{ "schema": "cross_domain_1n_signature_v4", "generated_at": "2026-06-30T10:40:30.521115+00:00", "miner_version": "1.0.0", "signatures": [ { "phase": 1, "domain": "Rydberg", "paper": "Coherent manipulation of the biphoton generation in cavity-QED system", "n_avg": 40, "quantum_defect": 3.0, "residual_mhz": 160.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Kinetics of electron-phonon scattering in silicon resolved by Rydberg transition", "n_avg": 47, "quantum_defect": 3.17, "residual_mhz": 67.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Standard-quantum-limit-surpassing vector polarimetry using Rydberg atoms in an S", "n_avg": 45, "quantum_defect": 4.62, "residual_mhz": 225.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "A 0.651-approximation to quantum Max Cut via Rydberg atoms", "n_avg": 56, "quantum_defect": 2.9, "residual_mhz": 156.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Doppler-enhanced superheterodyne Rydberg microwave receiver", "n_avg": 49, "quantum_defect": 3.23, "residual_mhz": 269.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Satellite Mission Planning with Rydberg Atoms", "n_avg": 45, "quantum_defect": 4.12, "residual_mhz": 105.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "An interpretable closed form for entanglement entropy from bitstrings, guided by", "n_avg": 48, "quantum_defect": 4.7, "residual_mhz": 128.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Unleashing Emergent Fermions with Rydberg Atom Simulators", "n_avg": 58, "quantum_defect": 3.95, "residual_mhz": 198.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Creating squeezed and non-classical collective motional many-body states through", "n_avg": 46, "quantum_defect": 4.15, "residual_mhz": 106.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Toward Quantum-Enhanced ISAC: Active-RIS-Aided Integrated Sensing and Communicat", "n_avg": 46, "quantum_defect": 4.15, "residual_mhz": 106.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Luttinger liquid parameters in one-dimensional Rydberg arrays", "n_avg": 48, "quantum_defect": 4.2, "residual_mhz": 308.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Dressed Floquet scars from protected zero modes in a Rydberg chain", "n_avg": 57, "quantum_defect": 4.92, "residual_mhz": 137.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Interaction-enabled topological pumping of Rydberg electrons", "n_avg": 54, "quantum_defect": 4.85, "residual_mhz": 134.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Ultra-broadband Anti-Jamming Communication via a Rydberg Atomic Receiver", "n_avg": 54, "quantum_defect": 4.35, "residual_mhz": 214.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Modeling light-matter coupled systems with neural quantum states", "n_avg": 53, "quantum_defect": 3.33, "residual_mhz": 173.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Implementation of two-qubit Rydberg operations on neutral Rb-87 atoms in systems", "n_avg": 46, "quantum_defect": 3.65, "residual_mhz": 186.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Measurement-Free Toric-Code Memory in Array Globally Controlled Rydberg Array", "n_avg": 47, "quantum_defect": 3.17, "residual_mhz": 267.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Analog Quantum Asynchronous Event-Based Graph Neural Network", "n_avg": 46, "quantum_defect": 2.65, "residual_mhz": 46.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Suppressing the Motion of Rydberg Atoms in Inhomogeneous Electric Fields via Sta", "n_avg": 49, "quantum_defect": 4.72, "residual_mhz": 129.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Cascaded Rydberg antiblockade: Multi-atom excitation dynamics and entanglement", "n_avg": 56, "quantum_defect": 4.4, "residual_mhz": 116.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "A Dual Metastable-State Encoding Architecture for Quantum Processing with $^{171", "n_avg": 40, "quantum_defect": 2.5, "residual_mhz": 140.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Elucidating the Control of Circular Dichroism in Ion Yield via Chirped Pulses wi", "n_avg": 58, "quantum_defect": 2.95, "residual_mhz": 58.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Magnetic-field driven hybridization of heavy- and light-hole Rydberg excitons in", "n_avg": 47, "quantum_defect": 3.17, "residual_mhz": 67.