{"total":15,"items":[{"citing_arxiv_id":"2606.30270","ref_index":25,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Cyclic Attractor Detection in Boolean Network Dynamics under Local Logical Constraints","primary_cat":"cs.CC","submitted_at":"2026-06-29T13:17:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"For every fixed k ≥ 2 the cyclic attractor detection problem is NP-complete precisely when the local Boolean function class contains majority-like self-dual rules or mixed conjunctive-disjunctive monotone families, and polynomial-time solvable in all other Post classes.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.24657","ref_index":7,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Limited surface mobility inhibits stable glass formation for 2-ethyl-1-hexanol","primary_cat":"cond-mat.soft","submitted_at":"2026-06-23T14:49:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Vapor deposition experiments show 2-ethyl-1-hexanol glass kinetic stability rises sharply with slower deposition rates, attributed to surface mobility more than 4 orders of magnitude lower than ethylcyclohexane at 0.85 Tg.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.27150","ref_index":16,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"The butterflies' effects","primary_cat":"math.SP","submitted_at":"2026-05-26T15:12:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Spectral butterflies form in parameter-dependent Schrödinger operators on weighted Delone sets and reflect fractal self-similar structures, with the framework extending across dimensions and to non-Abelian groups.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"In the joint work [18], periodic approximations of irrational frequencies, together with a symbolic encoding of the spectral bands (see Section 5.1), are used to represent the spectrum as the boundary of a spectral tree (see Section 5.2). This construction is in- spired by a coding scheme introduced by Raymond [207] for large coupling constants that control the amplitude of the potential. His approach was revisited and extended in [16], incorporating recent advances from [18]. A key achievement of [18] was the extension of this symbolic encoding to all non-zero coupling constants. Together with the spectral tree representation, these developments ultimately lead to a resolution of thedry ten Martini problem(DTMP) for Sturmian Hamiltonians, as detailed in Section 5.3. The DTMP originated in the study of the almost Mathieu operator (the"},{"citing_arxiv_id":"2605.11138","ref_index":10,"ref_count":2,"confidence":0.5,"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":"stochastic fluctuations suppress the formation of ordered structures. The spontaneous formation of ordered domains, characterized by the dynamics of domain walls, represents the emergence of non-trivial correlations within the stochastic background. Critical behavior is characterized by the competition between pixel ordering and power-law fluctuations encoded in the correlation matrix [10]. This work relates the methodology developed in [1-8] with signal detection in high-NSR regimes, where traditional analysis is most constrained. In data science, raw data often take the form of large matricesX∈RN×P, whereNis the sample size (e.g., the number of images in the dataset) andPrepresents the dimensionality of the data (e.g., the number of pixels in the images)."},{"citing_arxiv_id":"2605.06705","ref_index":21,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Emergence of Tsallis Statistics from a Self-Referential Nonlinear Operator: A Variational Framework","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-06T16:14:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Tsallis q-exponential distributions arise by minimizing a free energy built from a self-consistency entropy defined via a nonlinear operator Omega, with q = alpha + beta obtained directly from the operator's fixed-point structure.","context_count":1,"top_context_role":"background","top_context_polarity":"support","context_text":"The derivation follows a standard Landau expansion and is therefore physically controlled but not fully rigorous in a functional-analytic sense. A more detailed justification of the expansion coefficients is provided in Appendix B. Remark 1. For q ≤ 1, Tc ≤ 0: the uniform phase is stable for all T ≥ 0, consistent with known BG stability results [21,22]. Remark 2. The dependence Tc ∝ 1/(q−1) implies that systems with stronger non -extensive feedback (large q) have elevated critical temperatures: non -local self -referential coupling promotes symmetry breaking at higher temperatures than in BG systems [10,12]. The dependence on λ₁ - the principal eigenvalue of the feedback operator ℱ - shows that stronger"},{"citing_arxiv_id":"2605.02670","ref_index":11,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Efficient generation of Gaussian random fields on metric graphs via domain decomposition and mass matrix lumping","primary_cat":"math.NA","submitted_at":"2026-05-04T14:51:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Neumann-Neumann decomposition plus mass lumping enables fast sampling of Gaussian random fields on metric graphs while preserving theoretical convergence rates of the underlying finite-element scheme.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.02483","ref_index":29,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"A unified equation for saturation magnetization and spin transport in weakly disordered ferromagnets","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-04T11:34:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A unified equation describes saturation magnetization loss from finite-size effects in weakly disordered spin-1/2 ferromagnets and yields a unified Bloch equation plus spin transport expression.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Ritzmann, D. Hinzke, A. Kehlberger, E.-J. Guo, M. Kl¨ aui, and U. Nowak, Magnetic field control of the spin Seebeck effect, Phys. Rev. B92, 174411 (2015). 10.1103/PhysRevB.92.174411 [28] Y. Wang, J. Xia, H. Xu, G. Lan, X. Han, and G. Yu, Magnons in van der Waals Antiferromag- netic Materials, Adv. Funct. Mater.36, e17690 (2026). 10.1002/adfm.202517690 [29] S. Cojocaru, A. Naddeo, and R. Citro, Modification of the Bloch law in ferromagnetic nanostructures, Euro phys. Lett. (EPL)106, 17001 (2014). 10.1209/0295- 5075/106/17001 [30] S. Maekawa, T. Kikkawa, H. Chudo, J. Ieda, and E. Saitoh, Spin and spin current-From fundamentals to recent progress, J. Appl. Phys.133, 020902 (2023). 10.1063/5.0133335 [31] D."