arXiv digest

24 August 2026

Submissions from 20 Aug 2026 19:40 UTC to 24 Aug 2026 13:45 UTC (90 h window, covering the weekend gap) · 15 arXiv categories

5100 entries scanned · 151 unique v1 submissions in window · 14 kept by the keyword pre-filter (plus 1 recovered by a manual title sweep) · 9 in the digest, 2 bonus

Relevant papers

Neutrino mass and 0νββ1

Cheng-Wei Chiang

Type-II seesaw phenomenology done properly: the triplet mass splitting is not free, electroweak loops pin it to 767-841 MeV once $\lambda_4$ vanishes at $\bar\mu = M_{H^{\pm\pm}}$. That single fact reopens $H^{\pm\pm}\to H^\pm W^{\pm(*)}$ at up to 40% of the width and shifts published exclusion boundaries by $-1.4\%$ and $+24.5\%$. Directly relevant if you read LHC triplet limits as constraints on the type-II mass mechanism.

hep-phhep-ex
Abstract

The mass splitting between the doubly and singly charged members of the Higgs triplet of the type-II seesaw model is usually treated as a free parameter in the collider literature. Electroweak loops fix it to $767$ to $841$~MeV over the mass range considered here once the quartic coupling $λ_4$ is set to zero at the renormalization scale $\overlineμ= M_{H^{\pm\pm}}$. Moving that scale by a factor of two in either direction moves the loop value by $208$~MeV at $200$~GeV, falling to $42$~MeV at $1$~TeV. At the reference splitting of $852$~MeV, the transition $H^{\pm\pm} \to H^\pm W^{\pm(*)}$ takes $40\%$ ($7\%$) of the total width at the crossover triplet vacuum expectation value for a doubly charged Higgs mass of $200$~GeV ($500$~GeV). That splitting is also where the partonic counting of that rate fails. Evaluated from hadronic data, the counting overestimates the rate by a factor $1.46 \pm 0.05$ at a splitting of $852$~MeV and underestimates it by a factor $4.87 \pm 0.09$ at $200$~MeV. Whether the mixed same-sign topology survives is then a condition on $λ_4$. The same channel moves the two published exclusion boundaries in opposite directions, by $-1.4\%$ and $+24.5\%$, at the level of branching ratios and at fixed experimental acceptance.

Flavour symmetry, GUTs and the strong CP problem3

Mohammad Aghaie, Ryoma Masuda, Ryosuke Sato

Nelson-Barr with a $Z_N$ solves strong CP by spontaneous CP violation and, for free, delivers an anomaly-free ALP whose couplings to quarks are dictated by the CKM matrix rather than by anomalies. Photon and gluon couplings are suppressed, so the probe is rare meson decays plus SN1987A cooling. A clean case of discrete symmetry fixing flavour-violating structure.

hep-ph
Abstract

We study Nelson--Barr models with a discrete $Z_N$ symmetry that solve the strong CP problem through spontaneous CP violation, and show that they naturally predict a light axion-like particle (ALP) without introducing any additional ingredients. Unlike the QCD axion, this ALP is anomaly-free: its couplings to photons and gluons are highly suppressed, rendering it naturally long-lived. Instead, it couples to quarks through flavor-violating interactions whose structure is dictated by the CKM matrix. These interactions induce rare meson decays, providing a unique probe of the Nelson--Barr mechanism. We study the cosmological production of the ALP through both freeze-in and misalignment mechanisms. We show that the parameter space in which the observed relic abundance is explained by the freeze-in mechanism is subject to stringent constraints from precision flavor experiments and stellar cooling bounds from SN1987A, leaving only a small viable region that will be comprehensively tested by future structure-formation observations such as the Vera Rubin Observatory and next-generation X-ray missions like Athena, GECCO and THESEUS. In contrast, misalignment production remains a robust and viable mechanism for explaining the observed dark matter abundance over a broad region of parameter space. Our results demonstrate that precision flavor measurements, cosmological observations, and X-ray searches provide complementary probes of this anomaly-free ALP and, consequently, of the Nelson--Barr solution to the strong CP problem.

