PaperPanorama

HEP Phenomenology·hep-ph

Fri·Mar 28, 2025

45 papers27 primary·18 cross-listed·reconstructed*

  1. 01*

    From SIMP miracles to WIMP dead ends: navigating the freeze out of MeV-mass dark matter

    Xiaoyong Chu🇨🇳 · Josef Pradler🇦🇹

    We summarize here our studies \cite{Chu:2022xuh,Chu:2023jyb,Chu:2024rrv} on two distinct scenarios for MeV-mass thermal dark matter freeze-out. First, we determine the minimal viable mass for dark matter below tens of MeV, considering annihilation into Standard Model particles, including photons, electrons, and neutrinos. Using a full three-sector abundance calculation, we track heat transfer between sectors and provide accurate thermal annihilation cross sections, particularly for velocity-dependent cases. The results identify fine-tuned regions where neutrino final states permit otherwise excluded p-wave annihilation scenarios. Second, we examine dark matter freeze-out in strongly interacting theories, where the relic abundance can be regulated not only through standard annihilation but also via bound-state formation , enabling effective two-body processes and/or . Together, these studies highlight complementary pathways to thermal MeV-mass dark matter.

    hep-phPoS(2025)·0 citations
  2. 02*

    Mass-unspecific classifiers for mass-dependent searches

    J. A. Aguilar-Saavedra🇪🇸 · S. Rodríguez-Benítez🇪🇸

    Searches for new particles often span a wide range of mass scales, where the shape of potential signals and the SM background varies significantly. We make use of a multivariate method that fully exploits the correlation between signal and background features and the explored mass scale, and is trained on a sample that is balanced across the entire mass range. The classifiers, either a neural network or a boosted decision tree, produce a continuous output across the full mass range and, at a given mass, achieve nearly the same performance as a classifier specifically trained for that mass. The performance of the classifiers is better than the one obtained with parameterised neural networks and similar methods.

    hep-phhep-exEPJC(2026)·0 citations
  3. 03*

    Squeezing Proton Decay and Neutrino Masses: Upper Bounds on Standard Model Extensions

    Arnau Bas i Beneito🇪🇸 · John Gargalionis🇪🇸 · Juan Herrero-Garcia🇪🇸 · Michael A. Schmidt🇦🇺

    Baryon and lepton number are excellent low-energy symmetries of the Standard Model (SM) that tightly constrain the form of its extensions. In this paper we investigate the possibility that these accidental symmetries are violated in the deep UV, in such a way that one multiplet necessary for their violation lives at an intermediate energy scale above the electroweak scale. We write down the simplest effective operators containing each multiplet that may couple linearly to the SM at the renormalisable level and estimate the dominant contribution of the underlying UV model to the pertinent operators in the SMEFT: the dimension-5 Weinberg operator and the baryon-number-violating operators up to dimension 7. Our results are upper bounds on the scale for each multiplet--operator pair, derived from neutrino-oscillation data as well as prospective nucleon-decay searches. We also analyse the possibility that both processes are simultaneously explained within a natural UV model. In addition, we advocate that our framework provides a convenient and digestible way of organising the space of UV models that violate these symmetries.

    hep-phJHEP(2025)·6 citations
  4. 04*

    -violating effects of the neutral triple gauge couplings in production at the LHC

    Artur E. Semushin🇷🇺 · Evgeny Yu. Soldatov🇷🇺 · Anastasia S. Kurova🇷🇺

    The main goal of modern experiments in high-energy physics area is to find deviations from the Standard Model, the theoretical framework which describes data well but is expected to be extended to a more general theory. The anomalous coupling approach provides an opportunity to look for a wide range of new physics effects in different experimental signatures thanks to its model independence. In this work, the neutral triple gauge couplings are considered in channel, and an effective field theory is used to parameterize these couplings in the Lagrangian. Neutral triple gauge couplings are triple interactions between bosons and photons, and some of them violate symmetry. This work presents a study of -sensitive variables in the aforementioned channel using special angular variables and matrix-element-based optimal observables. Based on these variables, expected limits on the coupling parameters are set for the conditions of Run II and Run III at LHC experiments, demonstrating the possibility of studying the -violation using a neutral triple gauge coupling approach and special -sensitive variables.