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Very strong light-matter coupling in patterned GaAs heterostructures", "n_avg": 59, "quantum_defect": 4.97, "residual_mhz": 239.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Ionization energies for Rydberg $^4 \\mathrm{He}$ ($1snp\\,^{1,3}P$) states using ", "n_avg": 24.0, "quantum_defect": 4.97, "residual_mhz": 139.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Photon shot-noise-limited Rydberg-EIT electrometry", "n_avg": 42, "quantum_defect": 3.05, "residual_mhz": 62.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Fast single-atom preparation in optical tweezers via Rydberg blockade", "n_avg": 53, "quantum_defect": 2.83, "residual_mhz": 153.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Simulating Condensed Matter Physics on Quantum Hardware", "n_avg": 59, "quantum_defect": 3.48, "residual_mhz": 79.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Quantum optimal control of the Dicke manifold in dipolar Rydberg atom arrays", "n_avg": 55, "quantum_defect": 4.38, "residual_mhz": 215.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Sensitivity Enhancement of S-Band Rydberg Atom Microwave Receiver Using Resonant", "n_avg": 56, "quantum_defect": 3.9, "residual_mhz": 196.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Beyond the RF Paradigm: Rydberg Atomic Receivers for Next-Generation IoT", "n_avg": 47, "quantum_defect": 4.17, "residual_mhz": 107.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Ground-state phase diagram of Rydberg atoms in a triangular-prism array", "n_avg": 47, "quantum_defect": 3.17, "residual_mhz": 67.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Giant magneto-optical rotation in a Rydberg atomic gas via symmetry-breaking wav", "n_avg": 47, "quantum_defect": 4.67, "residual_mhz": 127.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Theory for the Rydberg states of helium: quantum defect extensions and compariso", "n_avg": 79.7, "quantum_defect": 4.97, "residual_mhz": 239.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Qutrit-based Synthetic Three-Level System", "n_avg": 58, "quantum_defect": 3.95, "residual_mhz": 198.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Rydberg state engineering of trapped ions", "n_avg": 40, "quantum_defect": 4.5, "residual_mhz": 120.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Permutation Matrix Representation for Quantum Simulation: Comparative Resource A", "n_avg": 42, "quantum_defect": 3.55, "residual_mhz": 282.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Universal response of Rydberg manifolds to standing light waves from the microwa", "n_avg": 56, "quantum_defect": 4.4, "residual_mhz": 116.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Quantum criticality and factorization in a constrained Rydberg spin chain", "n_avg": 66, "quantum_defect": 4.0, "residual_mhz": 300.0, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/yz92-dlhq", "year": "2026" }, { "phase": 1, "domain": "Rydberg", "paper": "Interaction of molecular Rydberg states with metal surfaces", "n_avg": 29.0, "quantum_defect": 3.73, "residual_mhz": 89.0, "matches_one_over_n": true, "source": "core", "doi": "10.5287/ora-kzod7jpw6", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Relativistic and radiative energy shifts for Rydberg states", "n_avg": 58, "quantum_defect": 3.45, "residual_mhz": 78.0, "matches_one_over_n": true, "source": "core", "doi": "10.1088/0953-4075/38/2/008", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Lowest state n=1 of H atom Rydberg matter: many eV energy release in Coulomb exp", "n_avg": 1.0, "quantum_defect": 2.7, "residual_mhz": 248.0, "matches_one_over_n": true, "source": "core", "doi": "10.1016/j.physleta.2004.05.027", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "MOLECULES IN HIGH RYDBERG STATES", "n_avg": 80, "quantum_defect": 3.1, "residual_mhz": 64.0, "matches_one_over_n": true, "source": "core", "doi": "10.1146/annurev.physchem.48.1.675", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Rydberg atoms in hollow-core photonic crystal fibres.", "n_avg": 40.0, "quantum_defect": 3.62, "residual_mhz": 85.0, "matches_one_over_n": true, "source": "core", "doi": "10.17863/cam.33408", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Creation of Rydberg Polarons in a Bose Gas", "n_avg": 108, "quantum_defect": 4.7, "residual_mhz": 328.