size to be Rext = IPTE/Pin, with peak-to-peak value of the demodulated PTE photocurrent signal measured at 2√2π/4Ilock-in
|
We measure the detector responsivity for our experimental THz spot size to be Rext = IPTE/Pin, with peak-to-peak value of the demodulated PTE photocurrent signal measured at 2√2π/4Ilock-in
|
[
"Terascan 1550 terahertz spectroscopy system",
"Peak power: 7.6 µW at 89 GHz",
"Lock-in amplifier detection with reference frequency 39.7 kHz"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03308v1
|
https://arxiv.org/abs/2511.03308v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
f4d905b3d35607799bd52ce47bada53f1e056e817d278571f9121443a2877ecd
|
Extracted from ArXiv paper 2511.03308v1 (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": "2511.03308v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:46:15.993076Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_184718617958
|
No significant reduction in turbulent transport observed when increasing toroidal rotation and its radial gradient by nearly a factor of four at ρtor = 0.6
|
No significant reduction in turbulent transport observed when increasing toroidal rotation and its radial gradient by nearly a factor of four at ρtor = 0.6
|
[
"GENE simulations using the electrostatic limit",
"Toroidal rotation profiles based on QuaLiKiz and Chrystal's model [76]",
"Linear growth rates of drift-wave modes and zonal flow shearing rates"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.03336v1
|
https://arxiv.org/abs/2511.03336v1
|
[
"physics.plasm-ph"
] |
89d9f32ed77561800ce4b4b8c68cddf480177f19ebfa46b25d3a67c294a9755a
|
Extracted from ArXiv paper 2511.03336v1 (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": "2511.03336v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:47:18.617958Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185129372962
|
Improved core confinement is observed in shot #93890, with ITB present in the ion temperature profile, and elevated peak core-ion temperature following fishbone excitation.
|
Improved core confinement is observed in shot #93890, with ITB present in the ion temperature profile, and elevated peak core-ion temperature following fishbone excitation.
|
[
"EAST discharge #93890",
"5000 ms data sample",
"ITB formation due to fishbone excitation"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.04051v1
|
https://arxiv.org/abs/2511.04051v1
|
[
"physics.plasm-ph"
] |
9cda0fe5ab07bbf391a3b583d4bcf8e02128bde90831e8dc532824135f0220e5
|
Extracted from ArXiv paper 2511.04051v1 (chunk 2)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 2,
"paper_id": "2511.04051v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:51:29.372962Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185440792664
|
The nonresonant SABRE mechanism is observed to directly and efficiently produce two-spin z order in the target ligand.
|
The nonresonant SABRE mechanism is observed to directly and efficiently produce two-spin z order in the target ligand.
|
[
"SABRE experiments on 15N-pyridine with polarization at 0.5 μT",
"Signal growth at later times in off-resonance conditions",
"Comparable antiphase signals at three different lab locations without shielding"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.04851v1
|
https://arxiv.org/abs/2511.04851v1
|
[
"physics.chem-ph"
] |
e9942e8049b8940b0baa62856bb705833bcb9cf0ae7d1eed3d21a24603927818
|
Extracted from ArXiv paper 2511.04851v1 (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": "2511.04851v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:54:40.792664Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185547994586
|
Asymmetric visible pulse generated by a Fabry–Pérot etalon was characterized with good agreement between experimentally measured and simulated cross-correlation
|
Asymmetric visible pulse generated by a Fabry–Pérot etalon was characterized with good agreement between experimentally measured and simulated cross-correlation
|
[
"air-spaced Fabry–Pérot etalon",
"IR pulse",
"GaAs substrate"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.04965v1
|
https://arxiv.org/abs/2511.04965v1
|
[
"physics.optics",
"cond-mat.mes-hall",
"physics.chem-ph"
] |
812d695ece7cfc505e09f6551eb8a1a54c65229f4c4e22526d57ceff2cc78733
|
Extracted from ArXiv paper 2511.04965v1 (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": "2511.04965v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:55:47.994586Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185835259294
|
The phase velocity of surface acoustic waves on hBN/SiO2 substrate is measured to decrease with increasing wave vector k
|
The phase velocity of surface acoustic waves on hBN/SiO2 substrate is measured to decrease with increasing wave vector k
|
[
"Hilbert transform applied to spatial spectra of SAW pulses",
"Comparison of phase velocities at different times (T, 2T, 3T)",
"Phase velocity vph(k) determined for k-dependent phase velocity"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05703v1
|
https://arxiv.org/abs/2511.05703v1
|
[
"cond-mat.mtrl-sci",
"cond-mat.mes-hall",
"physics.app-ph",
"physics.optics"
] |
4fe3b1ecdb9a59540013e8c58efdea77c427fe59747cc673491f5366a7b15294
|
Extracted from ArXiv paper 2511.05703v1 (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": "2511.05703v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:58:35.259294Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185912555013
|
Li loss on anode side observed during cyclic aging, resulting in reduced Li accessibility and increased delithiation of the cathode.
|
Li loss on anode side observed during cyclic aging, resulting in reduced Li accessibility and increased delithiation of the cathode.
|
[
"NCM cathode analysis",
"Lattice parameters show unit cell contraction and c parameter decrease with extended aging.",
"Li loss estimated at -34% relative decrease of a parameter movement from SOH100 to SOH70."
