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Physics

arXiv preprints from January 1, 2026 through September 21, 2026 — 19:42:28 EST

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Posted in astro-ph.GA · 2026-08-27 · David Lomeli, Kedron Silsbee, Alexei Ivlev, Marta Obolentseva

Map of the Interstellar Continuum FUV Field within 800 Parsecs

The far-ultraviolet (FUV) field, consisting of photons with energies between 6 and 13.6 electron volts, plays an important role in the chemical and thermodynamical evolution of the interstellar medium. FUV continuum radiation is produced by bright stars in the galaxy and absorbed by interstellar dust. We used newly available maps of...

💬 0 commentsarXiv:2608.27400v1PDF
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Posted in quant-ph · 2026-08-27 · Shunji Matsuura, Yoji Kawamura, Joseph Salfi, Satoshi Iso

Krylov Break Times from an Inhomogeneous Lieb--Robinson Light Cone

Krylov and Lanczos approximations are used in quantum dynamics, quantum subspace methods, and Hamiltonian learning. A practical question is how long an $m$-dimensional Krylov truncation can be trusted. We argue that this time is fixed by causal propagation on the associated Jacobi chain. The relevant distance is not the Krylov index...

💬 0 commentsarXiv:2608.27399v1PDF
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Posted in astro-ph.GA · 2026-08-27 · Hannah V. Bish, J. E. G. Peek, Catherine Zucker, Karl D. Gordon, Claire E. Murray, Susan E. Clark, Mathieu Willems, Erika Hamden

LightCube: A Parsec-Resolution 3D Model of the Local Far-Ultraviolet Interstellar Radiation Field

We present a three-dimensional model of the local interstellar radiation field (ISRF) in the ultraviolet (UV). Using UV flux measurements from the TD1 catalog and stellar distances from Gaia and Hipparcos, we construct a catalog of stars that we expect to dominate the UV flux in the nearby Galaxy. We use the radiative transfer code...

💬 0 commentsarXiv:2608.27389v1PDF
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Posted in hep-th · 2026-08-27 · Omer Guleryuz

Quantum Selection of Classical Histories

Can a finite quantum episode populate a classical future that the same prepared state never reaches deterministically? We show that it can, using inflation as a cosmological laboratory. In our supergravity realization, two classical continuations already exist, but the prepared state reaches only one without noise. A stable entropy...

💬 0 commentsarXiv:2608.27388v1PDF
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Posted in quant-ph · 2026-08-27 · Zhanhai Yu, Di Xiang, Xiaotian Zhang, Hao Zhang

Stochastic transport of a Goldstone mode in a self-organized atomic crystal

Spontaneous breaking of a continuous symmetry produces a massless Goldstone mode that can evolve across a degenerate manifold at zero energy cost. Goldstone modes have been identified primarily through excitation spectra, mode softening or collective oscillations. However, their time-domain transport under intrinsic fluctuations and...

💬 0 commentsarXiv:2608.27387v1PDF
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Posted in physics.chem-ph · 2026-08-27 · Jiří Suchan, B. Scott Fales, Benjamin G. Levine, Eva Muchová, Petr Slavíček

Real-Time Emergence of Charge-Transfer-to-Solvent States from Core Excitation

Charge-transfer-to-solvent (CTTS) excitations provide a chemically central route to generating hydrated electrons and initiating redox chemistry in solution, yet the earliest stage of CTTS---the formation of the excited state itself---is usually treated as instantaneous. Here we present a time-domain perspective of how CTTS character...

💬 0 commentsarXiv:2608.27385v1PDF
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Posted in astro-ph.CO · 2026-08-27 · Darby M. Kramer, Alexander van Engelen, Frank J. Qu, Christopher Cain, Irene Abril-Cabezas, J. Richard Bond, Vera Gluscevic, Carlos Hervías-Caimapo, Niall MacCrann, Mathew S. Madhavacheril, Jeff McMahon, Toshiya Namikawa, Bruce Partridge, Emmanuel Schaan, Neelima Sehgal, Cristóbal Sifón, Ed Wollack

The Atacama Cosmology Telescope: Constraints on the anisotropic screening and birefringence effects with DR6

While we have learned much from recent surveys of the mm-wave sky, many secondary anisotropies of the CMB remain under-explored. We consider two of these here: the anisotropic screening induced by Thomson scattering of CMB photons off free electrons, and cosmic birefringence, the rotation of CMB polarization due to parity-violating...

💬 0 commentsarXiv:2608.27458v1PDF
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Posted in quant-ph · 2026-08-27 · Graham Van Goffrier, Debasish Banerjee, Bipasha Chakraborty, Emilie Huffman

Spectral Fingerprints of Gauge Theories on a Quantum Computer

Maximally mixed state spectral sampling is an unbiased quantum algorithm that allows for extraction of a finite-resolution spectral distribution from a Hamiltonian over potentially the entire allowed range of energies. We show how it may be focused on any desired area of the spectrum in order to learn about the full...