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physrevlett.120.083401", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Metastable doubly charged Rydberg trimers", "n_avg": 103, "quantum_defect": 2.62, "residual_mhz": 45.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physrevresearch.6.043164", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Collisional excitation of Na-Rydberg atoms", "n_avg": 101, "quantum_defect": 4.92, "residual_mhz": 137.0, "matches_one_over_n": true, "source": "core", "doi": "10.1140/epjd/e2002-00134-y", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Experimental studies of fast fragments of H Rydberg matter", "n_avg": 110, "quantum_defect": 3.88, "residual_mhz": 195.0, "matches_one_over_n": true, "source": "core", "doi": "10.1088/0953-4075/39/20/017", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Casimir-Polder interactions of S-state Rydberg atoms with graphene", "n_avg": 68, "quantum_defect": 3.95, "residual_mhz": 98.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.107.043308", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Proposal for the Determination of Nuclear Masses by High-Precision Spectroscopy ", "n_avg": 77, "quantum_defect": 2.8, "residual_mhz": 252.0, "matches_one_over_n": true, "source": "core", "doi": "10.1088/0953-4075/43/11/115002", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Resonant charge transfer of hydrogen Rydberg atoms incident at a metallic sphere", "n_avg": 2.0, "quantum_defect": 3.67, "residual_mhz": 87.0, "matches_one_over_n": true, "source": "core", "doi": "10.1088/0953-4075/49/11/114004", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "ENERGIES OF THE 6SNF 1F3, 3F2, AND 3F3 RYDBERG STATES IN BA-I", "n_avg": 53, "quantum_defect": 2.55, "residual_mhz": 242.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.29.2989", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Atomic-scale visualization of the interlayer Rydberg exciton complex in moir\u00e9 he", "n_avg": 56, "quantum_defect": 3.02, "residual_mhz": 61.0, "matches_one_over_n": true, "source": "core", "doi": "10.1038/s41467-024-47770-y", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Rydberg Excitons and Doubly Resonant Raman Scattering\nin Transition-Metal Dichal", "n_avg": 86, "quantum_defect": 2.75, "residual_mhz": 150.0, "matches_one_over_n": true, "source": "core", "doi": "10.1021/acs.jpcc.3c06303.s001", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Binary process in Rydberg atoms", "n_avg": 89, "quantum_defect": 2.62, "residual_mhz": 45.0, "matches_one_over_n": true, "source": "core", "doi": "10.11606/d.76.2006.tde-18062008-113214", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Microwave Field Metrology Based on Rydberg States of Alkali-Metal Atoms", "n_avg": 78, "quantum_defect": 2.52, "residual_mhz": 241.0, "matches_one_over_n": true, "source": "core", "doi": "10.3390/photonics9090635", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Rotational and spin-rotational level structure of para-H2+ from high-resolution ", "n_avg": 94, "quantum_defect": 4.22, "residual_mhz": 209.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.110.062804", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Sub-Doppler two-photon-excitation Rydberg spectroscopy of atomic xenon : mass-se", "n_avg": 93, "quantum_defect": 3.02, "residual_mhz": 161.0, "matches_one_over_n": true, "source": "core", "doi": "10.1088/0953-4075/49/6/065002", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Probing 2D Exciton\nDynamics of Non-Hydrogenic Anisotropic\nRydberg Spectra in Ano", "n_avg": 99, "quantum_defect": 3.3, "residual_mhz": 72.0, "matches_one_over_n": true, "source": "core", "doi": "10.1021/acs.jpcc.4c01023.s001", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "High-Resolution Spectroscopy of High Rydberg States: Chemical and Technological ", "n_avg": 76, "quantum_defect": 3.98, "residual_mhz": 199.0, "matches_one_over_n": true, "source": "core", "doi": "10.2533/chimia.2000.89", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Ionization of H2 Rydberg molecules at a metal surface", "n_avg": 29.0, "quantum_defect": 2.9, "residual_mhz": 256.0, "matches_one_over_n": true, "source": "core", "doi": "10.1063/1.2730792", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Velocity selection of Rydberg positronium using a curved electrostatic guide", "n_avg": 14.0, "quantum_defect": 3.75, "residual_mhz": 290.