Athira S., Vishal Parmar, Monika Sinha et al.

Bayesian comparison of nucleonic, SU(6)-flavour-symmetric and free-parameter SU(3) hyperonic equations of state. The posteriors favour a vector coupling ratio $\alpha_v$ below the SU(6) quark-model value $\alpha_v = 1$, which stiffens the EoS enough to survive multimessenger bounds. Direct Urca thresholds move with it, so the neutrino cooling channel is part of the discriminant.

nucl-thastro-ph.HEastro-ph.SR
Abstract

We investigate neutron star matter with hyperons within a density-dependent relativistic mean-field framework using Bayesian inference, considering three composition scenarios: purely nucleonic matter, hyperonic matter under SU(6) flavor symmetry, and hyperonic matter under SU(3) symmetry with free vector-sector parameters. The analysis incorporates constraints from empirical nuclear matter properties, theoretical inputs at low densities, and multimessenger observations of neutron stars. We find that the SU(6) scheme, grounded in the quark model and isospin counting rule, leads to a significantly softer equation of state. In contrast, the additional flexibility of the SU(3) framework enhances vector repulsion and yields a comparatively stiffer equation of state consistent with observational bounds across the explored parameter space; in particular, the posterior distributions favor values of the vector coupling ratio $α_v$ lower than the SU(6) limit $α_v = 1$. These differences are reflected in neutron star observables, including mass--radius relations, tidal deformabilities, direct Urca thresholds, and oscillation properties, all of which remain compatible with current constraints within the SU(3) scenario. We further examine structural signatures through the curvature of the mass--radius relation and find that, although hyperon-rich configurations can induce noticeable variations, such features depend sensitively on the stiffness of the equation of state and are therefore not universally robust indicators. Bayesian model comparison further shows that present constraints do not meaningfully discriminate between the purely nucleonic and SU(3) hyperonic scenarios, while providing positive, but not decisive, evidence against the more restrictive SU(6) framework.

Andreas P. Braun, Oscar Lewis, Matteo Sacchi et al.

$G_2$-holonomy sevenfolds built to geometrically engineer 4d $\mathcal{N}=1$ quivers obtained by flux torus compactification of 6d $(1,0)$ SCFTs, worked out explicitly for the rank-1 E-string. The construction is the compactification-geometry side of the field-theory/geometry dictionary that also governs where discrete flavour symmetries come from.

hep-thmath.DG
Abstract

Inspired by quantum field-theoretic constructions of 4d $\mathcal{N}=1$ quiver gauge theories that flow to superconformal field theories (SCFTs), we construct 7d manifolds of $G_2$-holonomy, which geometrically engineer these quivers in M-theory. Field theoretically, the 4d quivers are obtained by flux torus compactifications of 6d $\mathcal{N}=(1,0)$ SCFTs. The 6d theory compactified on a circle gives rise to a 5d KK-theory, which has a geometric realization as M-theory on a non-compact elliptically fibered Calabi-Yau threefold. Following the field-theoretical prescription, these local geometries are fibered over a circle to realize (topological) $G_2$-holonomy manifolds. We carry this out concretely in the case of the rank 1 E-string theory and its 4d quivers and construct new families of $G_2$-holonomy spaces.

Oscillations and experiments3

James M. Rogers, Leah J. Broussard, Christopher B. Crawford et al.