},{"citing_arxiv_id":"2604.27729","ref_index":15,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"On the proposed concept of mechanical phasons in Ni-Mn-Ga modulated martensite","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-04-30T11:21:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A simple mechanical model shows that modulation phasons in Ni-Mn-Ga 10M martensite relax shear loadings for commensurate and weakly incommensurate modulations but not for strongly incommensurate ones, explaining anomalous elastic behavior and related lattice properties.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"This discrepancy is too large to be ascribed to the limited accuracy and reliability of first principles calculations, although the size and complexity of the 10M unit cell and the effect of magnetism may put these both under question. Moreover, these calculations are also strongly supported by inelastic neutron scattering (INS) results: Shapiro et al. [15] performed INS experiments on incommensurate 10M Ni-Mn-Ga crystals, and have determined the slope of the TA2 phonon branch in the[ζζ0]direction to be 1.6 mm.µs−1, which corresponds toc55 = 20.5GPa. The same result was later confirmed independently by Ener et al. [16]. In other words, at crystal-lattice lengthscales where the INS interaction takes place, the 10M lattice is indeed as stiff as predicted by the first-principles"},{"citing_arxiv_id":"2604.16631","ref_index":33,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Quantum Reference Frames and Correlation Geometry","primary_cat":"math-ph","submitted_at":"2026-04-17T18:39:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Correlation geometry underlies causal fermion systems by providing a thermodynamic-style description of physical systems that incorporates gauge symmetries and diffeomorphisms via the principle of unitary equivalence.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.12546","ref_index":56,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Predicting success of cooperators across arbitrary heterogeneous environmental landscapes","primary_cat":"q-bio.PE","submitted_at":"2026-04-14T10:17:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A single spatial correlation index predicts cooperator fixation across arbitrary heterogeneous landscapes, with segregated environments enhancing and intermixed ones suppressing cooperation under weak selection.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"provides a benefit b at a personal cost c, while defectors incur no costs and provide no benefits. Fitness is linearly derived from payoff, scaled by a selection-intensity parameter w (0 < w < 1) (see Supplementary Note 1). We consider lattice graph population structures: a one-dimensional cycle with degree k = 2 and a two-dimensional square lattice with degree k = 4 . Evolutionary dynamics follows a spatial Moran death-birth process [ 56, 57]. The fixation probability ρC of a single randomly placed cooperator is our primary measure of cooperative success. Payoffs and the environmental landscape. Environmental heterogeneity is introduced by assigning a rich or poor condition to each node, affecting the benefit of cooperation while keeping the cost constant. Cooperators in poor locations provide benefit, bpoor and in rich locations, brich."},{"citing_arxiv_id":"2506.22436","ref_index":73,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Is Lindblad for me?","primary_cat":"quant-ph","submitted_at":"2025-06-27T17:59:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A review that contrasts common assumptions about the Lindblad equation with refined expectations drawn from examples, culminating in a checklist for assessing its breakdown.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"for weak interactions between the subsystems and for times before the timescale required to fully thermalize the system. Whether the approximation is accurate or not depends on the particular case at hand [55, 57, 64-70], although there are some general attempts [52, 71]. Nevertheless, the resulting lack of (complete) thermalization can lead to inconsistent physical predictions [72,73]. See also [74] for a discussion on the relation between perturbation theory , 19The other possible jump operator σ+ would correspond to absorption of energy from the bath, but this cannot happen if the latter is in the ground state. 20It should be evident that in the present formalism, thermalization is enforced by the dissipative part of the Lindblad dynamics (the jump operators), and not by the system dynamics (as it happens for isolated quantum"},{"citing_arxiv_id":"2410.19652","ref_index":4,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Scattering makes a difference in circular dichroic angle-resolved photoemission","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-10-25T15:55:46+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Scattering and interference dominate circular-dichroic ARPES signals in graphene and WSe2, complicating extraction of initial-state orbital angular momentum.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2405.11608","ref_index":18,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Private Delegated Quantum Computing for User-Level and Industry-Level Settings","primary_cat":"quant-ph","submitted_at":"2024-05-19T16:36:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Presents a hierarchy of private delegated quantum computation protocols separating state privacy, transcript ambiguity, and output privacy under stated leakage and collusion assumptions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2312.09014","ref_index":25,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Hole doping and electronic correlations in Cr-substituted BaFe$_{2}$As$_{2}$","primary_cat":"cond-mat.str-el","submitted_at":"2023-12-14T15:03:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Cr substitution induces hole doping and Hund's correlations in BaFe2As2, with superconductivity suppressed by local-moment competition instead of Fermi-surface evolution.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2105.05208","ref_index":9,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Challenges for $\\Lambda$CDM: An update","primary_cat":"astro-ph.CO","submitted_at":"2021-05-11T17:17:34+00:00","verdict":"ACCEPT","verdict_confidence":"MODERATE","novelty_score":3.0,"formal_verification":"none","one_line_summary":"The review updates the status of multiple cosmological and astrophysical signals that appear inconsistent with LambdaCDM as defined by the Cosmological Principle, General Relativity, and Planck18 parameters.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}