{"total":12,"items":[{"citing_arxiv_id":"2606.26789","ref_index":4,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Spectral condensation in a finite nonequilibrium atmospheric transition","primary_cat":"physics.ao-ph","submitted_at":"2026-06-25T09:23:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Spectral condensation of eigen-microstate occupations, quantified by emergent-sector entropy, diagnoses finite nonequilibrium transitions such as polar-vortex breakdown in ERA5 data and a wave-mean-flow model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.18059","ref_index":17,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Universal scaling and relaxation in decaying turbulence of Bose gases","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-06-16T15:35:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Review of universal scaling laws, nonthermal fixed points, and direct/inverse cascades observed in the relaxation of turbulent three-dimensional Bose-Einstein condensates.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.12968","ref_index":136,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Quantum-Driven Neuromorphic Computing for Million-Qubit-Scale Workloads","primary_cat":"quant-ph","submitted_at":"2026-06-11T06:55:19+00:00","verdict":"REJECT","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Apollo is a room-temperature 10000-node CMOS neuromorphic chip whose p-qubit network emulates transverse-field quantum annealing via Suzuki-Trotter and reportedly achieves lower energies than cryogenic QA on 3D spin-glass benchmarks across 300 realizations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.07417","ref_index":164,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"An optimal local theory for reaction-diffusion equations driven by non-trace-class noise","primary_cat":"math.AP","submitted_at":"2026-06-05T16:10:51+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Establishes optimal local well-posedness for reaction-diffusion SPDEs with non-trace-class multiplicative noise, critical initial-data spaces, instantaneous regularization, and applications to prototypical models.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15655","ref_index":47,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Critical slowing down of black hole phase transition and universal dynamic scaling in AdS black holes","primary_cat":"hep-th","submitted_at":"2026-05-15T06:24:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Black hole phase transitions in AdS spacetime show critical slowing down with relaxation time scaling as τ = |ε|^{-2/3}, and this exponent is the same for RN-AdS, Kerr-AdS, and Bardeen black holes.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.11138","ref_index":24,"ref_count":2,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Field Theory of Data: Anomaly Detection via the Functional Renormalization Group. The 2D Ising Model as a Benchmark","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-11T18:43:14+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Establishes correspondence between anomaly detection and functional renormalization group flow of non-equilibrium field theories, benchmarked on 2D Ising model identifying critical thresholds with <4% error.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"The bare transition temperature T0 is fixed at1. WhenT <1, the potential exhibits a double-well structure andφ= 0becomes an unstable solution. However,T 0 is not the physical critical temperatureT c. Due to the quartic interaction, the system displays an additional rigidity from fluctuations that corrects the bare temperature value (see Appendix A) [24]. The code of the simulation can be found on https://github.com/ParhamRadpay/Model-A. The correspondence with the 2D Ising model can be established heuristically as follows. For simplicity, we consider a unit Boltzmann constant. The critical temperature in mean-field theory isT 0 = 4J, whereJ >0is the Ising coupling in the HamiltonianHIsing =J ∑ ⟨i,j⟩SiSj, and⟨i, j⟩"},{"citing_arxiv_id":"2605.10346","ref_index":94,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Non-equilibrium scaling across first-order transitions with relativistic scalar fields","primary_cat":"hep-ph","submitted_at":"2026-05-11T10:49:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Fast driving across first-order transitions in relativistic scalar fields produces temperature- and dimension-independent finite-time scaling matching mean-field theory, crossing over to Kibble-Zurek scaling near criticality and nucleation-dominated dynamics at low temperatures.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"simulations in d =2 and d =3 spatial dimensions that follows in Section 5. Finally, we conclude in Section 6 with a summary of our findings and highlight possible future research directions. 2 2. Model setup We study a system in the static Z2 Ising universality class and the dynamic universality class of Model A in the Hohenberg-Halperin classification scheme [94], characterized by a nonconserved real scalar order-parameter field ϕ following the second-order Langevin equation of motion ∂2ϕ ∂t2 +γ ∂ϕ ∂t =− δF[ϕ] δϕ +ξ.(1) Here ξ is a stochastic noise term with zero mean ⟨ξ⟩ =0 and variance ⟨ξ(t,x )ξ(t′,x ′)⟩ =2 γTδ (t−t ′)δ(x−x ′), where the temperature T determines the strength of fluctuations, andγ is a damping coefficient."