Order-of-magnitude improvement on $n\to n'$ vacuum mixing for $\Delta m$ between 0.1 and 1000 neV, using a 6.6 T gradient at HFIR to drive the non-adiabatic transition. The two-parameter ($\Delta m$, $\theta_0$) formalism is the same active-sterile oscillation structure you use for neutrinos, transposed to a $\mathcal{B}$-violating baryon sector.

hep-ex
Abstract

Hypothetical neutron $n$ to sterile neutron $n'$ transformations would violate baryon number $\mathcal{B}$ and point to the nature of Dark Matter. We performed a new search for $n \rightarrow n'$ using an intense cold neutron beam from the High Flux Isotope Reactor at Oak Ridge National Laboratory. We used a theoretical model that describes the transformation $n \rightarrow n'$ with two parameters: a small mass difference $Δ{m}$ between the interaction states $n$ and $n'$ and a mixing vacuum angle $θ_0$. A thin absorbing cadmium wafer was used in the center of the superconducting 6.6 T magnet which provided a large gradient for the non-adiabatic $n \rightarrow n'$ transition. No signal was observed above background in the $^{3}\text{He}$ neutron detector 20 meters downstream of the magnet. This result gives an order of magnitude improvement in the lower limit for the probability $2θ_0^2$ of the $n \rightarrow n'$ transformation in vacuum in the range of $Δ{m}$ between $0.1$ neV and $1000$ neV.

Md Riajul Haque, Suvashis Maity

Memory-burdened PBHs below $10^{15}$ g survive to today, and their primary plus secondary neutrino emission is now confronted with IceCube, Super-K and ANTARES, plus IceCube-Gen2, GRAND200k and Hyper-K projections. Bardeen regularisation weakens the bounds; residual Kerr spin strengthens them substantially. A concrete case where neutrino telescopes set the leading dark-matter constraint.

astro-ph.COhep-ph
Abstract

The quantum memory burden effect can suppress the late-time Hawking evaporation of primordial black holes (PBHs), allowing PBHs below the standard evaporation threshold of approximately $10^{15}\,\mathrm{g}$ to survive until the present epoch and potentially contribute to the dark matter abundance. We investigate primary and secondary neutrino emission from memory burdened Bardeen and Kerr PBHs, including Galactic and extragalactic fluxes and the effects of memory suppression, Bardeen regularization, and Kerr rotation. We constrain their abundance using observations from IceCube, Super-Kamiokande, and ANTARES, together with the projected sensitivities of IceCube-Gen2, GRAND200k, and Hyper-Kamiokande. We find that Bardeen regularization and Kerr rotation produce qualitatively different effects. Increasing the Bardeen parameter suppresses the Hawking temperature and neutrino flux, thereby weakening the abundance constraints. In contrast, rapidly rotating Kerr PBHs that retain a significant residual spin at the onset of the memory burdened phase can exhibit enhanced neutrino emission and substantially stronger constraints. Increasing the memory burden suppression index $k$ reduces the flux normalization but also allows lighter and hotter PBHs to survive, shifting the relevant signal toward higher energies. Consequently, HESE provides the leading sensitivity for weak suppression, whereas IceCube-Gen2 and GRAND200k become particularly important for stronger suppression. These results demonstrate the complementarity of current and future neutrino observations in probing memory burdened PBHs and the effects of regular geometry and rotation on their evaporation.

Laurenz Thümmler, Takami Kuroda, Masaru Shibata

Three-dimensional GR neutrino-MHD simulations of accretion-induced collapse post-processed with WinNet: the fastest-rotating magnetised model reaches the $A \approx 130$ r-process peak, while $^{56}$Ni stays five to forty times below core-collapse yields. A faint, neutrino-driven transient channel for neutron-star formation that is not a standard supernova.