    hep-phhep-exPRD(2025)·2 citations
  5. 05*

    New Physics Search with the Optical Dump Concept at Future Colliders

    Ivo Schulthess🇩🇪 · Federico Meloni🇩🇪

    Beam-dump experiments offer an opportunity to search for new physics beyond the Standard Model of particle physics. In this work, we explore the use of a high-energy photon beam on a fixed target. Such photons can be produced via Compton backscattering when colliding high-energy electrons with a high-intensity laser pulse, such as in setups of strong-field quantum electrodynamics experiments. We present various options for implementing such photon sources at future facilities and discuss how the photons can be used to search for axion-like particles. We compare the projected sensitivities of the proposed options with existing constraints, projections from current experiments, and direct searches at future colliders.

    hep-phhep-ex9 citations
  6. 06*

    First study of polarized proton-proton scattering with small- helicity evolution

    Daniel Adamiak🇺🇸 · Nicholas Baldonado🇺🇸 · Yuri V. Kovchegov🇺🇸 · Ming Li🇺🇸 · W. Melnitchouk🇺🇸 · Daniel Pitonyak🇺🇸 · Nobuo Sato🇺🇸 · Matthew D. Sievert🇺🇸 · Andrey Tarasov🇺🇸 · Yossathorn Tawabutr🇫🇮

    We perform a phenomenological study of helicity-dependent parton distribution functions (PDFs) using small- helicity evolution equations, incorporating for the first time single-inclusive jet production data in polarized proton-proton () scattering at parton momentum fractions . We also simultaneously include double-longitudinal spin asymmetries in inclusive and semi-inclusive deep-inelastic scattering probing . Employing the polarized small- pure-glue calculation of for the jet production cross section, we modify the large- KPS-CTT evolution equations by setting to replicate the large- (pure-glue) limit, while retaining external quark flavors for the spinor field operators. We find that the data have a considerable impact on the helicity PDFs at small , reducing their uncertainties and leading to a total quark and gluon helicity in the proton for of . Combining our analysis with the a recent JAM helicity PDF analysis of the world polarized data, which includes , we find a total quark and gluon helicity contribution for of between 0.02 and 0.51.

    hep-phhep-exnucl-exnucl-thPRD(2025)·12 citations
  7. 07*

    Properties of solutions by the Schwinger-Dyson equation at finite temperature and density : A four-fermion interaction model

    Hidekazu Tanaka🇯🇵 · Shuji Sasagawa🇯🇵

    In this paper, we examine the properties of the solutions obtained by the Schwinger-Dyson equation (SDE). As a simple example, we consider a two-dimensional model including four-fermion interaction. It is shown that when this model is solved by an iterative method using the SDE at finite density, multiple solutions depending on the initial input values are obtained. We investigate the reasons for this situation by examining the convergence of the solutions obtained by iterative method. We also consider the solution of the SDE using alternative methods. Furthermore, we compare these results with analytical solutions at zero temperature and discuss the relation with the behavior of the effective potential. We extend these considerations to finite temperatures. Based on these analyses, we consider ways to avoid spurious solutions that appear in the iterative method.

    hep-phhep-thPTEP(2025)·0 citations
  8. 08*

    Lepton collider imprints of Inelastic dark matter model

    Wei Liu🇨🇳 · Jin Sun🇰🇷

    We explore the potential for detecting the inelastic dark model (DM) with an additional gauge symmetry at various types of lepton colliders. The new gauge boson resulting from the spontaneous breaking of can act as a portal connecting the Standard Model fermions and DM fermions , thereby facilitating the production of and its decay into DM fermions. The mass difference between the excited DM fermion and the ground DM fermion induces the subsequent decays , where and serve as long lived particles and DM candidate, respectively. For the inelastic DM with a mass in the range of (1-100) GeV, we find that the future lepton colliders can probe many regions not accessible by current experiments and provide greater projected sensitivity than the LHC and Belle in previous studies. This suggests that future colliders can provide complementary exploration of the inelastic dark matter model.

    hep-phPRD(2025)·6 citations
  9. 09*

    Neutrino Theory Overview

    P. S. Bhupal Dev🇺🇸

    The neutrino sector is the least known in the Standard Model. We briefly review the open questions in neutrino physics and the future experimental prospects of answering them. We argue that a synergistic approach at multiple frontiers is needed.

    hep-phSpringer Proc.Phys.(2026)·0 citations
  10. 10*

    Global analysis of fragmentation functions to light neutral hadrons

    Jun Gao🇨🇳 · ChongYang Liu🇨🇳 · Mengyang Li🇨🇳 · XiaoMin Shen🇨🇳 · Hongxi Xing🇨🇳 · Yuxiang Zhao🇨🇳 · Yiyu Zhou🇮🇹