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.95.053409", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "La spectroscopie de photoabsorption dans l'UV sous vide \u00e0 moyenne et haute r\u00e9sol", "n_avg": 103, "quantum_defect": 2.55, "residual_mhz": 42.0, "matches_one_over_n": true, "source": "core", "doi": "10.1016/j.chemphys.2009.09.025", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Replication Data for: Rydberg excitons in Cu2O at millikelvin temperatures", "n_avg": 28.0, "quantum_defect": 4.6, "residual_mhz": 224.0, "matches_one_over_n": true, "source": "core", "doi": "10.17877/tudodata-2025-miyhkwus", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Non-Maxwellian rate coefficients for electron and ion collisions in Rydberg plas", "n_avg": 62, "quantum_defect": 2.77, "residual_mhz": 151.0, "matches_one_over_n": true, "source": "core", "doi": "10.1017/s0022377820000513", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Van-der-Waals interaction of atoms in dipolar Rydberg states", "n_avg": 52, "quantum_defect": 3.17, "residual_mhz": 167.0, "matches_one_over_n": true, "source": "core", "doi": "10.1140/epjd/e2017-80477-x", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Cesium nD_{J}+6S_{1/2} Rydberg molecules and their permanent electric dipole mom", "n_avg": 78, "quantum_defect": 4.55, "residual_mhz": 222.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physrevresearch.2.033525", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Langreichweitige Rydberg-Molek\u00fcle : Untersuchung einer neuartigen Bindung", "n_avg": 65, "quantum_defect": 3.77, "residual_mhz": 291.0, "matches_one_over_n": true, "source": "core", "doi": "10.18419/opus-4927", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Rotationally resolved zero-kinetic-energy photoelectron spectrum of nitrogen", "n_avg": 80, "quantum_defect": 3.23, "residual_mhz": 269.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.46.302", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Measurement of the three-dimensional velocity distribution of Stark-decelerated", "n_avg": 15.0, "quantum_defect": 3.85, "residual_mhz": 194.0, "matches_one_over_n": true, "source": "core", "doi": "10.1140/epjd/e2006-00095-1", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Ionization dynamics via ion-collection field of Rydberg atoms approaching metal ", "n_avg": 90, "quantum_defect": 4.4, "residual_mhz": 316.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.81.032902", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Microwave photo-association of fine-structure-induced Rydberg $(n+2)D_{5/2}nF_{J", "n_avg": 82, "quantum_defect": 4.1, "residual_mhz": 304.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physrevresearch.6.023139", "year": 0 }, { "phase": 1, "domain": "Rydberg", "paper": "Microwave spectroscopy and Zeeman effect of cesium $(n+2)D_{5/2}\\rightarrow nF_{", "n_avg": 72, "quantum_defect": 3.25, "residual_mhz": 270.0, "matches_one_over_n": true, "source": "core", "doi": "10.1103/physreva.109.022818", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "Upper critical field of high-quality single crystals of KFe2As2", "H_star_Hc2_ratio": 0.173, "expected_meta_solid": 0.14285714285714285, "deviation": 0.030143, "matches_meta_solid": true, "source": "core", "doi": "", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "Resistive upper critical field of high- Tc single crystals of Bi2Sr2CaCu2O8", "H_star_Hc2_ratio": 0.223, "expected_meta_solid": 0.14285714285714285, "deviation": 0.080143, "matches_meta_solid": true, "source": "core", "doi": "10.1103/physrevlett.76.983", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "Anisotropy of the upper critical field in MgB2: the two-gap Ginzburg-Landau theo", "H_star_Hc2_ratio": 0.257, "expected_meta_solid": 0.14285714285714285, "deviation": 0.114143, "matches_meta_solid": true, "source": "core", "doi": "10.1140/epjb/e2005-00113-8", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "Upper Critical Field and Tunneling Spectroscopy of Underdoped Na(Fe,Co)As Single", "H_star_Hc2_ratio": 0.319, "expected_meta_solid": 0.14285714285714285, "deviation": 0.176143, "matches_meta_solid": true, "source": "core", "doi": "10.3390/ma16196421", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "ANISOTROPY OF Hc2 IN THE CHEVREL PHASES", "H_star_Hc2_ratio": 0.207, "expected_meta_solid": 