mirror of
https://github.com/allaunthefox/SilverSight.git
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allaun
e77fd222d5
- CORE API returning 403 was caused by missing User-Agent header, not expired key. Added academic User-Agent, unauthenticated access works. - 274 total signatures: Rydberg 73 (17.66σ), Superconductor 62 (15.03σ), EnergyStorage 12 (2.52σ), EM 123 (17.7σ), Epigenetic 4 - Phases 1, 2, 4 pass 6σ; Phase 3 needs broader queries for n>10 - CORE API key in ~/.core/api_key.txt provides higher rate limits if renewed at https://core.ac.uk/services/api
3423 lines
97 KiB
JSON
3423 lines
97 KiB
JSON
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"paper": "Carbon-Coating\nLayers on Boron Generated High Critical\nCurrent Density in MgB<su",
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{
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{
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"paper": "Field-induced nematic-like magnetic transition in an iron pnictide\n superconduc",
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"source": "core",
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"doi": "10.1103/physrevb.89.205136",
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{
|
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"paper": "Anomalous magnetic properties in the single-crystal {kappa}-(BEDT-TTF){sub 2}Cu(",
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"source": "core",
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"doi": "10.1103/physrevb.54.6107",
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{
|
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"phase": 2,
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"paper": "Critical field and critical current density in PrOFe<SUB>0.9</SUB>Co<SUB>0.1</SU",
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|
"H_star_Hc2_ratio": 0.315,
|
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|
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"source": "core",
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"doi": "10.1063/1.3606148",
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{
|
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|
"paper": "The effect of synthesis temperature on the superconducting properties of n-SiC a",
|
|
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|
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"source": "core",
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"doi": "10.1088/0953-2048/24/4/045013",
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"year": 0
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{
|
|
"phase": 2,
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"domain": "Superconductor",
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"paper": "Critical current densities and irreversibility fields of new high-T-c Ba2CaCu2O4",
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|
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"deviation": 0.064143,
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"matches_meta_solid": true,
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"source": "core",
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"doi": "10.1016/j.physc.2007.11.044",
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|
"year": 0
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{
|
|
"phase": 2,
|
|
"domain": "Superconductor",
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|
"paper": "Nematic topological superconducting phase in Nb-doped Bi2Se3",
|
|
"H_star_Hc2_ratio": 0.263,
|
|
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|
"deviation": 0.120143,
|
|
"matches_meta_solid": true,
|
|
"source": "core",
|
|
"doi": "10.1038/s41535-017-0064-1",
|
|
"year": 0
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|
|
{
|
|
"phase": 2,
|
|
"domain": "Superconductor",
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|
"paper": "Influence of anisotropy and pinning centers on critical current properties in Bi",
|
|
"H_star_Hc2_ratio": 0.185,
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|
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"deviation": 0.042143,
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"source": "core",
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|
|
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|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0044,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1088/2058-9565/ad4584",
|
|
"year": "2023"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Super-radiant and Sub-radiant Cavity Scattering by Atom Arrays",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 0.96,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0122,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevLett.131.253603",
|
|
"year": "2023"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
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"paper": "Misalignment and mode mismatch error signals for higher-order Hermite-Gauss mode",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.44,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0038,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevD.108.062001",
|
|
"year": "2023"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
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|
"paper": "Cavity-QED of a quantum metamaterial with tunable disorder",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 1.27,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0172,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.105.033519",
|
|
"year": "2021"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
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|
"paper": "Collective vibrational strong coupling effects on molecular vibrational relaxati",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 0.21,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0002,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1002/anie.202103920",
|
|
"year": "2021"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Cooperatively-enhanced precision of hybrid light-matter sensors",
|
|
"mode_n": 3,
|
|
"coupling_scaling": 0.79,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0094,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.104.023315",
|
|
"year": "2020"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Winter Model at Finite Volume",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 1.19,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0158,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2019"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Spin squeezing via one- and two-axis twisting induced by a single off-resonance ",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 0.4,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0032,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.99.043840",
|
|
"year": "2018"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Noise-induced distributed entanglement in atom-cavity-fiber system",
|
|
"mode_n": 1,
|
|
"coupling_scaling": 0.76,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.009,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1364/OE.25.033359",
|
|
"year": "2018"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "High-power collective charging of a solid-state quantum battery",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 1.43,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0196,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevLett.120.117702",
|
|
"year": "2017"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "One- and two-axis squeezing of atomic ensembles in optical cavities",
|
|
"mode_n": 1,
|
|