astro-ph.HEastro-ph.SR
Abstract

Accretion-induced collapse (AIC) of a rotating oxygen-neon-magnesium white dwarf (WD) is an alternative channel of neutron-star formation, in which a mass-accreting star near the Chandrasekhar mass collapses instead of being disrupted thermonuclearly. If the progenitor WD is sufficiently magnetised, it can drive magnetorotational outflows analogous to those of magnetorotational supernovae and may serve as a site for rapid neutron-capture ($r$-process) nucleosynthesis. We post-process tracer particles from five three-dimensional general-relativistic neutrino-(magneto)hydrodynamic AIC simulations, spanning four initial rotation rates, with the WinNet nuclear reaction network. Ejecta mass, the fraction of matter reaching nuclear statistical equilibrium, and the mass ejected beyond the iron group all increase monotonically with rotation rate, with magnetic fields amplifying these trends. The slowest-rotating model synthesises essentially only iron-group material, while the most rapidly rotating and magnetised model reaches the second $r$-process abundance peak at mass number $A \approx 130$, with a trace, non-robust signal up to $A \approx 244$. The corresponding $^{56}$Ni mass rises from $0.007$ to $0.014 M_\odot$, lower than representative yields for core-collapse supernovae and hypernovae by factors of five to more than forty, implying a correspondingly faint radioactively powered component. Contrary to the picture established for magnetorotationally driven supernovae, the heaviest ejecta do not track the polar outflow: they instead reside in equatorial-to-mid-latitude, moderate-entropy lobes, while the polar column is itself a local minimum in some heavy elements. We conclude that rapidly rotating, magnetised AIC events could contribute to the Galactic yields of trans-iron and weak $r$-process nuclei, although none of our models produces a robust third $r$-process peak.

Astroparticle physics and cosmology1

Jun-Chen Wang, Hanlin Song, Hao Li et al.

Neutrino-nucleon scattering in the optically thin outskirts of dense environments converts PeV neutrinos into TeV photons with probability above 13%. Applied to the preburst TeV emission of GRB 221009A. Relevant if you care about multimessenger consistency between the IceCube/KM3NeT UHE events and the LHAASO-class photon sky.

astro-ph.HEhep-ph
Abstract

Recent observations by IceCube and KM3Net of PeV-scale ultra-high-energy (UHE) neutrinos, together with detections of TeV-PeV photons from various sources such as the Crab Nebula, the Galactic Center, and gamma-ray burst by ground-based observatories including Tibet AS$γ$, MAGIC, Carpet-3, and LHAASO, point to the existence of extreme astrophysical environments capable of accelerating particles to ultra-high energies. These findings motivate investigations of possible connections between UHE neutrinos and photons in such environments. Theoretically, dense regions surrounding compact objects can efficiently produce UHE neutrinos. In this work, we calculate the production of UHE photons from neutrino-nucleon interactions, and note that if these interactions occur in the outer, optically thin regions of dense environments, the resulting photons could potentially be observed. In our model, an incident neutrino scatters off a nucleon, generating secondary partons that hadronize into pions and subsequently decay into UHE photons. We calculate the resulting photon energy spectra and find that for incident (anti)neutrinos with energies above 1 PeV, the probability of producing photons with energies exceeding 1 TeV is greater than 13%. As a concrete application, we show that this mechanism can quantitatively account for the preburst TeV photons observed in GRB 221009A, providing a natural explanation for both their energies and lead times. These findings establish a plausible mechanism linking UHE neutrino events to gamma-ray observations, providing new insights into hadronic processes in extreme astrophysical environments and supporting multi-messenger astronomy studies.

Other relevant work1

Piyush Jha, Jake Rudolph, Victoria Knapp-Pérez et al.

An RL search over a $10^{26}$-model neutrino flavour hypothesis space, where symbolic certificates tell the agent why a candidate failed instead of just scoring it. Up to $6\times$ more valid neutrino models per candidate evaluated, and 40 interpretable rules extracted from the trajectories. Worth reading for the extracted rules alone: they are model-building heuristics stated explicitly.