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.05892v1
|
https://arxiv.org/abs/2511.05892v1
|
[
"physics.app-ph"
] |
1eedf4b11f0f0fa987be73d2a418cc160d92856f15299f17eec0d5c97e9972eb
|
Extracted from ArXiv paper 2511.05892v1 (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": "2511.05892v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:59:12.555013Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_185937284896
|
Capacity fade observed during long-term cycling is primarily attributed to microscopic degradation processes within the electrodes.
|
Capacity fade observed during long-term cycling is primarily attributed to microscopic degradation processes within the electrodes.
|
[
"in operando ND and NDP measurements",
"Three representative cells of identical composition analyzed",
"Minor manufacturing inhomogeneities may not be entirely excluded"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.05892v1
|
https://arxiv.org/abs/2511.05892v1
|
[
"physics.app-ph"
] |
42b397980dcca3066b587c788ed3985c192a14f4570b67678dce08181ce96f42
|
Extracted from ArXiv paper 2511.05892v1 (chunk 15)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2511.05892v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T18:59:37.284896Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190034764345
|
Thomson scattering and thermal bremsstrahlung spectra were measured in a plasma with electron temperature T_e = 100 eV and density n_e = 5 × 10^19 m^-3.
|
Thomson scattering and thermal bremsstrahlung spectra were measured in a plasma with electron temperature T_e = 100 eV and density n_e = 5 × 10^19 m^-3.
|
[
"ArXiv Paper 2511.06330v1",
"2560-channel spectroscopic system",
"Thomson scattering, thermal bremsstrahlung spectra"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06330v1
|
https://arxiv.org/abs/2511.06330v1
|
[
"physics.plasm-ph"
] |
d66e9cd17d50c159d9c9c2f3c94086d21ceb4c89a50e7e067982dfeebbdb2dd5
|
Extracted from ArXiv paper 2511.06330v1 (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": "2511.06330v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:00:34.764345Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190143394143
|
Anomalous enhancement of yield strength due to static friction is observed for high-friction coefficients, indicating a different treatment is necessary in the high-friction regime
|
Anomalous enhancement of yield strength due to static friction is observed for high-friction coefficients, indicating a different treatment is necessary in the high-friction regime
|
[
"DEM simulations with knr/mg = 102",
"High-friction coefficient (µ ≳0.8) causes breakdown of perturbative solution",
"Non-destructive behavior emerges even in elastic case"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06807v1
|
https://arxiv.org/abs/2511.06807v1
|
[
"cond-mat.soft",
"cond-mat.stat-mech",
"physics.app-ph"
] |
1a7757aba122c9d11b24a6fc94d4576a24ac21d5d748fe51fa5b7fc0312c32a7
|
Extracted from ArXiv paper 2511.06807v1 (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": "2511.06807v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:01:43.394143Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190141889737
|
The antiproton plasma temperature was measured to be around 50K with a radius of 1.5mm and Debye length of 0.036mm
|
The antiproton plasma temperature was measured to be around 50K with a radius of 1.5mm and Debye length of 0.036mm
|
[
"Tracking Scintillator detector",
"Radial distribution of plasma particles",
"Peak position accuracy: 0.03m in axial coordinate z"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.06883v1
|
https://arxiv.org/abs/2511.06883v1
|
[
"physics.atom-ph",
"hep-ex",
"physics.plasm-ph"
] |
8fbbf8ff26e405c62b98833f3365781235ef20c10e7e8529596f1e177627af5f
|
Extracted from ArXiv paper 2511.06883v1 (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": "2511.06883v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:01:41.889737Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190259272238
|
The lithospheric contribution to the geoneutrino signal at JUNO is predominantly influenced by the Local Crust within a few hundred kilometers of the detector, accounting for 40-80% of the signal.
|
The lithospheric contribution to the geoneutrino signal at JUNO is predominantly influenced by the Local Crust within a few hundred kilometers of the detector, accounting for 40-80% of the signal.
|
[
"JUNO detector in South China",
"Local Crust (LOC) has a larger impact on prediction compared to Rest Of the Crust (ROC) and Continental Lithospheric Mantle (CLM)",
"40-80% influence from LOC"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.07227v1
|
https://arxiv.org/abs/2511.07227v1
|
[
"hep-ex",
"physics.geo-ph"
] |
841233d19492813669e77cb457c0d3cbdeca2361b8d37e13c3a71d547988009d
|
Extracted from ArXiv paper 2511.07227v1 (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": "2511.07227v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:02:59.272238Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190602006845
|
We observed second harmonic ultrasound generation by MNPs under EMF for the first time, linked to their magnetic properties and presence of a magnetic field gradient
|
We observed second harmonic ultrasound generation by MNPs under EMF for the first time, linked to their magnetic properties and presence of a magnetic field gradient
|
[
"piezoelectric transducers",
"magnetic flux densities up to 65 mT",
"f = 800 kHz"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.08146v2
|
https://arxiv.org/abs/2511.08146v2
|
[
"physics.app-ph",
"cond-mat.mes-hall"
] |
a3b7ec9a75dab29c4a3ccc54e42eef0226bc7ebf7bb3e64d5288adf64414687d
|
Extracted from ArXiv paper 2511.08146v2 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2511.08146v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:06:02.006845Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190608727881
|
Second harmonic ultrasonic signal generation observed under isothermal MHz RF excitation, confirmed by magneto-acoustic interaction origin
|
Second harmonic ultrasonic signal generation observed under isothermal MHz RF excitation, confirmed by magneto-acoustic interaction origin
|
[
"M5Stack microcontroller controlled duty cycles with amplitude of 65mT at 800kHz",
"Oscilloscope synchronized with auxiliary pick-up coil and filtered using ONDA HFO-690 high pass filter (>2MHz)",
"Temperature fluctuations below 1°C maintained by optic fiber sensor (H201 by Rugged Monitoring)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.08146v2
|
https://arxiv.org/abs/2511.08146v2
|
[
"physics.app-ph",
"cond-mat.mes-hall"
] |
b5af32b03cfed64a1bc3bc8e5cb58a4d04e1220c5da87d2d2dadbadccf47cd55
|
Extracted from ArXiv paper 2511.08146v2 (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": "2511.08146v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:06:08.727881Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190631051245
|
Distinct changes in magnetic domain shape, size and density were observed under varying voltage inputs
|
Distinct changes in magnetic domain shape, size and density were observed under varying voltage inputs
|
[
"Mackey-Glass voltage inputs",
"MOKE microscopy frames captured at 16 fps",
"Reservoir state vectors generated from video frames"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08346v1
|
https://arxiv.org/abs/2511.08346v1
|
[
"physics.app-ph"
] |
3d51fbdd68059cc6aec1084ebb6be92d0873e3cd3a22fa7947529e723f68654e
|
Extracted from ArXiv paper 2511.08346v1 (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": "2511.08346v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:06:31.051245Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190649275327
|
The nutation angle induced by the detection pulse modulates the apparent relaxation rates measured through individual peaks at ultralow fields.