},{"citing_arxiv_id":"2605.02397","ref_index":1,"ref_count":2,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Dynamical universality in a driven quantum fluid of light","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-05-04T09:40:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Direct measurement of static correlation length ξ and dynamical relaxation time τ in the disordered phase of a driven polariton fluid yields τ ∝ ξ^z with z ≈ 2, indicating diffusive dynamics of a non-conserved order parameter.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"the interferometric signal by isolating the first-order sideband in Fourier space𝐼 1. The extracted 𝑔 (1) (𝑟,−𝑟)was verified to be robust against variations of the Fourier filtering window within a reasonable range. The central (DC) component is removed by applying the same spatial filtering procedure, allowing for a normalized reconstruction of the coherence function: 𝑔 (1) (Δ𝑥,Δ𝑦)= 2|𝐼 𝐹𝐹𝑇[𝐼 1(Δ𝑥,Δ𝑦)] | |𝐼 𝐹𝐹𝑇[𝐼 0(Δ𝑥,Δ𝑦)] | (S1) S5 The normalization procedure assumes balanced intensities in the two interferometer arms; this condition was verified experimentally by measuring the individual arm intensities and ensuring symmetric overlap. The profiles of𝑔 (1) (𝑟,−𝑟)are radially averaged to improve the signal to noise ratio and the correlation length is then extracted by fitting the spatial decay of𝑔(1) (|(𝑟)|)with"},{"citing_arxiv_id":"2604.12375","ref_index":36,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Small-System Group: Thermodynamics as a Complete Self-Similarity Limit","primary_cat":"physics.gen-ph","submitted_at":"2026-04-14T07:02:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Thermodynamics emerges as the complete-similarity limit of statistical mechanics when the small-system group Π_B = k_B/(c ℓ³) becomes irrelevant at macroscopic scales.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.10920","ref_index":43,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Non-Monotonic Marangoni Suppression of Hydrodynamic Coarsening in Bicontinuous Liquid-Liquid Phase Separation","primary_cat":"physics.flu-dyn","submitted_at":"2026-04-13T02:35:56+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Surfactant Marangoni stresses suppress hydrodynamic coarsening in bicontinuous phase separation non-monotonically with Péclet number, strongest at intermediate values because of competition between surfactant replenishment and gradient retention.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Korteweg, Sur la forme que prennent les ' equations du mouvements des fluides si l'on tient compte des forces capillaires caus' ees par des variations de densit' e consid' erables mais connues et sur la th' eorie de la capillarit' e dans l'hypoth` ese d'une variation continue de la densit' e, Archives N' eerlandaises des Sciences exactes et naturelles 6 (1901) 1-24. 27 [43] P. C. Hohenberg, B. I. Halperin, Theory of dynamic critical phenomena, Reviews of Modern Physics 49 (3) (1977) 435. https://doi.org/10.1103/RevModPhys.49.435 [44] C.-W. Shu, Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws, Springer Berlin Heidelberg, Berlin, Heidelberg, 1998, pp. 325-432."},{"citing_arxiv_id":"2604.02133","ref_index":50,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Effective Field Theory for Superconducting Phase Transitions","primary_cat":"hep-th","submitted_at":"2026-04-02T15:07:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"An effective field theory for superconducting phase transitions is constructed via Schwinger-Keldysh formalism, reproducing Ginzburg-Landau equations upon truncation while showing overdamped Higgs modes and complex relaxation in holographic validation.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Yoshimura, Y. Akamatsu, and Y. Hirono, \"Effective field theory for dissipative photons from higher-form symmetries,\"arXiv:2601.00605 [hep-th]. [48] A. Kamenev,Field Theory of Non-Equilibrium Systems. Cambridge University Press, 2 ed., 2023. [49] P. Glorioso and H. Liu, \"The second law of thermodynamics from symmetry and unitarity,\"arXiv:1612.07705 [hep-th]. [50] P. C. Hohenberg and B. I. Halperin, \"Theory of dynamic critical phenomena,\"Rev. Mod. Phys.49(Jul, 1977) 435-479. https://link.aps.org/doi/10.1103/RevModPhys.49.435. [51] Y. Bu, X. Sun, and B. Zhang, \"Holographic Schwinger-Keldysh field theory of SU(2) diffusion,\"JHEP08(2022) 223,arXiv:2205.00195 [hep-th]. [52] M. Flory, S. Grieninger, and S. Morales-Tejera, \"Critical and near-critical relaxation of"},{"citing_arxiv_id":"2602.08022","ref_index":34,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Linear Response and Optimal Fingerprinting for Nonautonomous Systems","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-02-08T15:53:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Extends linear response theory to nonautonomous systems and applies it to optimal fingerprinting for attributing changes to multiple forcings in time-dependent backgrounds, with numerical tests on a climate model.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"correlation between generic observables becomes subexponential [32], as a result of the closure of the so-called spectral gap, which is associated with the real part of the first subdominant eigenvalue of the Kolmogorov operator. This provides a solid foundation [33] to the theory of critical slowing down, which was first introduced in the context of second order phase transitions [34] and then widely used in the context of tipping points research [35-37]. The practical implementation of the spectral response theory relies on the choice of the Kolmogorov dictionary [29], and currently benefits from the extremely encouraging development of accurate, efficient, and mathematically sound variants of the so-called extended dynamical"}],"limit":50,"offset":0}