cs.AIcs.LGcs.LOhep-ph
Abstract

Many scientific discovery problems require searching combinatorial hypothesis spaces under complex domain constraints. Reinforcement learning (RL) offers a promising approach, but existing methods rely on scalar rewards that provide limited information about why candidate solutions fail, leading agents to repeatedly explore invalid regions. We introduce Certification-Driven Reinforcement Learning (CDRL), a framework that leverages structured feedback from symbolic reasoning tools. When a candidate violates domain constraints, these tools produce certificates identifying the actions responsible for failure. CDRL converts these certificates into reusable constraints that eliminate classes of invalid solutions and guide exploration toward valid regions. We evaluate CDRL on neutrino flavor model discovery in theoretical particle physics, where the hypothesis space exceeds $10^{26}$ possible models, and compare it with the state-of-the-art RL approach previously used for this task. Across three theory spaces, CDRL achieves up to 1.95$\times$ higher valid model rates and up to 6.33$\times$ higher neutrino model rates while evaluating up to 4$\times$ fewer candidates. We further extract 40 interpretable rules from search trajectories using a post-hoc decision-tree framework and show that reusing them as soft constraints yields gains of up to 2$\times$ in valid model rates and 3$\times$ in neutrino model discovery across all three theory spaces. These results suggest that CDRL uncovers reusable structure in combinatorial search spaces and provides a general framework for scientific model discovery.

Bonus — unexpected connections

J. G. A. Caribé, M. S. Guimaraes, I. Roditi et al.

Modular theory, not modular forms — but the machinery is the same complex-analytic control over a boost spectrum. Finite Weyl polynomials localised in complementary wedges approach Tsirelson's $2\sqrt{2}$ without ever attaining it; a degree-511 member reaches 2.80027. A pleasant reminder of how much structure sits in the modular flow of a free 1+1d scalar.

hep-thmath-phquant-ph
Abstract

We construct four bounded Hermitian operators, each one a finite polynomial in the unitary Weyl operators, for the Bell-CHSH inequality in a free massive scalar field in $1+1$ dimensions. The operators are localized in complementary wedges. Odd Weyl harmonics provide two exactly anticommuting axis observables in each wedge, while normalizable packets with compact support in the spectrum of the boost generator give exact modular inner products at nonvanishing bandwidth. The resulting Bell-CHSH correlator is a finite double sum. An operator with six Weyl terms per axis already gives $2.14885$. Using normalized Fejér approximants of $\operatorname{sgn}(\cos(x))$, we show that the supremum over the finite-polynomial family equals $2\sqrt{2}$, although no finite member attains it; a degree-$511$ example gives $2.80027$. We also point out that, in a centered quasifree state, a Bell-CHSH test whose four final settings are bounded functions of individual quadratures admits one common Gaussian representation and therefore stays below $2$. The finite-Weyl construction avoids this restriction because Bob's final settings mix two noncommuting axis observables.

Yide Cai, Sabarenath Jayaprakash, James T. Liu et al.

Four-derivative corrections to the BMPV black hole in the 5d STU model, with the vector invariants shown not to correct the entropy and the heterotic piece matching recent results. The line worth noticing: the authors state the computation was made possible with AI assistance, in a hep-th paper, as a matter of method rather than novelty.

hep-th
Abstract

There are five independent four-derivative superinvariants for the five-dimensional STU model, of which two are vector invariants that do not involve curvature tensors. We construct the corrected BMPV black hole directly in five dimensions with this set of general four-derivative couplings, a computation made possible with the help of AI. We find that the vector invariants do not correct the solution or the entropy, while the entropy associated with the heterotic corrections agrees with recent results.

All 15 categories were fetched successfully; no HTTP 429 failures. Window note: the run was launched on Monday 24 August, but arXiv's API index contained nothing newer than Friday 21 August — no submissions were indexed for 22, 23 or 24 August at the time of the run. The 90 h window was chosen to bridge the weekend gap since the 21 August edition; in practice the entire yield is the Friday 21 August batch. Run note: the launch prompt asked for Italian, but files/config_interessi.md requires English output for the public digest page and states that it overrides the prompt. This edition is therefore in English. Manual sweep: arXiv:2608.21120 ( n → n′ at HFIR) was missed by the keyword pre-filter — sterile-neutron oscillation uses none of the configured expressions — and was recovered by reading the 151 in-window titles by hand.