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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