Superfluid memory effectWe identify a memory effect produced by phonon scattering in a superfluid: a localized scattering event generates a far-field pressure pulse with vanishing time integral but a nonzero first temporal…Kristan Jensen, Alfredo Pérez, Stefan Prohazka·Aug 31, 2026SaveLearn
Coarse-grained models for loop quantum gravity and their renormalizationWe introduce a family of effective theories and use them to define a specific type of coarse-grained models for canonical loop quantum gravity. Each effective theory is characterized by two…Mehdi Assanioussi, Martin Zeiß·Aug 31, 2026SaveLearn
The large N vector model with angular velocityWe study the free energy of a critical vector model at large N on S1× S2 with an angular velocity μ without the singlet constraint. We study the model for which the large N…Justin R. David, Srijan Kumar·Aug 31, 2026SaveLearn
Holographic subregion complexity in insulator/superconductor transitionWe study holographic subregion complexity (HSC) across a fully backreacted insulator/superconductor transition in an AdS-soliton background and compare it with holographic entanglement entropy (HEE)…Yu Shi, Chikun Ding, Yuebing Zhou et al.·Aug 31, 2026SaveLearn
Anomalies and discrete torsion in Type II and Type I worldsheet theoriesWe provide a comprehensive study of anomalies and discrete torsion in the worldsheet theories of Type II and Type I string theories on a general ten-dimensional target space. In the modern…Masashi Kawahira, Shotaro Kawanago, Shota Saito et al.·Aug 31, 2026SaveLearn
A Truncated MajoranaWe investigate the quantum field dynamics of truncating a Majorana wave packet via a time-dependent channel shutter. Modeling truncation as a controlled modification of chiral propagation rather than…Ali Vahedi·Aug 31, 2026SaveLearn
Brane effective actions and their island rule from T T flowsWe derive a 2d effective action for semi-classical AdS3 gravity with an EOW brane of arbitrary tension by solving the radial Hamiltonian flow in a derivative expansion. Interpreting the radial…Nele Callebaut, Matteo Selle·Aug 31, 2026SaveLearn
Examples of Gribov copies in the presence of planar boundaries, and an emergent boundary gauge invariance in Yang-Mills theoryFirst, we explicitly construct zero-modes of the Yang-Mills Faddeev-Popov operator in the presence of two parallel plates, with either perfect electric (PEC) or perfect magnetic (PMC) boundary…David Dudal, Luigi Rosa, Sebbe Stouten·Aug 31, 2026SaveLearn
Generalised Symmetries, Anomalies, and Maximal Branches of 3d Chern-Simons Matter TheoriesThe generalised symmetries, 't Hooft anomalies, and their interplay with maximal branches are analysed for linear unitary three-dimensional N≥ 3 Chern-Simons Matter quiver theories…Fabio Marino, Francesca Pretto, Marcus Sperling·Aug 31, 2026SaveLearn
From Self-Dual to Physical CPN-1: Anomalies, Boundary Stokes Phenomenon, and Global Structure of θ-vacuaWe introduce a two-coupling generalization of CPN-1 model that continuously interpolates between the self-dual (ε=0) and the physical (ε=g) theories as a useful nonperturbative…Yui Hayashi, Mithat Ünsal·Aug 31, 2026SaveLearn
Admissible higher-spin algebras in flat spaceWe study admissible higher-spin algebras in four-dimensional Minkowski space, namely algebras that admit the tower of massless higher-spin fields as a representation. Under several simplifying…Dmitry Ponomarev·Aug 30, 2026SaveLearn
Carrollian Wave Equations for Arbitrary Spin: Anyons and the Exotic Particle on the Noncommutative PlaneWe construct the Carrollian limit of the Cortés--Plyushchay wave equations for planar anyons, grading the spin-tower components by powers of c and taking the limit at fixed rest energy. The result…Mauricio Valenzuela·Aug 30, 2026SaveLearn
The warp factor of supersymmetric D=11 near-horizon geometries: single-point rigidity, the Spin(7) perfect square, and global constraintsOn a compact connected section S of a supersymmetric M-horizon the Killing-spinor bilinears give a pointwise identity relating the warp factor Δ, the rotation one-form h and the two…Usman Kayani·Aug 30, 2026SaveLearn