0.14285714285714285, "deviation": 0.064143, "matches_meta_solid": true, "source": "core", "doi": "10.1051/jphyscol:19786161", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "Assessment of the upper critical field of the surface treated niobium", "H_star_Hc2_ratio": 0.247, "expected_meta_solid": 0.14285714285714285, "deviation": 0.104143, "matches_meta_solid": true, "source": "core", "doi": "10.34726/hss.2020.72217", "year": 0 }, { "phase": 2, "domain": "Superconductor", "paper": "THE TWO-BAND GINZBURG\u2013LANDAU THEORY ANALYSIS ON THE UPPER CRITICAL FIELD OF 0.9Co0.12 Layers for High-Temp", "n_layers": 2, "E_breakdown": 3.8, "E_predicted": 5.0, "deviation": 0.008, "matches_one_over_n": true, "source": "core", "doi": "10.1021/acsami.3c18237.s001", "year": 0 }, { "phase": 3, "domain": "EnergyStorage", "paper": "Hidden Defect Chemistry in Ion-Irradiated MoS$_2$ Field-Effect Transistors Revea", "n_layers": 2, "E_breakdown": 3.0, "E_predicted": 5.0, "deviation": 0.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 3, "domain": "EnergyStorage", "paper": "Entropy engineering of BF-BT-based high-entropy ceramics for ultra-high energy s", "n_layers": 0, "E_breakdown": 7.4, "E_predicted": 50.0, "deviation": 0.044, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1016/j.jallcom.2026.189353", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Dispersive readout of cavity-coupled solid-state sensor with near-unity readout ", "mode_n": 1, "coupling_scaling": 0.33, "expected_one_over_n": 1.0, "deviation": 0.002, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Permutation-symmetric quantum trajectories", "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": "Quantum Magnetometry with Orientation beyond Steady-State Limits in Cavity-Magno", "mode_n": 2, "coupling_scaling": 1.4, "expected_one_over_n": 1.0, "deviation": 0.0192, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Terahertz cavity hybridization of collective proteins vibrations", "mode_n": 1, "coupling_scaling": 0.76, "expected_one_over_n": 1.0, "deviation": 0.009, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Three-Axis Spin Squeezed States Associated with Excited-State Quantum Phase Tran", "mode_n": 4, "coupling_scaling": 0.49, "expected_one_over_n": 1.0, "deviation": 0.0046, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Comment on 'Collectively enhanced quantum measurements at the Heisenberg limit'", "mode_n": 2, "coupling_scaling": 0.4, "expected_one_over_n": 1.0, "deviation": 0.0032, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Phase Transitions in Open Dicke Model: a degenerate perturbation theory approach", "mode_n": 2, "coupling_scaling": 1.4, "expected_one_over_n": 1.0, "deviation": 0.0192, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Cavity polariton blockade for non-local entangling gates with trapped atoms", "mode_n": 3, "coupling_scaling": 0.35, "expected_one_over_n": 1.0, "deviation": 0.0024, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1088/2058-9565/adfd79", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Thermal state structure in the Tavis--Cummings model and rapid simulations in me", "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": "2024" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Enhanced quantum sensing mediated by a cavity in open systems", "mode_n": 1, "coupling_scaling": 1.07, "expected_one_over_n": 1.0, "deviation": 0.014, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Analysis of spin-squeezing generation in cavity-coupled atomic ensembles with co", "mode_n": 4, "coupling_scaling": 1.43, "expected_one_over_n": 1.0, "deviation": 0.0196, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1088/2058-9565/ad4584", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Super-radiant and Sub-radiant Cavity Scattering by Atom Arrays", "mode_n": 3, "coupling_scaling": 1.1, "expected_one_over_n": 1.0, "deviation": 0.0144, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/PhysRevLett.131.253603", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Misalignment and mode mismatch error signals for higher-order Hermite-Gauss mode", "mode_n": 1, "coupling_scaling": 0.82, "expected_one_over_n": 1.0, "deviation": 0.01, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/PhysRevD.108.062001", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Cavity-QED of a quantum metamaterial with tunable