|
The nutation angle induced by the detection pulse modulates the apparent relaxation rates measured through individual peaks at ultralow fields.
|
[
"Quantum magnetometers, not classical induction coils",
"Nutation profiles were fitted with a mono-exponential function S(ts) = A exp(−R1 ts)",
"Measurement field of B0 = 0.1 µT or 5 µT"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08517v1
|
https://arxiv.org/abs/2511.08517v1
|
[
"physics.chem-ph",
"physics.atom-ph"
] |
4b6edd63c0044a87c6698cebe24de0235e481fe4205b2f8bfe34f35f059850ec
|
Extracted from ArXiv paper 2511.08517v1 (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": "2511.08517v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:06:49.275327Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190715213358
|
Relaxation rates of [13CH3] system populations and coherences measured at ultralow field, with clear segregation into low-energy and high-energy manifolds
|
Relaxation rates of [13CH3] system populations and coherences measured at ultralow field, with clear segregation into low-energy and high-energy manifolds
|
[
"QuSpin magnetometer (QZFM Gen-2)",
"Pulse amplitude: Bp = 30.64 µT",
"Detection performed by one channel of QuSpin magnetometer along the y-axis"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08517v1
|
https://arxiv.org/abs/2511.08517v1
|
[
"physics.chem-ph",
"physics.atom-ph"
] |
da3583537b3a5fd535826562253e8ab5d0edf643b47f152ea08893ac0de51d36
|
Extracted from ArXiv paper 2511.08517v1 (chunk 15)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 15,
"paper_id": "2511.08517v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:07:15.213358Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190715908991
|
Charge transfer rates measured to exhibit two distinct behaviors with respect to donor-acceptor energy gap, influenced by dissipation rate and bath temperature.
|
Charge transfer rates measured to exhibit two distinct behaviors with respect to donor-acceptor energy gap, influenced by dissipation rate and bath temperature.
|
[
"Theoretical predictions using Eq. (1) with γ ≪ω and γ ≪kBT",
"Experimental results from resampling [40]",
"Dissipation rates: γ = 0.0360ω"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08689v1
|
https://arxiv.org/abs/2511.08689v1
|
[
"quant-ph",
"cond-mat.quant-gas",
"physics.atom-ph",
"physics.chem-ph"
] |
7c40f39ed382aa210f29c50b5789d78159967b4e8c0626011d2addca102d2ab4
|
Extracted from ArXiv paper 2511.08689v1 (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": "2511.08689v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:07:15.908991Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190919819607
|
Spin-polarization of lepton beams and emitted photons is accurately reproduced using spin- and polarization-resolved QED code, with average positron polarization measured as 57.9% and average lepton spin polarization measured as 8.8%
|
Spin-polarization of lepton beams and emitted photons is accurately reproduced using spin- and polarization-resolved QED code, with average positron polarization measured as 57.9% and average lepton spin polarization measured as 8.8%
|
[
"OSIRIS simulation",
"2D particle-in-cell simulation",
"Comparison to reference paper [48]"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.08929v1
|
https://arxiv.org/abs/2511.08929v1
|
[
"physics.plasm-ph",
"physics.comp-ph"
] |
fa5d3bece0ba4da25873f269472d35d2ece1bbde1be9b7856ff524494b43f75c
|
Extracted from ArXiv paper 2511.08929v1 (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": "2511.08929v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:09:19.819607Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190908321578
|
Energy separation between K and Q valleys (∆EQK) under biaxial strain is measured as 234 meV/%ε for MoS2, 211 meV/%ε for MoSe2, and 278 meV/%ε for WS2.
|
Energy separation between K and Q valleys (∆EQK) under biaxial strain is measured as 234 meV/%ε for MoS2, 211 meV/%ε for MoSe2, and 278 meV/%ε for WS2.
|
[
"First-principles calculations",
"MoS2, MoSe2, WS2 materials under biaxial strain",
"Energy separation ∆EQK measured at different strains"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.08975v1
|
https://arxiv.org/abs/2511.08975v1
|
[
"physics.app-ph"
] |
d64ce76ef819144832aedb0275ca75e84caaa97a229e150913431338a587795f
|
Extracted from ArXiv paper 2511.08975v1 (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": "2511.08975v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:09:08.322107Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190932463142
|
A notable drop in maser peak power is observed between 0 cm and 5 cm separation, corresponding to the transition from guided signal delivery to radiative free-space propagation.
|
A notable drop in maser peak power is observed between 0 cm and 5 cm separation, corresponding to the transition from guided signal delivery to radiative free-space propagation.