    Fragmentation functions (FFs) are crucial non-perturbative components in quantum chromodynamics (QCD), playing a vital role in predictions and understanding of the hadronization process. In this paper, we present the FFs for , , mesons, and baryons in the context of global QCD analysis. The data included in the fit are from single inclusive annihilation (SIA), semi-inclusive deep-inelastic scattering (SIDIS) and proton-proton collisions, with kinematic cuts carefully applied to ensure validity of collinear factorization and perturbative QCD expansion. For the first time, data from SIDIS and hadron-in-jet production in SIA have been incorporated into the extraction of FFs for light-flavor neutral hadrons. Our analysis reveals that these data play a critical role in constraining the gluon distribution, and in distinguishing between different quark flavors. Pulls from different datasets are also studied by performing alternative fits with systematically subtracting groups of data from the nominal fit. For the quality of the fit, good values are achieved for most of the datasets, and FFs are generally well constrained within the momentum fraction region . The extracted fragmentation functions, together with the FFs constructed from FFs via isospin symmetry, are used to test isospin symmetry in kaon fragmentation. Although a definitive conclusion cannot be reached yet, these studies have identified several potential measurements that can be performed at existing facilities, which may ultimately help us to arrive at a conclusive answer. With the comprehensive species of FFs extracted within the NPC framework, we are able to perform a test on the momentum sum rule with the light-flavor charged and neutral hadrons.

    hep-phhep-exnucl-exnucl-thPRD(2025)·19 citations
  11. 11*

    A anomaly motivated boson at the energy and precision frontiers

    Ben Allanach🇬🇧 · Christoph Englert🇬🇧 · Wrishik Naskar🇬🇧

    TeV-scale bosons with family-dependent couplings can explain some anomalies inferred from meson measurements of processes involving the transition. A originating from kinetically-mixed spontaneously broken gauge symmetry has been shown to greatly ameliorate global fits~\cite{Allanach:2024ozu} in a `flavour-preferred' region of parameter space. We provide an exploration of this region at the high luminosity (HL-)LHC with particular attention to which signals could be verified across different discovery modes. Even if the HL-LHC does not discover the boson in a resonant di-lepton channel, a FCC-ee -pole run would detect oblique corrections to the electroweak precision observables (EWPOs). Changes due to -induced non-oblique corrections are unlikely to be detected, to within experimental precision. In any case, the extended discovery potential offered by a 100 TeV collider would afford sensitivity to the entire flavour-preferred region and enable a fine-grained and forensic analysis of the~model.

    hep-phhep-exPLB(2025)·2 citations
  12. 12*

    Beautiful Majorana Higgses at Colliders

    Benjamin Fuks🇫🇷 · Jonathan Kriewald🇸🇮 · Miha Nemevšek🇸🇮 · Fabrizio Nesti🇮🇹

    We investigate a novel collider signature within the minimal Left-Right Symmetric Model, featuring a Higgs sector composed of a bi-doublet and two triplets. Our study focuses on a region of the parameter space where the charged gauge boson lies in the multi-TeV regime (3-100 TeV) and the additional Higgs states play a significant role. In this scenario, a heavy neutral Higgs boson with a dominant triplet component can be produced in association with either a Standard Model Higgs boson or a massive weak boson. The subsequent decay of the heavy Higgs into Majorana neutrinos results in displaced lepton signatures, providing a striking manifestation of lepton number violation. Additionally, we explore how the production of -jets in these processes can enhance hadron-collider sensitivity to such signals. A particularly compelling channel, , offers the exciting possibility of simultaneously probing the spontaneous mass origin of both Dirac fermions and Majorana states. Based on an optimised event selection strategy and state-of-the-art Monte Carlo simulations, we outline the expected reach at the HL-LHC and future colliders. Our findings demonstrate that this channel probes a region of parameter space where the neutral Higgs triplet and heavy neutrino masses are relatively light ( GeV, GeV), indirectly constraining the boson to the deep multi-TeV domain, with sensitivity extending up to 70-80 TeV, effectively turning the LHC into a precision machine.

    hep-phhep-exJHEP(2025)·6 citations
  13. 13*

    Color structure of deuteron on the light front

    Satvir Kaur🇨🇳 · Jiatong Wu🇨🇳 · Siqi Xu🇨🇳 · Chandan Mondal🇨🇳 · Xingbo Zhao🇨🇳 · James P. Vary🇺🇸