💬 0 commentsarXiv:2608.27457v1PDF
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Posted in cond-mat.str-el · 2026-08-27 · Zhengyan Darius Shi

Metallogenic quantum criticality: Fermi surface nucleation at transitions between gapped phases

Continuous quantum phase transitions in interacting many-body systems exhibit universal phenomena that are largely independent of microscopic details. An organizing principle distilled from canonical examples such as the magnetic transition in Ising models is that the low-energy physics of transitions between gapped phases is governed...

💬 0 commentsarXiv:2608.27453v1PDF
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Posted in cond-mat.mes-hall · 2026-08-27 · Binayyak Bhusan Roy, Jay Deep Sau, Sumanta Tewari

Distinguishing Quantum Capacitance Signatures of a Topological Majorana Wire from a Normal Wire Segment

Majorana zero modes (MZMs) are spatially separated, near-zero-energy excitations expected at the ends of a topological superconducting (TS) wire. A quantum-dot interferometer can be used to probe the quantum capacitance of the TS wire, and the location and magnitude of the capacitance resonances provide information about the MZMs,...

💬 0 commentsarXiv:2608.27452v1PDF
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Posted in hep-th · 2026-08-27 · Le-Feng Chen, Kilar Zhang

Proof of the AGT Conjecture at Generic $β$

We give an all-level proof of the four-point $SU(2)$ AGT correspondence with four fundamental hypermultiplets at generic $β=-ε_1/ε_2$, by proving an all-level factorization formula for Selberg averages of generalized Jack polynomials. Taking a coefficientwise Jack limit of the generalized Macdonald Pieri rule, we obtain the required...

💬 0 commentsarXiv:2608.27447v1PDF
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Posted in cond-mat.str-el · 2026-08-27 · Jonah Herzog-Arbeitman, Eslam Khalaf, Zhaoyu Han

Exact Stiffness and Dynamical Responses from Fock-Space Fragmentation

Exactly solvable quantum many-body models are rare, and even when their spectra are algebraically organized, dynamical responses generally remain difficult to obtain because they probe an extensive number of excited states. Here we show that quantum geometric nesting (QGN) models admit an unusually strong form of solvability rooted in...

💬 0 commentsarXiv:2608.27446v1PDF
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Posted in cond-mat.mes-hall · 2026-08-27 · Elena Derunova, Mazhar N. Ali

Band's Geometry Origin of Quantum Spin Transport Phenomena

We develop a geometric description of spin-dependent transport based on the local geometric structure of electronic bands and the Fermi surfaces. For quasi-two-dimensional systems, we show that hyperbolic regions of constant-energy surfaces generate a geometrical contribution to the Fermi velocity that couples naturally to electron...

💬 0 commentsarXiv:2608.27445v1PDF
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Posted in cond-mat.mes-hall · 2026-08-27 · Mario Di Luca, Emily Hajigeorgiou, Ning Ma, Alexandra Waldherr, Kenji Watanabe, Takashi Taniguchi, Mitali Banerjee

Trapping $e/4$ quasiparticles in bilayer graphene

Measuring the charge of the quasiparticles hosted by even-denominator fractional quantum Hall (FQH) states is essential to identify the topology of their ground state. Here, we use a gate-defined antidot in bilayer graphene, with an additional gate to control only the antidot potential, to measure the charge of the quasiparticles...

💬 0 commentsarXiv:2608.27444v1PDF
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Posted in quant-ph · 2026-08-27 · Ratul Thakur, Sthitadhi Roy

Dynamics of local quantum information in random unitary circuits

The physics of information scrambling in quantum many-body systems is intimately related to thermalisation and emergence of chaos. However, its standard characterisation through bipartite entanglement or operator growth remains inherently coarse-grained, obscuring the spatiotemporal anatomy of how quantum information flows between...

💬 0 commentsarXiv:2608.27440v1PDF
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Posted in astro-ph.SR · 2026-08-27 · András Gáspár, Jarron M. Leisenring, Schuyler Grace Wolff, Kellen Lawson, George H. Rieke, Dingshan Deng, Marcia J. Rieke, Antranik A. Sefilian, Charles Beichman, Joshua B. Lovell, John Krist, Marie Ygouf, Jorge Llop-Sayson, Geoffrey Bryden, Christopher C. Stark, Christine H. Chen

The JWST/NIRCam Scattered Light Disks GTO 2780 program: panchromatic coronagraphic imaging of the HD 10647, HD 32297, HD 61005, HD 107146, and HD 181327 debris disk systems

Debris disks, composed of rocks, boulders, planetesimals, and the dust produced in their collisions, present the most readily observable components of mature planetary systems. They also serve as valuable diagnostic tools, enabling studies of planetary dynamical interactions and mineral compositions. Observed from optical to radio...

💬 0 commentsarXiv:2608.27437v1PDF
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Posted in nlin.AO · 2026-08-27 · Kai Tokunaga

Low-Dimensional Reduction Theory for Populations of Phase Oscillators with a Gaussian Frequency Distribution

Low-dimensional reduction theories such as the Ott-Antonsen ansatz have played a crucial role in the study of populations of coupled oscillators. Their application, however, has largely been restricted to systems with frequency distributions of rational-function form, such as the Cauchy distribution. For such distributions, the...