|
[
"Patch antenna used (patch width D ≈ 75 mm)",
"Distance across free space: 0-25 cm",
"SNR values remain above 20 dBc at all separations"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09059v1
|
https://arxiv.org/abs/2511.09059v1
|
[
"physics.app-ph"
] |
999588eb3fdb2d355c0c7fd2dd364e84c93baed3b5fba6e68c8708f756bad2b0
|
Extracted from ArXiv paper 2511.09059v1 (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": "2511.09059v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:09:32.463658Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_190946341919
|
Frequency-domain vacuum Rabi splitting observed via FFT analysis with measured values of 1.0681 MHz for Pc:PTP and 2.136 MHz for DAP:PTP, remaining spectrally invariant across environments
|
Frequency-domain vacuum Rabi splitting observed via FFT analysis with measured values of 1.0681 MHz for Pc:PTP and 2.136 MHz for DAP:PTP, remaining spectrally invariant across environments
|
[
"Pc:PTP and DAP:PTP devices",
"Cavity decay rate (𝜅𝑐) calculated as 0.181 MHz and 0.185 MHz respectively",
"Cooperativity ranges of C∗ ∈ [403 − 1063] for Pc:PTP and C∗ ∈ [395 −1043] for DAP:PTP"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.09059v1
|
https://arxiv.org/abs/2511.09059v1
|
[
"physics.app-ph"
] |
d60687abd9bcda2df515212da9c2c6969823987bd26c4eb8d9388e346c16906f
|
Extracted from ArXiv paper 2511.09059v1 (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": "2511.09059v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:09:46.341919Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_191100329061
|
Quantum dot photoluminescence spectral shift measured up to 5.6 nm in coated CBGs and 2.4 nm in uncoated CBGs under piezoelectric actuation.
|
Quantum dot photoluminescence spectral shift measured up to 5.6 nm in coated CBGs and 2.4 nm in uncoated CBGs under piezoelectric actuation.
|
[
"Coated CBGs on a piezoelectric substrate with Al₂O₃ layer",
"Devices layout and SEM images presented in Figure 1",
"Spectral tuning range measured up to 37 kV/cm"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.09155v1
|
https://arxiv.org/abs/2511.09155v1
|
[
"cond-mat.mtrl-sci",
"physics.app-ph",
"quant-ph"
] |
bf46e66e45050ceb134571e15934c6086302636e41a672f592a3c1ed087efaab
|
Extracted from ArXiv paper 2511.09155v1 (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": "2511.09155v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:11:00.329061Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_191712671636
|
Shock formation and decay observed in solid-density plasmas with few-nanometre precision after irradiation by intense short-pulse laser.
|
Shock formation and decay observed in solid-density plasmas with few-nanometre precision after irradiation by intense short-pulse laser.
|
[
"LCLS end station, Matter in Extreme Conditions",
"45 fs, 0.9 J pulses at 3.5 × 10^19 W/cm2",
"XRM visualizes compression and ablation with ∼200 nm resolution"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10127v1
|
https://arxiv.org/abs/2511.10127v1
|
[
"physics.plasm-ph"
] |
b87b4a978c684731537c4bf2365856ee4b629efa914f47b76190ba0b1391b428
|
Extracted from ArXiv paper 2511.10127v1 (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": "2511.10127v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:17:12.671636Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_191733092032
|
The shock formation time is estimated to be approximately 18 ± 3 ps, matching the observed SAXS evolution and supporting a nonlinear steepening of an initially smooth compression wave.
|
The shock formation time is estimated to be approximately 18 ± 3 ps, matching the observed SAXS evolution and supporting a nonlinear steepening of an initially smooth compression wave.
|
[
"XRM and SAXS analysis",
"Temperature profile and sound-speed gradient measurements",
"Estimated breaking time tsh ≈18±3 ps"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10127v1
|
https://arxiv.org/abs/2511.10127v1
|
[
"physics.plasm-ph"
] |
32f255e941aa40a8918c900bad633badf846844de670a7f2a08131a84c1fc053
|
Extracted from ArXiv paper 2511.10127v1 (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": "2511.10127v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:17:33.092032Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_191944160899
|
Antenna near-fields and k-weighting measured for stripline and CPW exciters in YIG film with approximately equal return splits and three-peak profiles.
|
Antenna near-fields and k-weighting measured for stripline and CPW exciters in YIG film with approximately equal return splits and three-peak profiles.
|
[
"GGB 40A probes, Anritsu MS4642B VNA",
"Applied RF power: -25 dBm",
"Bias field up to 900 mT"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10346v1
|
https://arxiv.org/abs/2511.10346v1
|
[
"cond-mat.mes-hall",
"physics.app-ph"
] |
47ffc5406abfba23a91f6c061f6adb788f215df73e7f8b9b821187c21d989808
|
Extracted from ArXiv paper 2511.10346v1 (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": "2511.10346v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:19:44.160899Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192052505477
|
The PVC substrate's viscoelastic parameters were measured and modeled, allowing for simulation of microstructural deformation during thermoforming.
|
The PVC substrate's viscoelastic parameters were measured and modeled, allowing for simulation of microstructural deformation during thermoforming.
|
[
"Dynamic mechanical analysis (ARES-G2, TA Instruments) with 2° cone-plate geometry",
"Angular frequency sweeps conducted over 0.3-100 rad/s",
"Fitted using MCalibration software based on a linear elastic model"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10447v1
|
https://arxiv.org/abs/2511.10447v1
|
[
"physics.optics",
"physics.app-ph"
] |
a9c2e512704392088cf8daf6328fdab9aced02dd42f915378bb586a693918329
|
Extracted from ArXiv paper 2511.10447v1 (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": "2511.10447v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:20:52.505477Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192133032823
|
Atomic alignment of O I levels is highly sensitive to elastic collision rates and magnetic fields, with significant effects observed at densities above 10^15 cm^-3.