    We investigate the color structure of the deuteron by solving the light-front QCD Hamiltonian for its six-quark and six-quark-one-gluon components using basis light-front quantization. In this framework, the deuteron wavefunction consists of a singlet-singlet color state as well as additional hidden color states arising from non-trivial color rearrangements. Our analysis shows that while the singlet-singlet state is present, the hidden color states collectively dominate, contributing a larger probability to the deuteron wavefunction. These findings provide new insights into the role of hidden color components in the QCD description of nuclear structure.

    hep-phPoS(2025)·2 citations
  14. 14*

    Basis light-front quantization: Advancing a first principles approach for the nucleon

    Chandan Mondal🇨🇳 · Siqi Xu🇨🇳 · Yiping Liu🇨🇳 · Jiangshan Lan🇨🇳 · Yang Li🇨🇳 · Xingbo Zhao🇨🇳 · James P. Vary🇺🇸

    We present our recent progress in applying the basis light-front quantization approach to investigate the nucleon's structure. We solve its wave functions from the eigenstates of the light-front QCD Hamiltonian using a fully relativistic, nonperturbative approach without an explicit confining potential. These eigenstates are determined for the three-quark, three-quark-gluon, and three-quark-quark-antiquark Fock representations, making them suitable for low-resolution probes. From these wave functions, we compute the nucleon's quark and gluon matter densities, as well as its helicity and transversity distributions, showing qualitative consistency with experimental data. We also determine the quark and gluon helicity contributions to the proton spin and the tensor charges. The resulting light-front wave functions represent a significant step toward a unified description of hadron distribution functions in both longitudinal and transverse momentum space.

    hep-phPoS(2025)·1 citation
  15. 15*

    Extending the symmetries of the generalized CP-symmetric 2HDM scalar potential to the Yukawa sector

    Sergio Carrolo🇩🇪 · Howard E. Haber🇺🇸 · Luis Lourenco🇩🇪 · João P. Silva🇵🇹

    There are only six independent types of symmetry-constrained (renormalizable) scalar potentials in the two Higgs doublet model (2HDM). For example, the scalar sector symmetry known as , generated by the simultaneous application of two independent symmetries acting on the scalar fields, and the generalized CP symmetry known as GCP2 yield equivalent 2HDM scalar potentials. A similar situation arises for the scalar sector symmetries known as U(1) and GCP3, respectively. In this paper, we show that this "degeneracy" remains when the definitions of the corresponding symmetries are extended to the Yukawa sector with three quark generations. The proof involves the exploration of all possible extensions of the corresponding symmetries to the Yukawa sector, consistent with the phenomenological constraints of nonzero quark masses and a nontrivial quark mixing matrix. Moreover, we find that this result is a peculiarity of a Yukawa sector with three quark generations. In particular, with two quark generations, we find that models based on the extension of to the Yukawa sector are inequivalent with those based on GCP2.

    hep-phPRD(2025)·0 citations
  16. 16*

    Exploring the flavor structure of leptons via diffusion models

    Satsuki Nishimura🇯🇵 · Hajime Otsuka🇯🇵 · Haruki Uchiyama🇯🇵

    We propose a method to explore the flavor structure of leptons using diffusion models, which are known as one of generative artificial intelligence (generative AI). We consider a simple extension of the Standard Model with the type I seesaw mechanism and train a neural network to generate the neutrino mass matrix. By utilizing transfer learning, the diffusion model generates 104 solutions that are consistent with the neutrino mass squared differences and the leptonic mixing angles. The distributions of the CP phases and the sums of neutrino masses, which are not included in the conditional labels but are calculated from the solutions, exhibit non-trivial tendencies. In addition, the effective mass in neutrinoless double beta decay is concentrated near the boundaries of the existing confidence intervals, allowing us to verify the obtained solutions through future experiments. An inverse approach using the diffusion model is expected to facilitate the experimental verification of flavor models from a perspective distinct from conventional analytical methods.

    hep-phcs.LGhep-thPRD(2026)·4 citations
  17. 17*

    Natural Top Quark Condensation (a Redux)