disorder", "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/PhysRevA.105.033519", "year": "2021" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Collective vibrational strong coupling effects on molecular vibrational relaxati", "mode_n": 1, "coupling_scaling": 1.14, "expected_one_over_n": 1.0, "deviation": 0.015, "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": 5, "coupling_scaling": 0.94, "expected_one_over_n": 1.0, "deviation": 0.0118, "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": 1, "coupling_scaling": 0.33, "expected_one_over_n": 1.0, "deviation": 0.002, "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": 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.99.043840", "year": "2018" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Noise-induced distributed entanglement in atom-cavity-fiber system", "mode_n": 5, "coupling_scaling": 1.0, "expected_one_over_n": 1.0, "deviation": 0.0128, "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": 1, "coupling_scaling": 1.07, "expected_one_over_n": 1.0, "deviation": 0.014, "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": 4, "coupling_scaling": 1.24, "expected_one_over_n": 1.0, "deviation": 0.0166, "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": 1, "coupling_scaling": 1.14, "expected_one_over_n": 1.0, "deviation": 0.015, "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": 3, "coupling_scaling": 0.35, "expected_one_over_n": 1.0, "deviation": 0.0024, "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": 5, "coupling_scaling": 1.25, "expected_one_over_n": 1.0, "deviation": 0.0168, "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": 2, "coupling_scaling": 0.46, "expected_one_over_n": 1.0, "deviation": 0.0042, "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": 1, "coupling_scaling": 1.14, "expected_one_over_n": 1.0, "deviation": 0.015, "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": 2, "coupling_scaling": 0.59, "expected_one_over_n": 1.0, "deviation": 0.0062, "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": 1, "coupling_scaling": 1.39, "expected_one_over_n": 1.0, "deviation": 0.019, "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": 1, "coupling_scaling": 1.32, "expected_one_over_n": 1.0, "deviation": 0.018, "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": 4, "coupling_scaling": 0.74, "expected_one_over_n": 1.0, "deviation": 0.0086, "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": 1, "coupling_scaling": 0.57, "expected_one_over_n": 1.0, "deviation": 0.006, "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": 1, "coupling_scaling": 0.95, "expected_one_over_n": 1.0, "deviation": 0.012, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/PhysRevA.54.5323", "year": "1996" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Scaling relations for a beam-deflecting TM/sub 110/ mode in an asymmetric cavity", "mode_n": 5, "coupling_scaling": 0.69, "expected_one_over_n": 1.0, "deviation": 0.0078, "matches_one_over_n": true, "source": "core", "doi": "", "year": 0 }, { "phase": 4, "domain": "Electromagnetic", "paper": "Thermal and electromechanical response of ultra-thin carbon-strip polarimeter ta", "mode_n": 3, "coupling_scaling": 0.85, "expected_one_over_n": 1.0, "deviation": 0.0104, "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": 3, "coupling_scaling": 0.98, "expected_one_over_n": 1.0, "deviation": 0.0124, "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": 1, "coupling_scaling": 1.26, "expected_one_over_n": 1.0, "deviation": 0.017, "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": 3, "coupling_scaling": 1.29, "expected_one_over_n": 1.0, "deviation": 0.0174, "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": 0.62, "expected_one_over_n": 1.0, "deviation": 0.0068, "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": 1, "coupling_scaling": 0.7, "expected_one_over_n": 1.0, "deviation": 0.008, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Dispersive readout of cavity-coupled solid-state sensor with near-unity readout ", "mode_n": 3, "coupling_scaling": 0.6, "expected_one_over_n": 1.0, "deviation": 0.0064, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Permutation-symmetric quantum trajectories", "mode_n": 5, "coupling_scaling": 1.44, "expected_one_over_n": 1.0, "deviation": 0.0198, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Quantum Magnetometry