|
Atomic alignment of O I levels is highly sensitive to elastic collision rates and magnetic fields, with significant effects observed at densities above 10^15 cm^-3.
|
[
"Differential cross-section measurements for H-O collisions",
"Hydrogen density range: 10^14 - 5*10^16 cm^-3",
"Magnetic field strength up to 100 G"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10476v1
|
https://arxiv.org/abs/2511.10476v1
|
[
"astro-ph.SR",
"physics.atom-ph",
"physics.plasm-ph"
] |
da4dfd7f83cf65416718a7f74fddd39a84c70f469e86c453a938dd9a10369b35
|
Extracted from ArXiv paper 2511.10476v1 (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": "2511.10476v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:21:33.032823Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192205559132
|
Acoustic particle velocity within the chip frame was measured to be 2.4 mm/s at 100 Hz with an acoustic pressure of 1 Pa, corresponding to a planar-wave particle velocity.
|
Acoustic particle velocity within the chip frame was measured to be 2.4 mm/s at 100 Hz with an acoustic pressure of 1 Pa, corresponding to a planar-wave particle velocity.
|
[
"finite element analysis (FEA), Fig. 2a,b",
"acoustic pressure: 1 Pa",
"particle velocity: 2.4 mm/s"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10830v1
|
https://arxiv.org/abs/2511.10830v1
|
[
"physics.flu-dyn",
"physics.app-ph"
] |
80a26650ad8f1c72839d98ab2a0c85559fb4490f5ed908fb666fdcdac6d4297b
|
Extracted from ArXiv paper 2511.10830v1 (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": "2511.10830v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:22:05.559132Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192157985642
|
Two 5-minute oscillation events were observed in the solar wind by PSP, with significances of 5.8σ and 6.2σ, respectively.
|
Two 5-minute oscillation events were observed in the solar wind by PSP, with significances of 5.8σ and 6.2σ, respectively.
|
[
"Parker Solar Probe (PSP) observations within ±7 days of perihelion",
"Interval from 09:50 to 12:05 UTC on 2024-12-24",
"Significant peaks around 3.2 mHz in rectified trace magnetic field power spectral density (PSD)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10906v1
|
https://arxiv.org/abs/2511.10906v1
|
[
"astro-ph.SR",
"physics.plasm-ph",
"physics.space-ph"
] |
335701833ccfc3e99ebe497d277689586d65597a5070b893d89f3b9e24c4e3ec
|
Extracted from ArXiv paper 2511.10906v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2511.10906v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:21:57.985642Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192208936082
|
The first definitive in situ evidence of 5-minute oscillations in the upper solar corona and primordial solar wind was observed by Parker Solar Probe.
|
The first definitive in situ evidence of 5-minute oscillations in the upper solar corona and primordial solar wind was observed by Parker Solar Probe.
|
[
"Parker Solar Probe (PSP) data from E22 event",
"Wave train lasted approximately 35 minutes, consistent with remote sensing data",
"Oscillations remained in-phase over about 3.5 degrees in Carrington longitude"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10906v1
|
https://arxiv.org/abs/2511.10906v1
|
[
"astro-ph.SR",
"physics.plasm-ph",
"physics.space-ph"
] |
c545e18c602897e9b99ddf8f7909459319e615cd04054a14f7d74f7dbd5e1af4
|
Extracted from ArXiv paper 2511.10906v1 (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": "2511.10906v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:22:08.936082Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192220962493
|
Parker Solar Probe observed 5-minute oscillations in the solar wind, providing in situ evidence of Alfvénic fluctuations.
|
Parker Solar Probe observed 5-minute oscillations in the solar wind, providing in situ evidence of Alfvénic fluctuations.
|
[
"FIELDS instrument suite magnetic field data",
"SPAN-i and SPAN-a plasma moments data",
"Quasi-Thermal-Noise (QTN) spectroscopy electron number density"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.10906v1
|
https://arxiv.org/abs/2511.10906v1
|
[
"astro-ph.SR",
"physics.plasm-ph",
"physics.space-ph"
] |
5e45fb2e27b9dac9ae7a0856e8e5b17d2fb0669f79f1fbd93becf59d6becb214
|
Extracted from ArXiv paper 2511.10906v1 (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": "2511.10906v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:22:20.962493Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192246172721
|
Electron density changes were measured via time-resolved Langmuir probe in RF-CCP dusty plasma, with electron photodetachment caused by a Nd:YAG laser beam
|
Electron density changes were measured via time-resolved Langmuir probe in RF-CCP dusty plasma, with electron photodetachment caused by a Nd:YAG laser beam
|
[
"RF compensated single Langmuir probe (114.3 μm radius), Siglent SDS 2354X HD oscilloscope (350 MHz, 2 Gs/s)",
"Laser beam energy varied between 2-75 mJ",
"Probe tip kept outside plasma region during growth phase and biased -20V to repel negatively charged dust particles"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.10956v1
|
https://arxiv.org/abs/2511.10956v1
|
[
"physics.plasm-ph"
] |
ed49d817ae16efd3ac7d19faa26d9ec1638078b171ed74be08c340cc3597e8d8
|
Extracted from ArXiv paper 2511.10956v1 (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": "2511.10956v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:22:46.172721Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192349615587
|
Broadband lasers reduce SBS reflectivity in high-Z Au plasmas, contrary to low-Z systems where mitigation effects were observed.