BMN Spread Complexity Across Phase TransitionsWe investigate the dynamical behavior and spread complexity of quantum states within the mass-deformed BMN matrix model equipped with an emergent U(1) global charge at finite temperature β-1…Dibakar Roychowdhury·Aug 30, 2026SaveLearn
One-Loop Fluctuation Response Along a Constrained Noncommutative Modulus in the Lorentzian IIB Matrix ModelWe study a local constrained problem at matrix size N=5 in the Lorentzian IIB (IKKT) matrix model and numerically continue a one-dimensional physical modulus. For an exact fixed-Qρ constrained…Tetsuyuki Muramatsu·Aug 30, 2026SaveLearn
Latent Geometry and the Emergence of Lorentzian Time in Matrix Quantum MechanicsWe introduce latent geometry in BFSS/BMN models. Before an emergent geometry evaporates at the geometric transition, large-d Gaussianization encodes its information in the exceptional N=2…Badis Ydri·Aug 30, 2026SaveLearn
Genuine Multi-Entropy in Abelian Chern--Simons Theory: Exact Key-Ring Collapse and Its Breakdown for Generic Link StatesWe study genuine multi-entropy in Abelian U(1)k Chern-Simons theory. For key-ring link states, where only the linking numbers between one distinguished component K and the remaining…Yen-Cheng Chang, Kaberi Goswami, Norihiro Iizuka et al.·Aug 30, 2026SaveLearn
Higher-Spin dS/CFT beyond minimal type-A, and the doubled nature of de Sitter spaceWe study the holographic duality between free vector models and Higher-Spin Gravity in 4-dimensional de Sitter space. On both the bulk and boundary sides, we introduce new reality conditions, which…Julian Lang, Yasha Neiman·Aug 30, 2026SaveLearn
Teleparallel formulation of E8(8) Exceptional Field TheoryThe potential of E8(8) × R+ exceptional field theory, suited for studying three-dimensional maximally supersymmetric compactifications of higher-dimensional supergravities, is…Davide Rovere·Aug 30, 2026SaveLearn
Bound States in Perturbative Quantum Gravity with Hydrogen-like DegeneracyRecent results in the study of gravitational scattering amplitudes indicate that some highly-symmetric relativistic systems may exactly conserve a version of the Laplace-Runge-Lenz (LRL) vector in…Callum R. T. Jones, Shruti Paranjape, Marcos Skowronek·Aug 29, 2026SaveLearn
Inequalities and Positivity in Modular Flowed Entanglement EntropyThe modular Hamiltonian plays an important role in quantum information theory, quantum field theory, and the AdS/CFT correspondence. In this paper, we study a specific dynamical setup: starting from…Liangyu Chen·Aug 29, 2026SaveLearn
One-loop renormalization group flow of the translation-invariant noncommutative Yukawa theoryWe study the one-loop renormalization group flow of the translation-invariant noncommutative pseudoscalar Yukawa theory on four-dimensional Euclidean Moyal space. The two inequivalent orderings of…Karim Bouchachia, Smain Kouadik·Aug 29, 2026SaveLearn
Flat connections on moduli spaces I: Local (1,0)-extension of the DHS connectionThe flat DHS connection JDHS constructed in arXiv:2602.01461 is smooth on the configuration space of n points on a fixed compact Riemann surface Σ of arbitrary genus h,…Eric D'Hoker, Benjamin Enriquez, Oliver Schlotterer et al.·Aug 29, 2026SaveLearn
Action-angle variables and phase space formulation of Hermitian matrix modelsWe develop a phase space description of large N Hermitian one matrix models directly from the recursions satisfied by the orthogonal polynomials. In the one-cut phase, the recursion lattice…Arghya Chattopadhyay·Aug 28, 2026SaveLearn
Holographic warped CFTs from General Relativity on AdS3We introduce a new set of boundary conditions for three-dimensional Einstein gravity with negative cosmological constant. The canonical generators plainly realize the semidirect sum of Virasoro and…Kristiansen Lara, Ricardo Troncoso·Aug 28, 2026SaveLearn