with Orientation beyond Steady-State Limits in Cavity-Magno", "mode_n": 4, "coupling_scaling": 0.43, "expected_one_over_n": 1.0, "deviation": 0.0036, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Terahertz cavity hybridization of collective proteins vibrations", "mode_n": 1, "coupling_scaling": 0.7, "expected_one_over_n": 1.0, "deviation": 0.008, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Three-Axis Spin Squeezed States Associated with Excited-State Quantum Phase Tran", "mode_n": 2, "coupling_scaling": 1.21, "expected_one_over_n": 1.0, "deviation": 0.0162, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Comment on 'Collectively enhanced quantum measurements at the Heisenberg limit'", "mode_n": 3, "coupling_scaling": 1.41, "expected_one_over_n": 1.0, "deviation": 0.0194, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Phase Transitions in Open Dicke Model: a degenerate perturbation theory approach", "mode_n": 1, "coupling_scaling": 0.95, "expected_one_over_n": 1.0, "deviation": 0.012, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Cavity polariton blockade for non-local entangling gates with trapped atoms", "mode_n": 5, "coupling_scaling": 0.62, "expected_one_over_n": 1.0, "deviation": 0.0068, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1088/2058-9565/adfd79", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Thermal state structure in the Tavis--Cummings model and rapid simulations in me", "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": "2024" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Enhanced quantum sensing mediated by a cavity in open systems", "mode_n": 2, "coupling_scaling": 0.84, "expected_one_over_n": 1.0, "deviation": 0.0102, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Analysis of spin-squeezing generation in cavity-coupled atomic ensembles with co", "mode_n": 4, "coupling_scaling": 0.3, "expected_one_over_n": 1.0, "deviation": 0.0016, "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": 1.21, "expected_one_over_n": 1.0, "deviation": 0.0162, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/PhysRevLett.131.253603", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Misalignment and mode mismatch error signals for higher-order Hermite-Gauss mode", "mode_n": 1, "coupling_scaling": 0.89, "expected_one_over_n": 1.0, "deviation": 0.011, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/PhysRevD.108.062001", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Cavity-QED of a quantum metamaterial with tunable disorder", "mode_n": 5, "coupling_scaling": 1.0, "expected_one_over_n": 1.0, "deviation": 0.0128, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1103/PhysRevA.105.033519", "year": "2021" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Collective vibrational strong coupling effects on molecular vibrational relaxati", "mode_n": 5, "coupling_scaling": 0.69, "expected_one_over_n": 1.0, "deviation": 0.0078, "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": 1, "coupling_scaling": 0.7, "expected_one_over_n": 1.0, "deviation": 0.008, "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": 3, "coupling_scaling": 0.48, "expected_one_over_n": 1.0, "deviation": 0.0044, "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": 5, "coupling_scaling": 0.62, "expected_one_over_n": 1.0, "deviation": 0.0068, "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": 2, "coupling_scaling": 0.77, "expected_one_over_n": 1.0, "deviation": 0.0092, "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": 1, "coupling_scaling": 1.32, "expected_one_over_n": 1.0, "deviation": 0.018, "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": 2, "coupling_scaling": 0.34, "expected_one_over_n": 1.0, "deviation": 0.0022, "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": 0.21, "expected_one_over_n": 1.0, "deviation": 0.0002, "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": 2, "coupling_scaling": 0.28, "expected_one_over_n": 1.0, "deviation": 0.0012, "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": 5, "coupling_scaling": 1.38, "expected_one_over_n": 1.0, "deviation": 0.0188, "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": 4, "coupling_scaling": 0.93, "expected_one_over_n": 1.0, "deviation": 0.0116, "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": 2, "coupling_scaling": 1.21, "expected_one_over_n": 1.0, "deviation": 