    Christopher T. Hill🇺🇸

    The Nambu--Jona-Lasinio (NJL) model involves a pointlike 4-fermion interaction. While it gives a useful description of chiral dynamics (mainly in QCD), it nonetheless omits the crucially important internal wave-function of a two-body bound state, . This becomes significant near critical coupling where extends to large distance, leading to dilution and suppression of induced couplings , such as the Yukawa and quartic couplings, as well as reduced fine-tuning of a hierarchy. In top quark condensation, where the BEH boson is a bound state and we have a UV completion such as topcolor, we must go beyond the NJL model and include effects of . We provide a formulation of this for the Brout-Englert-Higgs boson, and find that it leads to an extended , a significantly reduced and natural composite scale of TeV, a successful prediction for the quartic coupling, , and fine tuning that is reduced to a few percent, providing a compelling candidate solution to the naturalness problem of the BEH boson. The theory is testable and new physics should begin to emerge on the multi-TeV mass scales and possibly accessible to the LHC.

    hep-phhep-exhep-thNPB(2025)·5 citations
  18. 18*

    The impact of future - and -meson measurements with the SMOG2 program at LHCb on the determination of nuclear parton distribution functions

    Carlo Flore🇮🇹 · Cynthia Hadjidakis🇫🇷 · Daniel Kikoła🇵🇱 · Aleksander Kusina🇵🇱 · Anton Safronov🇵🇱

    We perform an analysis of the potential impact of future - and -meson measurement within the SMOG2 fixed-target program at the LHCb experiment on nuclear parton distribution functions. Following~\cite{Bursche:2018orf}, we assume that SMOG2 will collect data for five nuclear targets: He, Ne, Ar, Kr, Xe and hydrogen which will provide a baseline for constructing nuclear ratios. The analysis is performed by using the PDF reweighting method. We demonstrate that such a measurement will allow to considerably reduce the current uncertainties of the nuclear gluon distribution and, to some extent, even the uncertainties of the light sea-quark distributions. Furthermore, it will provide the first possibility to systematically study the current assumptions on the -dependence of the nuclear parton distributions.

    hep-phhep-exhep-thnucl-ex+1PLB(2025)·2 citations
  19. 19*

    20 Years of Light Pentaquark Searches

    Moskov Amaryan🇺🇸

    In this paper, I pay tribute to my exceptional colleagues and friends Dmitri Diakonov, Victor Petrov, and Maxim Polyakov by examining the experimental progress and current status of the searches of the pentaquark from its inception to the present.

    hep-phActa Phys.Polon.B(2025)·2 citations
  20. 20*

    Internal structure of and by using compositeness

    Tomona Kinugawa🇯🇵 · Tetsuo Hyodo🇯🇵

    The internal structure of the near-threshold exotic hadrons, and , are studied by respecting the decay and coupled-channel contributions. The effective field theory model is introduced to calculate the compositeness, the probability of finding the hadronic molecular component. Applying the new interpretation scheme for the complex compositeness of unstable states and using the bare energies of the compact component estimated by the constituent quark model, we find that approximately 50 % of the wavefunction is occupied by the molecular component. This indicates that the structure of is primarily dominated by the component, having the nearest threshold. However, other components, such as the isospin partner channels, also provide non-negligible contributions. On the other hand, about 90 % of is composed of the molecular component. This is because the non-composite bare state and the charged threshold are located relatively far from the and contribute very little to its internal structure.

    hep-phnucl-thPoS(2025)·1 citation
  21. 21*

    Transitioning to Memory Burden: Detectable Small Primordial Black Holes as Dark Matter

    Gia Dvali🇩🇪 · Michael Zantedeschi🇮🇹 · Sebastian Zell🇩🇪

    Mounting theoretical evidence suggests that black holes are subjected to the memory burden effect, implying that after certain time the information stored in them suppresses the decay rate. This effect opens up a new window for small primordial black holes (PBHs) below as dark matter. We show that the smooth transition from semi-classical evaporation to the memory-burdened phase strongly impacts observational bounds on the abundance of small PBHs. The most stringent constraints come from present-day fluxes of astrophysical particles. Remarkably, currently-transitioning small PBHs are detectable through high-energetic neutrino events.

    hep-phastro-ph.COastro-ph.HEgr-qc+152 citations
  22. 22*

    Effects of dissipation on phase diagram and bosonic excitations in the quark-meson model