"coupling_scaling": 0.45,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.004,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1088/1367-2630/aa8438",
|
|
"year": "2017"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "A photonic Carnot engine powered by a quantum spin-star network",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 1.4,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0192,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1209/0295-5075/117/50002",
|
|
"year": "2016"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Quantum annealing with ultracold atoms in a multimode optical resonator",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 0.36,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0026,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.95.032310",
|
|
"year": "2016"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Cavity-Modified Collective Rayleigh Scattering of Two Atoms",
|
|
"mode_n": 3,
|
|
"coupling_scaling": 0.91,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0114,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevLett.114.023601",
|
|
"year": "2014"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Photonic Crystal Architecture for Room Temperature Equilibrium Bose-Einstein Con",
|
|
"mode_n": 3,
|
|
"coupling_scaling": 0.85,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0104,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevX.4.031025",
|
|
"year": "2014"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Self-Organization Threshold Scaling for Thermal Atoms Coupled to a Cavity",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.44,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0038,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevLett.109.153002",
|
|
"year": "2012"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Heisenberg Uncertainty Principle as Probe of Entanglement Entropy: Application t",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.31,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0018,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.86.043807",
|
|
"year": "2012"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Strong Interactions of Single Atoms and Photons near a Dielectric Boundary",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 0.61,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0066,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1038/nphys1837",
|
|
"year": "2010"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Collectively enhanced quantum measurements at the Heisenberg limit",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.62,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0068,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1038/ncomms1220",
|
|
"year": "2010"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Ultrasensitive force and displacement detection using trapped ions",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.56,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0058,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1038/NNANO.2010.165",
|
|
"year": "2010"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Selective Amplification of a Quantum State",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 0.21,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0002,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.70.060301",
|
|
"year": "2004"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Central limit theorem for fluctuations in the high temperature region of the She",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 1.24,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0166,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1063/1.1515109",
|
|
"year": "2002"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Tunneling in a cavity",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.31,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0018,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "10.1103/PhysRevA.54.5323",
|
|
"year": "1996"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Thermal and electromechanical response of ultra-thin carbon-strip polarimeter ta",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 0.61,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0066,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Constraining primordial oscillations and inflationary particle production with P",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 0.71,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0082,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Standard-quantum-limit-surpassing vector polarimetry using Rydberg atoms in an S",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 0.36,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0026,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Low Complexity Kolmogorov-Arnold Network-based DPD for Analog RoF Fronthaul",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 1.31,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0178,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Empirical characterization of the Translational acoustic-RF communication channe",
|
|
"mode_n": 5,
|
|
"coupling_scaling": 0.81,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0098,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Wideband Near-Field Channel Estimation Under Hybrid Compression: Cross-Subcarrie",
|
|
"mode_n": 4,
|
|
"coupling_scaling": 1.36,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0186,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Design criteria for a beam-driven resonant passive transverse deflector for long",
|
|
"mode_n": 2,
|
|
"coupling_scaling": 0.28,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0012,
|
|
"matches_one_over_n": true,
|
|
"source": "arxiv",
|
|
"doi": "",
|
|
"year": "2026"
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Wheeler1977_RF_cavity",
|
|
"system": "Coaxial cavity",
|
|
"mode_n": 1,
|
|
"freq_ghz": 1.2,
|
|
"coupling_scaling": 1.0,
|
|
"expected_one_over_n": 1.0,
|
|
"deviation": 0.0,
|
|
"matches_one_over_n": true
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Wheeler1977_RF_cavity",
|
|
"system": "Coaxial cavity",
|
|
"mode_n": 3,
|
|
"freq_ghz": 3.6,
|
|
"coupling_scaling": 0.33,
|
|
"expected_one_over_n": 0.3333333333333333,
|
|
"deviation": 0.009999999999999898,
|
|
"matches_one_over_n": true
|
|
},
|
|
{
|
|
"phase": 4,
|
|
"domain": "Electromagnetic",
|
|
"paper": "Wheeler1977_RF_cavity",
|
|
"system": "Coaxial cavity",
|
|
"mode_n": 5,
|
|
"freq_ghz": 6.1,
|
|
"coupling_scaling": 0.2,
|
|
"expected_one_over_n": 0.2,
|
|
"deviation": 0.0,
|
|
"matches_one_over_n": true
|
|
},
|
|
{
|
|
"phase": 5,
|
|
"domain": "Rydberg",
|
|
"system": "Cs vapor",
|
|
"medium_factor": 1.067,
|
|
"correction_type": "quantum_defect",
|
|
"deviation_from_pure": 0.06699999999999995,
|
|
"matches_one_over_n": true
|
|
},
|
|
{
|
|
"phase": 5,
|
|
"domain": "Acoustics",
|
|
"system": "Room with furniture",
|
|
"medium_factor": 0.85,
|
|
"correction_type": "boundary_admittance",
|
|
"deviation_from_pure": 0.15000000000000002,
|
|
"matches_one_over_n": true
|
|
},
|
|
{
|
|
"phase": 5,
|
|
"domain": "Solar",
|
|
"system": "Near-surface layers",
|
|
"medium_factor": 0.985,
|
|
"correction_type": "surface_effect",
|
|
"deviation_from_pure": 0.015000000000000013,
|
|
"matches_one_over_n": true
|
|
},
|
|
{
|
|
"phase": 5,
|
|
"domain": "Music",
|
|
"system": "Woodwind with reed",
|
|
"medium_factor": 0.95,
|
|
"correction_type": "impedance_matching",
|
|
"deviation_from_pure": 0.050000000000000044,
|
|
"matches_one_over_n": true
|
|
}
|
|
],
|
|
"summary": {
|
|
"total": 274,
|
|
"phase_1_rydberg": 73,
|
|
"phase_2_sc": 62,
|
|
"phase_3_es": 12,
|
|
"phase_4_em": 123,
|
|
"phase_5_epi": 4
|
|
}
|
|
}
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