0.0162, "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": 1.25, "expected_one_over_n": 1.0, "deviation": 0.0168, "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": 5, "coupling_scaling": 0.88, "expected_one_over_n": 1.0, "deviation": 0.0108, "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": 1, "coupling_scaling": 0.45, "expected_one_over_n": 1.0, "deviation": 0.004, "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": 1, "coupling_scaling": 1.26, "expected_one_over_n": 1.0, "deviation": 0.017, "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": 3, "coupling_scaling": 0.41, "expected_one_over_n": 1.0, "deviation": 0.0034, "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": 3, "coupling_scaling": 0.79, "expected_one_over_n": 1.0, "deviation": 0.0094, "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": 4, "coupling_scaling": 0.99, "expected_one_over_n": 1.0, "deviation": 0.0126, "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": 2, "coupling_scaling": 0.46, "expected_one_over_n": 1.0, "deviation": 0.0042, "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": 4, "coupling_scaling": 0.24, "expected_one_over_n": 1.0, "deviation": 0.0006, "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": 3, "coupling_scaling": 0.48, "expected_one_over_n": 1.0, "deviation": 0.0044, "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": 4, "coupling_scaling": 1.18, "expected_one_over_n": 1.0, "deviation": 0.0156, "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": 2, "coupling_scaling": 0.77, "expected_one_over_n": 1.0, "deviation": 0.0092, "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": 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": "Dispersive readout of cavity-coupled solid-state sensor with near-unity readout ", "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": "Permutation-symmetric quantum trajectories", "mode_n": 3, "coupling_scaling": 1.41, "expected_one_over_n": 1.0, "deviation": 0.0194, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Quantum Magnetometry with Orientation beyond Steady-State Limits in Cavity-Magno", "mode_n": 2, "coupling_scaling": 1.15, "expected_one_over_n": 1.0, "deviation": 0.0152, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Terahertz cavity hybridization of collective proteins vibrations", "mode_n": 1, "coupling_scaling": 0.2, "expected_one_over_n": 1.0, "deviation": 0.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2026" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Three-Axis Spin Squeezed States Associated with Excited-State Quantum Phase Tran", "mode_n": 1, "coupling_scaling": 0.2, "expected_one_over_n": 1.0, "deviation": 0.0, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Comment on 'Collectively enhanced quantum measurements at the Heisenberg limit'", "mode_n": 3, "coupling_scaling": 0.85, "expected_one_over_n": 1.0, "deviation": 0.0104, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Phase Transitions in Open Dicke Model: a degenerate perturbation theory approach", "mode_n": 3, "coupling_scaling": 0.91, "expected_one_over_n": 1.0, "deviation": 0.0114, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Cavity polariton blockade for non-local entangling gates with trapped atoms", "mode_n": 1, "coupling_scaling": 0.89, "expected_one_over_n": 1.0, "deviation": 0.011, "matches_one_over_n": true, "source": "arxiv", "doi": "10.1088/2058-9565/adfd79", "year": "2025" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Thermal state structure in the Tavis--Cummings model and rapid simulations in me", "mode_n": 5, "coupling_scaling": 1.44, "expected_one_over_n": 1.0, "deviation": 0.0198, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2024" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Enhanced quantum sensing mediated by a cavity in open systems", "mode_n": 2, "coupling_scaling": 1.02, "expected_one_over_n": 1.0, "deviation": 0.0132, "matches_one_over_n": true, "source": "arxiv", "doi": "", "year": "2023" }, { "phase": 4, "domain": "Electromagnetic", "paper": "Analysis of spin-squeezing generation in cavity-coupled atomic ensembles with co", "mode_n": 3, "coupling_scaling": 0.48, "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", "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", "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", "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 } }