    Johannes V. Roth🇩🇪 · Yunxin Ye🇩🇪 · Sören Schlichting🇩🇪 · Lorenz von Smekal🇩🇪

    In this work we study the quark-meson model within a real-time formulation of the functional renormalization group (FRG) on the Schwinger-Keldysh contour. First, we discuss in detail the symmetry of thermal equilibrium for the fermionic sector of the Keldysh action. We take into account dissipation for the bosonic degrees of freedom in the spirit of the Caldeira-Leggett model by coupling the system to an invariant external heat bath. We study the effect of dissipation on static equilibrium properties, most prominently on the FRG flow of the effective potential and thus on the resulting phase diagram. We find that, unlike in classical systems, through the contributions from non-zero Matsubara modes the dissipative dynamics can in general have an effect on static observables. We investigate these effects within two phenomenological models for the temperature dependence of the pion damping to verify that they are quantitatively small. To estimate their largest possible influence, we consider limits where the damping constants approach infinity.

    hep-phPRD(2026)·3 citations
  23. 23*

    Positivity at 1-Loop: Bounds on Photon and Gluon EFTs

    Jay Desai🇮🇳 · Diptimoy Ghosh🇮🇳

    In this paper, we attempt to derive ``positivity" bounds on Photon and Gluon Effective Field Theories (EFTs) at one loop level. While for the Photon case, the one loop amplitude is IR finite and well defined in the forward limit, earlier studies failed to obtain a dispersive bound on dimension-12 operators due to the dependence of the ``arc integral" on the artificial low-energy scale. We show that this awkward dependence can be taken care of by analysing the ultra-violet (UV) side of dispersion relation closely. In particular, we derive an IR safe and RG improved bound at 1-loop. Thereafter, we perform a similar analysis on the Gluon EFT, which has additional complications due to ill-defined forward limit and IR divergences at 1-loop. We show that even in this case, one can get a meaningful bound at 1-loop.

    hep-phhep-thJHEP(2025)·6 citations
  24. 24*

    Small radius inclusive jet production at the LHC through NNLO+NNLL

    Terry Generet🇬🇧 · Kyle Lee🇺🇸 · Ian Moult🇺🇸 · Rene Poncelet🇵🇱 · Xiaoyuan Zhang🇺🇸

    The study of hadronic jets and their substructure at hadronic colliders is crucial for improving our understanding of QCD, and searching for new physics. As such, there has been a significant effort to improve their theoretical description. In the small radius limit, inclusive jet production exhibits a universal factorization, enabling the resummation of logarithms which greatly stabilizes theoretical predictions. In this paper, we show how to combine a recently introduced framework for small- resummation with the STRIPPER subtraction formalism for fragmentation, enabling next-to-next-to-leading order calculations of small- inclusive jet production for a wide variety of processes at the LHC. We extract the two-loop constants for the jet functions, enabling for the first time next-to-next-to-leading logarithmic resummation matched to next-to-next-to-leading order perturbative calculation. We compare with CMS data for small- jet production, and find that our results greatly improve the accuracy of the predictions at small-, and stabilize the perturbative convergence and error estimates at larger . Our approach is applicable to a wide class of jet substructure observables exhibiting similar factorization theorems, opening the door to an NNLO jet substructure program at the LHC.

    hep-phhep-exnucl-thJHEP(2025)·12 citations
  25. 25*

    Visualizing How Jet Structure Shapes Jet Wakes

    Arjun Srinivasan Kudinoor🇺🇸 · Daniel Pablos🇪🇸 · Krishna Rajagopal🇺🇸

    The ATLAS Collaboration has developed a method to analyze large-radius jets composed of skinny subjets in heavy-ion collisions. We first demonstrate that the measurements pioneered by ATLAS constrain the value of , the resolution length of QGP -- and rule out any picture in which an entire parton shower loses energy coherently as a single entity. We then analyze the response of the medium to the passage of large-radius jets containing two skinny subjets in gamma-jet events. We introduce novel jet-shape observables that allow us to visualize how the internal structure of large-radius jets shapes the wakes they excite in the QGP. We find that even when the subjets are radians apart, the angular shape of the soft hadrons originating from their wake forms a single broad structure. Only when the two subjets are even farther apart are two sub-wakes revealed. We show that the way in which jet structure shapes the structure of jet-induced wakes can be visualized with similar clarity in experiments by using only low- hadrons. The observables we introduce offer a new and distinctive way of seeing jet-induced wakes -- and wake substructure -- in heavy-ion collision data.

    hep-phnucl-exnucl-thEPJ Web Conf.(2025)·1 citation
  26. 26*

    Proposal for a shared transverse LLP detector for FCC-ee and FCC-hh and a forward LLP detector for FCC-hh