|
Broadband lasers reduce SBS reflectivity in high-Z Au plasmas, contrary to low-Z systems where mitigation effects were observed.
|
[
"EPOCH PIC simulations",
"Au plasma with 0.3 nc electron density",
"1000 macro-particles per cell for electrons"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.11395v1
|
https://arxiv.org/abs/2511.11395v1
|
[
"physics.plasm-ph"
] |
26959106ac119ac4d8376e202ff44c23d566551438ce925c288ea629c81c947f
|
Extracted from ArXiv paper 2511.11395v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2511.11395v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:23:49.615587Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192429794589
|
The sensitivity of the sensor scales with 1/√R and can be improved by increasing optical power, using low-noise photodiodes, or detecting the signal with single-photon detectors.
|
The sensitivity of the sensor scales with 1/√R and can be improved by increasing optical power, using low-noise photodiodes, or detecting the signal with single-photon detectors.
|
[
"CW-ODMR measurements",
"Sensitivity improvement observed in Fig. 2f",
"Optical power scaling"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.11496v1
|
https://arxiv.org/abs/2511.11496v1
|
[
"quant-ph",
"physics.app-ph",
"physics.optics"
] |
69167d723b074d7391e1c758902bba4cd55dbb3ff64d954ae71a2d601fc8bf77
|
Extracted from ArXiv paper 2511.11496v1 (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": "2511.11496v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:24:29.794589Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192435104056
|
A 40% contrast in MW reflection from the sensor head is measured, comparable to spin-ensemble readout contrasts of 1%-2%
|
A 40% contrast in MW reflection from the sensor head is measured, comparable to spin-ensemble readout contrasts of 1%-2%
|
[
"MW signal at frequency ωd",
"Signal generator and IQ mixer setup",
"Digitized I and Q outputs"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.11561v1
|
https://arxiv.org/abs/2511.11561v1
|
[
"quant-ph",
"cond-mat.mes-hall",
"physics.app-ph",
"physics.atom-ph"
] |
666d444111ebece98f41b3887725a2968048ec66dc8fcec86b691245a157aecc
|
Extracted from ArXiv paper 2511.11561v1 (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": "2511.11561v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:24:35.104056Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192447514319
|
The sensor achieved a thermal noise limit of 2 pT/√Hz, with measured sensitivities of 5.3 nT/√Hz to 250 pT/√Hz for different NV orientations.
|
The sensor achieved a thermal noise limit of 2 pT/√Hz, with measured sensitivities of 5.3 nT/√Hz to 250 pT/√Hz for different NV orientations.
|
[
"Simulations",
"NV orientations 1, 2, and 3",
"Thermal noise limit: 2 pT/√Hz"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.11561v1
|
https://arxiv.org/abs/2511.11561v1
|
[
"quant-ph",
"cond-mat.mes-hall",
"physics.app-ph",
"physics.atom-ph"
] |
b1d1f39bc4cbe1c58885761551ccbd19de40a57bc99ad8e49448f0b7ff0fc0dc
|
Extracted from ArXiv paper 2511.11561v1 (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": "2511.11561v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:24:47.514319Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192704483580
|
Compressive moduli of polymers were measured using a TA Instrument ARES-G2 rheometer, with epoxy resin having a compressive modulus of 5.3 MPa ± 0.2 and PDMS-UCNP films showing a non-linear increase in compressive modulus up to 150 nN
|
Compressive moduli of polymers were measured using a TA Instrument ARES-G2 rheometer, with epoxy resin having a compressive modulus of 5.3 MPa ± 0.2 and PDMS-UCNP films showing a non-linear increase in compressive modulus up to 150 nN
|
[
"TA Instrument ARES-G2 rheometer",
"25 mm stainless steel plate, flat parallel geometry",
"Polymer samples prepared by mixing and curing"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.11858v1
|
https://arxiv.org/abs/2511.11858v1
|
[
"physics.app-ph"
] |
7947de37a4dd5edded079ac26d38bf109e396ec58719def4e1fb79f38ee7203a
|
Extracted from ArXiv paper 2511.11858v1 (chunk 13)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 13,
"paper_id": "2511.11858v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:27:04.483580Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_192827807930
|
We measured the electric field within a plasma sheath with spatial resolution of 30 µm and sensitivity exceeding 1 V/cm.
|
We measured the electric field within a plasma sheath with spatial resolution of 30 µm and sensitivity exceeding 1 V/cm.
|
[
"Rubidium vapor added to argon plasma",
"Two-photon nonlinear process: electromagnetically induced transparency (EIT)",
"Fluorescence collected from illuminated region"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.12322v1
|
https://arxiv.org/abs/2511.12322v1
|
[
"physics.plasm-ph",
"physics.app-ph",
"physics.atom-ph",
"physics.optics",
"quant-ph"
] |
cedfe0c0ee88d737fcdfa40f46408785409ab19a1228ed1b83c991acfaf0cda4
|
Extracted from ArXiv paper 2511.12322v1 (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": "2511.12322v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:28:27.807930Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193045036654
|
Robust magnetic ordering observed in the edge state of zigzag graphene nanoribbons embedded in hexagonal boron nitride, with a large magnetoresistance ratio of ~1.3%.
|
Robust magnetic ordering observed in the edge state of zigzag graphene nanoribbons embedded in hexagonal boron nitride, with a large magnetoresistance ratio of ~1.3%.