💬 0 commentsarXiv:2608.27436v1PDF
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Posted in cond-mat.mes-hall · 2026-08-27 · Jianxiong Zhai, Zelei Zhang, Jiawei Yan

Occupation-Driven Josephson Diode in a Symmetric Junction

We propose a Josephson diode mechanism in which nonreciprocity arises not from a conventional asymmetric Andreev spectrum but from nonequilibrium occupation of the current-carrying states engineered by attached reservoirs. We realize this mechanism in a double-quantum-dot junction, where a phase-textured nonlocal reservoir acts as a...

💬 0 commentsarXiv:2608.27213v1PDF
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Posted in physics.med-ph · 2026-08-27 · Jinyang Yu, Oliver Gödicke, Frederik B. Laun, Obada T. Alhalabi, Iris A. Kohler, Jürgen Hesser, Sandro M. Krieg, Bogdana Suchorska, Heinz-Peter Schlemmer, Mark E. Ladd, David Bonekamp, Johann M. E. Jende, Tristan A. Kuder

Constrained estimation of rotational invariants of the cumulant expansion (RICE) for rapid tensor-valued diffusion MRI

Purpose: To complement 1.5-minute measurements of common tensor-valued diffusion MRI (dMRI) markers with rapid constrained fitting. Methods: Fast dMRI protocols for obtaining rotational invariants of the cumulant expansion (RICE) were paired with constrained weighted linear least squares (CWLLS) to stabilize the more fragile WLLS...

💬 0 commentsarXiv:2608.27212v1PDF
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Posted in quant-ph · 2026-08-27 · Dimiter Ostrev

The Find Rows and Columns and Decode algorithm for quantum expander codes

A new adaptation of the Find Erasures and Decode algorithm from classical to quantum expander codes is presented. It runs in linear time and is parallelizable to logarithmic depth. Compared to Small Set Flip and Small Set Find, the new algorithm avoids the overhead of considering the subsets of stabilizer generators, requires less...

💬 0 commentsarXiv:2608.27211v1PDF
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Posted in physics.soc-ph · 2026-08-27 · Jialu Zhang, Guanyu Zhang, Leyang Xue, Peng-Bi Cui

Distinct routes to phase transitions in spatial activation systems

Threshold-driven activation governs a wide range of collective phenomena, yet the microscopic origins of its phase transitions in spatial systems remain unresolved.Here, we show that spatial activation systems undergo multiple distinct routes to phase transitions, controlled by a single parameter---the interaction range.We uncover a...

💬 0 commentsarXiv:2608.27204v1PDF
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Posted in quant-ph · 2026-08-27 · Mario Berta, Hao-Chung Cheng, Roberto Rubboli, Marco Tomamichel

Strong Converse Exponent of Quantum State Merging

We determine the strong converse exponent for the entanglement cost of quantum state merging, showing that it is characterized by the optimized $α$-$z$ conditional Rényi entropies with $z=α/2\in[1/2,1]$. This contrasts with the sandwiched conditional Rényi entropies that typically govern strong converse exponents in quantum...

💬 0 commentsarXiv:2608.27202v1PDF
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Posted in cond-mat.str-el · 2026-08-27 · Mercè Roig, Jannik Gondolf, Andreas Kreisel, Brian M. Andersen, Daniel F. Agterberg

Multi-orbital physics in inverse Lieb lattice altermagnets

The inverse Lieb lattice has recently emerged as a promising platform for altermagnetism, with several materials with this structure proposed as $d$-wave altermagnetic candidates. Here, we develop a symmetry-based microscopic Hamiltonian for these materials that includes both sublattice and orbital degrees of freedom, going beyond the...

💬 0 commentsarXiv:2608.27200v1PDF
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Posted in astro-ph.HE · 2026-08-27 · Saikat Das, Soebur Razzaque, Justin D. Finke, Siyao Xu

Testing Narrow-jet Gamma-Ray Bursts as Sources of Ultrahigh-Energy Cosmic Rays

Gamma-ray bursts (GRBs) have long been considered candidate sources of ultrahigh-energy cosmic rays (UHECRs) due to their large energy release and relativistic outflows. The detection of multi-TeV $γ$-rays from GRB~221009A and its rarity have renewed interest in this connection and motivate considering an additional narrow-jet long...

💬 0 commentsarXiv:2608.27197v1PDF
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Posted in cond-mat.mes-hall · 2026-08-27 · Ashutosh Singh, Hongjing Xu, Xielin Wang, Kohei Fujiwara, Atsushi Tsukazaki, Shengxi Huang, Andrey Baydin, Junichiro Kono, Alexey Belyanin

Terahertz anomalous Hall effect in magnetic Weyl semimetal Co$_3$Sn$_2$S$_2$

Time-reversal-symmetry-broken Weyl semimetals are known to have at least two nodes in their electronic band structure, separated in momentum space and acting as sources and sinks of Berry curvature. This gives rise to a transverse Hall conductivity, known as the anomalous Hall effect (AHE), which, in the simplest two-node picture, is...

💬 0 commentsarXiv:2608.27195v1PDF