{"total":12,"items":[{"citing_arxiv_id":"2606.04897","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Experimental observation of three-dimensional Anderson localization of electromagnetic waves","primary_cat":"cond-mat.dis-nn","submitted_at":"2026-06-03T13:57:56+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First experimental demonstration of 3D Anderson localization of microwaves in disordered metal aggregates, distinguished from diffusion via scaling analysis of transmitted beam width.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.29745","ref_index":12,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Geometry and localization: Probing Localization Landscape Theory on the Bethe Lattice","primary_cat":"cond-mat.dis-nn","submitted_at":"2026-05-28T10:42:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"On the Bethe lattice the LLT percolation transition is mean-field while the Anderson transition is not, showing LLT reproduces some low-disorder features but fails to capture quantum critical properties.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.25098","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Three-dimensional Anderson localization of light in dielectric disorder","primary_cat":"physics.optics","submitted_at":"2026-05-24T14:24:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Time-domain Maxwell simulations of disordered high-index particle packs yield dynamical, spectral, and spatial signatures consistent with three-dimensional Anderson localization of vector light.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21441","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Observation of a tripartite quantum phase for coexisting extended, localized, and critical states","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-05-20T17:30:28+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Experimental observation of coexisting extended, localized, and critical states in a quasiperiodic Floquet-modulated orbital optical lattice using ultracold atoms.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.17953","ref_index":3,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Anderson Transition and Mobility Edges in a Family of 3D Fractal Lattices","primary_cat":"cond-mat.dis-nn","submitted_at":"2026-05-18T07:09:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"In tunable 3D fractal lattices with spectral dimension ds from 2 to 3, the Anderson transition critical disorder increases from 0 to 16.6 and the critical exponent decreases inversely with ds.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.12394","ref_index":2,"ref_count":2,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Detecting overfitting in Neural Networks during long-horizon grokking using Random Matrix Theory","primary_cat":"cs.LG","submitted_at":"2026-05-12T16:57:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Random Matrix Theory detects overfitting via growing Correlation Traps in weight spectra during the anti-grokking phase of neural network training.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"This is the crux of our analysis: such outliers (λtrap,v trap) can be detected directly from the weight matrices and indicate that the layer has developed structured, non-random correlations associated with overfitting. 1The corresponding physics analogies are Anderson localization, Bose-Einstein condensation, and the Curie-Weiss mean-field model of magnetization [2, 5, 6, 25]. 3 (a) (b) (c) Figure 2:Randomized ESDs, MP fits, and emergence of Correlation Traps.(a) Example of the ESD of Xrand compared with a Marchenko-Pastur (MP) fit. In a self-averaging randomized layer, the spectrum is described by the MP bulk and no large right-edge outliers remain. (b,c) Examples of trapped randomized spectra from Layer 2 of the MLP."},{"citing_arxiv_id":"2605.04273","ref_index":255,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Polyamorphism in Glassy Network Materials","primary_cat":"cond-mat.soft","submitted_at":"2026-05-05T20:13:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A tunable microscopic model of network liquids with a liquid-liquid phase transition, analyzed via RFOT theory, predicts nanonucleation near the glass transition and links thermodynamic and kinetic anomalies when matched to water-like conditions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.24829","ref_index":20,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"The Legacy of Enrico Fermi to Varenna","primary_cat":"physics.hist-ph","submitted_at":"2026-04-27T17:00:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"UNKNOWN","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Enrico Fermi's legacy from his Varenna lectures has shaped milestones in laser spectroscopy, Bose-Einstein condensation, and quantum information science.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"\"Nano Optics and Atomics: Transport of Light and Matter Waves\" that took place in Villa Monastero inVarennaonLakeComobetween23rdJuneand3rdJuly2009.ThecoursewasdirectedbyR.Kaiser and D. S. Wiersma, with the support of the scientific secretary L. Fallani. Copyright Società Italiana di Fisica (SIF), reproduced with permission. simulation of Anderson localization [20] using atoms in disordered optical potentials. Alain Aspect described this period as a \"friendly competition\" between the French and Italian scientific communities that accelerated progress in the field. Later in 2014, the dual role in organizational support and scientific innovation of Giacomo Roati was instrumental to the success of course 191 (Figure 14) that covered the major new"},{"citing_arxiv_id":"2511.05344","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Engineering Anderson Localization in Arbitrary Dimensions with Interacting Quasiperiodic Kicked Bosons","primary_cat":"cond-mat.quant-gas","submitted_at":"2025-11-07T15:39:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Interactions and quasiperiodic driving in the Lieb-Liniger kicked-boson model generate synthetic dimensions that realize Anderson localization and its critical behavior in up to four effective dimensions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2507.06286","ref_index":23,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Krylov Complexity","primary_cat":"hep-th","submitted_at":"2025-07-08T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Krylov complexity is a canonical, parameter-independent measure of operator spreading that probes chaotic dynamics to late times and admits a geometric interpretation in holographic duals.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Anti-de Sitter space in dimensiond+1 is the unique maximally symmetric solution to Einstein's equations with a negative cosmological constant,Λ < 0: Rµν − 1 2 Rgµν + Λgµν = 0 . (22) A geometric way to construct this solution is by considering the embedded hyperboloid of constant curvature in flat space of dimension d + 2, obeying the quadratic −X2 0 − X2 d+1 + X2 1 + · · · + X2 d = −ℓ2 . (23) For the case of AdS2 this hyperboloidal embedding can be visualized as follows: X1 X0 X3 Note that we can see this quadratic equation as a bilinear with the somewhat unusual 'two-time' signature quadratic form (−, +, · · · , +−). If this were instead the quadric form with all pluses, we would recognize this as the inner product of two standard vectors inRd+2 and we would conclude that the quadratic form is invariant under the orthogonal group"},{"citing_arxiv_id":"2405.12525","ref_index":7,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Cache Blocking of Distributed-Memory Parallel Matrix Power Kernels","primary_cat":"cs.DC","submitted_at":"2024-05-21T06:30:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Introduces Distributed Level-Blocked MPK combining RACE cache blocking with MPI, reporting substantial speedups up to 4x on 832 cores for matrix power kernels across scientific sparse matrices.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2111.11914","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Non-Hermitian pseudo mobility edge in a coupled chain system","primary_cat":"cond-mat.mes-hall","submitted_at":"2021-11-23T14:55:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Coupling a skin-localized non-Hermitian chain to a delocalized chain induces a pseudo mobility edge in complex energy that separates localized and extended states, with a quantized winding number characterizing transitions under mixed boundary conditions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}