    Biplob Bhattacherjee🇮🇳 · Camellia Bose🇮🇳 · Herbi K. Dreiner🇩🇪 · Nivedita Ghosh🇯🇵 · Shigeki Matsumoto🇯🇵 · Swagata Mukherjee🇮🇳 · Rhitaja Sengupta🇩🇪 · Anand Sharma🇮🇳

    As the particle physics community has explored most of the conventional avenues for new physics, the more elusive areas are becoming increasingly appealing. One such potential region, where new physics might be hiding, involves light and weakly interacting long-lived particles (LLPs). To probe deeper into this region, where the possibility of highly displaced scenarios weakens the role of general-purpose collider detectors, dedicated LLP detectors are our best option. However, their potential can only be fully realized if we optimize their position and dimensions to suit our physics goals. This is possible at the upcoming Future Circular Collider (FCC) facility, where the feasibility and design studies are still ongoing and can accommodate new proposals focused specifically on LLP searches. We propose optimized dedicated detectors in both the transverse and forward directions, DELIGHT and FOREHUNT, significantly enhancing the sensitivity to previously uncharted regions of the new physics parameter space. Our proposed DELIGHT detector can additionally serve as a shared transverse detector during both the FCC-ee and FCC-hh runs. The concept of a shared transverse detector is novel and sustainable, utilizing the same interaction points of the lepton and hadron colliders at the FCC. This minimizes costs and boosts the LLP physics case at the FCC.

    hep-phhep-exNPB(2026)·3 citations
  27. 27*

    Neutrino Theory in the Precision Era

    Asmaa Abada🇫🇷 · Gabriela Barenboim🇪🇸 · Toni Bertólez-Martínez🇪🇸 · Sandipan Bhattacherjee🇮🇳 · Sara Bolognesi🇫🇷 · Patrick D. Bolton🇸🇮 · Nilay Bostan🇺🇸 · Gustavo C. Branco🇵🇹 · Sabya Sachi Chatterjee🇩🇪 · Adriano Cherchiglia🇧🇷 · Marco Chianese🇮🇹 · B. A. Couto e Silva🇧🇷 and 67 other authors

    This document summarises discussions on future directions in theoretical neutrino physics, which are the outcome of a neutrino theory workshop held at CERN in February 2025. The starting point is the realisation that neutrino physics offers unique opportunities to address some of the most fundamental questions in physics. This motivates a vigorous experimental programme which the theory community fully supports. \textbf{A strong effort in theoretical neutrino physics is paramount to optimally take advantage of upcoming neutrino experiments and to explore the synergies with other areas of particle, astroparticle, and nuclear physics, as well as cosmology.} Progress on the theory side has the potential to significantly boost the physics reach of experiments, as well as go well beyond their original scope. Strong collaboration between theory and experiment is essential in the precision era. To foster such collaboration, \textbf{we propose to establish a CERN Neutrino Physics Centre.} Taking inspiration from the highly successful LHC Physics Center at Fermilab, the CERN Neutrino Physics Centre would be the European hub of the neutrino community, covering experimental and theoretical activities.

    hep-phastro-ph.COastro-ph.HEhep-ex+13 citations
  28. 28*

    Conceptual Design Report for the MATHUSLA Long-Lived Particle Detector near CMS

    Branden Aitken🇨🇦 · Cristiano Alpigiani🇺🇸 · Juan Carlos Arteaga-Velázquez🇲🇽 · Mitchel Baker🇨🇦 · Kincso Balazs🇨🇭 · Jared Barron🇺🇸 · Brian Batell🇺🇸 · Austin Batz🇺🇸 · Yan Benhammou🇮🇱 · Tamara Alice Bud🇨🇭 · Karen Salomé Caballero-Mora🇲🇽 · John Paul Chou🇺🇸 and 61 other authors