|
[
"Scanning NV center microscopy",
"Magneto-transport measurements at 4 Kelvin",
"Magnetoresistance ratio: ~1.3%"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.13075v1
|
https://arxiv.org/abs/2511.13075v1
|
[
"cond-mat.mes-hall",
"cond-mat.mtrl-sci",
"physics.app-ph"
] |
51a9fb981eb220727a59dfaad23d631ebddb7c2af4cef85dfbad72bae3668d2c
|
Extracted from ArXiv paper 2511.13075v1 (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": "2511.13075v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:30:45.036654Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193402874192
|
IR pre-excitation slows down CF3I dissociation process, with a significant delay observed when IR pulse is followed by UV pulse
|
IR pre-excitation slows down CF3I dissociation process, with a significant delay observed when IR pulse is followed by UV pulse
|
[
"Table-top keV-UED instrument",
"150 fs temporal resolution",
"800 nm-wavelength IR laser beam"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.13479v1
|
https://arxiv.org/abs/2511.13479v1
|
[
"physics.chem-ph"
] |
600e3300b82b67535b6ba8a5ce1a7da0fd968c46d6a5382ebc7d148ff6f0029f
|
Extracted from ArXiv paper 2511.13479v1 (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": "2511.13479v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:34:02.874192Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193425361220
|
A dissociation speed of 2.82 ± 0.57 Å/ps was measured for the IR+UV excitation case, significantly slower than the UV-only excitation dissociation speed
|
A dissociation speed of 2.82 ± 0.57 Å/ps was measured for the IR+UV excitation case, significantly slower than the UV-only excitation dissociation speed
|
[
"Experimental ∆PDF∥(𝑟, 𝑡) for IR + UV excitation (Figure 6(b))",
"Peak movement of F-I wavepacket indicates dissociation speed",
"Linear fit to peak center position vs time yields dissociation speed"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.13479v1
|
https://arxiv.org/abs/2511.13479v1
|
[
"physics.chem-ph"
] |
e8276f194883cbfca4c1decbec6ca6cd6b974fd4d80d356d8c2efd2ff4b6a69f
|
Extracted from ArXiv paper 2511.13479v1 (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": "2511.13479v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:34:25.361220Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193429628365
|
The [HNC]/[HCN] abundance ratio was accurately determined from measured absorption spectra to be highly sensitive to parameters such as internal energy relaxation and destruction rates
|
The [HNC]/[HCN] abundance ratio was accurately determined from measured absorption spectra to be highly sensitive to parameters such as internal energy relaxation and destruction rates
|
[
"OFC-FTS setup with mid-infrared frequency comb",
"Effective absorption pathlength of (146.0 ± 0.5) cm",
"Plasma reactor operated at a pressure of (1.00 ± 0.01) mbar, using gas flows and plasma power"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.13519v1
|
https://arxiv.org/abs/2511.13519v1
|
[
"physics.chem-ph",
"physics.plasm-ph"
] |
ef268307205b0545c5a1640b80540f713741e6488b72e037258624541b38c5e3
|
Extracted from ArXiv paper 2511.13519v1 (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": "2511.13519v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:34:29.628365Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193438024730
|
The [HNC]/[HCN] abundance ratio in molecular plasmas was measured to be between (1.15– 2.20) × 10−4, with an agreement within 25 – 30% between EC-QCL and OFC-FTS data.
|
The [HNC]/[HCN] abundance ratio in molecular plasmas was measured to be between (1.15– 2.20) × 10−4, with an agreement within 25 – 30% between EC-QCL and OFC-FTS data.
|
[
"EC-QCL setup",
"OFC-FTS measurements",
"Temporal evolution over 120 minutes"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.13519v1
|
https://arxiv.org/abs/2511.13519v1
|
[
"physics.chem-ph",
"physics.plasm-ph"
] |
355b9c8aa279a376e9c26f64da2229c9e02347486b9656b4721860f2069d700f
|
Extracted from ArXiv paper 2511.13519v1 (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": "2511.13519v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:34:38.024730Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193528625212
|
The response function of the InSb detector is throughput-independent and consistent with detectivity charts for InSb detectors.
|
The response function of the InSb detector is throughput-independent and consistent with detectivity charts for InSb detectors.
|
[
"InSb detector, CW measurements",
"Peak around 2200 cm-1 matches detectivity charts",
"Throughput-independent due to normalization"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.13577v1
|
https://arxiv.org/abs/2511.13577v1
|
[
"physics.optics",
"physics.app-ph"
] |
230c2ae71be11fc35b8aa050ee85dd16e02fca6a44e3aa9a6053f6cdbf68fdf5
|
Extracted from ArXiv paper 2511.13577v1 (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": "2511.13577v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:35:28.625212Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193537041628
|
Average receding bow shock speed measured to be ~19 km/s, with Mach number of ~4.7 for the new shock cycle
|
Average receding bow shock speed measured to be ~19 km/s, with Mach number of ~4.7 for the new shock cycle
|
[
"MMS spacecraft data",
"Bow shock crossings by MMS1, MMS2, and MMS3",
"Ion energy spectra indicating higher fluxes of suprathermal ions in the foreshock"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.13697v1
|
https://arxiv.org/abs/2511.13697v1
|
[
"physics.space-ph",
"physics.plasm-ph"
] |
ca822daa72ea251aeade17f1dea547cf31403ddd2f159f0a9d6c753901c980a2
|
Extracted from ArXiv paper 2511.13697v1 (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": "2511.13697v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:35:37.041628Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193547750591
|
Suprathermal ion densities decrease with distance to the bow shock, but suprathermal ions at MMS1 reach as high as those observed by MMS3
|
Suprathermal ion densities decrease with distance to the bow shock, but suprathermal ions at MMS1 reach as high as those observed by MMS3
|
[
"MMS spacecraft travel at ~2 km/s along the bow shock normal",
"Backstreaming ions abundance decreases with distance",
"Suprathermal ion densities in post-new shock region vary between MMS1 and MMS3 or MMS2"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.13697v1
|
https://arxiv.org/abs/2511.13697v1
|
[
"physics.space-ph",
"physics.plasm-ph"
] |
a215a5f81f808df18c865094d6ed2e4a41dfa218d8a0b6b04d5c599ad381dc04
|
Extracted from ArXiv paper 2511.13697v1 (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": "2511.13697v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:35:47.750591Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193614917142
|
The binding energy between PIM-1 and DNT was calculated to be 75.8 kJ/mol, with a measured value of 73 kJ/mol in excellent agreement.
|
The binding energy between PIM-1 and DNT was calculated to be 75.8 kJ/mol, with a measured value of 73 kJ/mol in excellent agreement.
|
[
"B3LYP-gCP-D3/6-31G(d) functional",
"10U-PIM-1+DNT configuration",
"Experimental binding energy estimated from absorbance changes at 241 nm"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.13938v1
|
https://arxiv.org/abs/2511.13938v1
|
[
"physics.chem-ph",
"cond-mat.mtrl-sci"
] |
84f5c7910e01966b2b09bfe09a1a9881217190b3ba9457dd11816555871449ba
|
Extracted from ArXiv paper 2511.13938v1 (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": "2511.13938v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:36:14.917142Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193828289531
|
Researchers simulated prominence formation using 3D MHD simulations, achieving realistic physical properties and reproducing observed filament morphology.
|
Researchers simulated prominence formation using 3D MHD simulations, achieving realistic physical properties and reproducing observed filament morphology.
|
[
"Xia and Keppens (2016) simulation",
"Prominence densities: ~1.9 × 10^10 cm^-3",
"Temperatures: ~17,500 K"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.14374v1
|
https://arxiv.org/abs/2511.14374v1
|
[
"astro-ph.SR",
"physics.plasm-ph",
"physics.space-ph"
] |
55ed41d82005371175ef121e8ad3896ae9149aad3840d7f616ae3d0942fe7750
|
Extracted from ArXiv paper 2511.14374v1 (chunk 29)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 29,
"paper_id": "2511.14374v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:38:28.289531Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193737158048
|
Microwave-frequency dielectric constant of hexagonal boron nitride (hBN) measured to be 10.5 ± 0.3 with loss tangent tan δ = 2.7 × 10^(-4)
|
Microwave-frequency dielectric constant of hexagonal boron nitride (hBN) measured to be 10.5 ± 0.3 with loss tangent tan δ = 2.7 × 10^(-4)
|
[
"van der Waals parallel-plate capacitor, base temperature 20 mK",
"Transmission coefficient S21 through the feedline of three hanger-type resonators",
"Capacitance CDUT and participation ratio p extracted from circle-fitting of resonance"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.14621v1
|
https://arxiv.org/abs/2511.14621v1
|
[
"quant-ph",
"cond-mat.supr-con",
"physics.app-ph"
] |
643beab2fb8ad389a980db46d82e8407774305747a1964f7177fb9a6c11874c1
|
Extracted from ArXiv paper 2511.14621v1 (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": "2511.14621v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:37:37.158048Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_193957123841
|
Spin-pumping effect in ferromagnetic thin films was observed due to inverse orbital Hall effect (IOHE) in neighboring Ti thin film with weak SOC.
|
Spin-pumping effect in ferromagnetic thin films was observed due to inverse orbital Hall effect (IOHE) in neighboring Ti thin film with weak SOC.
|
[
"Ti/Co bilayers studied with varying thickness of Ti",
"Damping variation measured using Ferromagnetic resonance (FMR)",
"Orbital current accumulated in Ti layer measured by magneto-optical Kerr effect (MOKE)"
] | 0.85
|
high
|
universal
|
physics
|
arxiv
|
2511.15307v1
|
https://arxiv.org/abs/2511.15307v1
|
[
"physics.app-ph"
] |
ab1cc7c1ad75ed2b67d606c738a9beb884a211cb7454149ea86882a9f3bb0762
|
Extracted from ArXiv paper 2511.15307v1 (chunk 1)
|
[
"experimental_physics",
"measurement"
] |
llama3.1:8b-instruct-q5_K_M
|
{
"ingested_by": "mneme",
"version": "physics_mvpn_1.0",
"contract": "WO-PHYS-03",
"chunk_id": 1,
"paper_id": "2511.15307v1"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:39:57.123841Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
w_20251209_194028422675
|
Refractive index and extinction coefficient of biocompatible HTL Yellow 20 μm resin measured with high precision for optogenetic applications
|
Refractive index and extinction coefficient of biocompatible HTL Yellow 20 μm resin measured with high precision for optogenetic applications
|
[
"Ellipsometry measurements on disks 3D printed from BMF resin",
"Refractive index (n) determined using Angle Spectroscopic Ellipsometer M-2000XI",
"Extinction coefficient (κ) determined via spectrophotometry with UV-Vis-NIR Evolution Spectrophotometer"
] | 0.85
|
medium
|
universal
|
physics
|
arxiv
|
2511.15420v2
|
https://arxiv.org/abs/2511.15420v2
|
[
"physics.optics",
"physics.app-ph",
"physics.bio-ph"
] |
d3a1886779c30b7b101bab97c6f4ba3ee41d0c5a74d8f1f45c34f4ea7cd4eae4
|
Extracted from ArXiv paper 2511.15420v2 (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": "2511.15420v2"
}
|
science
|
WO-ARX-01
|
2025-12-09T19:40:28.422675Z
|
arxiv
|
physics_recovered
|
arxiv_physics
|
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