    We present the Conceptual Design Report (CDR) for the MATHUSLA (MAssive Timing Hodoscope for Ultra-Stable neutraL pArticles) long-lived particle detector at the HL-LHC, covering the design, fabrication and installation at CERN Point 5. MATHUSLA is a 40 m-scale detector with an air-filled decay volume that is instrumented with scintillator tracking detectors, to be located near CMS. Its large size, close proximity to the CMS interaction point and about 100 m of rock shielding from HL-LHC backgrounds allows it to detect LLP production rates and lifetimes that are one to two orders of magnitude beyond the ultimate sensitivity of the HL-LHC main detectors for many highly motivated LLP signals. Data taking is projected to commence with the start of HL-LHC operations. We present a new 40m design for the detector: its individual scintillator bars and wavelength-shifting fibers, their organization into tracking layers, tracking modules, tower modules and the veto detector; define a high-level design for the supporting electronics, DAQ and trigger system, including supplying a hardware trigger signal to CMS to record the LLP production event; outline computing systems, civil engineering and safety considerations; and present preliminary cost estimates and timelines for the project. We also conduct detailed simulation studies of the important cosmic ray and HL-LHC muon backgrounds, implementing full track/vertex reconstruction and background rejection, to ultimately demonstrate high signal efficiency and background event in realistic LLP searches for the main physics targets at MATHUSLA. This sensitivity is robust with respect to detector design or background simulation details. Appendices provide various supplemental information.

    physics.ins-dethep-exhep-ph18 citations
  29. 29*

    Can a Breakdown of Hawking Evaporation Open a New Mass Window for Primordial Black Holes as Dark Matter?

    Gabriele Montefalcone🇺🇸 · Dan Hooper🇺🇸 · Katherine Freese🇺🇸 · Chris Kelso🇺🇸 · Florian Kuhnel🇩🇪 · Pearl Sandick🇺🇸

    Semi-classical Hawking evaporation is expected to break down at some point in a black hole's evolution as the effects of quantum gravity become important. In particular, it has been argued that the so-called memory-burden effect could cause black holes to become stabilized by the information that they carry, thereby suppressing the rate at which they undergo Hawking evaporation. It has furthermore been suggested that this opens a new mass window, between , over which primordial black holes could constitute the dark matter of our Universe. We show for the first time that this is true only if the transition from the semi-classical phase of a black hole to its memory-burdened phase is practically instantaneous. If this transition is instead more continuous, Hawking evaporation will persist at relevant levels throughout the eras of Big Bang Nucleosynthesis and recombination, leading to stringent constraints which rule out the possibility that black holes lighter than could make up all or most of the dark matter. More broadly, our analysis demonstrates that even if departures from the semi-classical Hawking evaporation occur as proposed, they must be both drastic and abrupt to open viable new mass windows for primordial black hole dark matter.

    astro-ph.COastro-ph.HEgr-qchep-phPRD(2026)·39 citations
  30. 30*

    Evidence for Cosmological Massive Neutrinos

    Deng Wang🇪🇸

    A key question in cosmology is whether massive neutrinos exist on cosmic scales. Current cosmological observations have severely compressed the viable range for neutrino masses and even prefer phenomenologically an effective negative mass. This poses a great challenge to the cosmological search for neutrinos. Based on current background and large scale structure data, taking a full redshift and/or scale tomography method, we find one beyond , two and two evidences of massive neutrinos, spanning both high and low redshifts, as well as both small and intermediate scales. Interestingly, these five neutrino masses are well consistent within confidence level, indicating a possible suppression of neutrino mass during the evolution of the universe. Using cosmic microwave background observations to constrain a redshift and scale dependent neutrino mass, we make the first neutrino mass map through the cosmic history and full scales for future high precision search.

    astro-ph.COastro-ph.HEgr-qchep-ex+10 citations
  31. 31*

    MPD physics performance studies in Bi+Bi collisions at GeV

    MPD Collaboration

    The Multi-Purpose Detector (MPD) is one of the three experiments of the Nuclotron Ion Collider-fAcility (NICA) complex, which is currently under construction at the Joint Institute for Nuclear Research in Dubna. With collisions of heavy ions in the collider mode, the MPD will cover the energy range 4-11 GeV to scan the high baryon-density region of the QCD phase diagram. With expected statistics of 50-100 million events collected during the first run, MPD will be able to study a number of observables, including measurements of light hadrons and hypernuclei production, particle flow, correlations and fluctuations, have a first look at dielectron production, and modification of vector-meson properties in dense matter. In this paper, we present selected results of the physics feasibility studies for the MPD experiment in Bismuth-Bismuth collisions at an energy of 9.2 GeV, the system considered as one of the first available at the NICA collider.

    nucl-exhep-phnucl-thRev.Mex.Fis.(2025)·25 citations
  32. 32*

    Heavy Neutron Star Phenomenology with an H-dibaryon

    Jesper Leong🇦🇺 · Anthony W. Thomas🇦🇺 · Pierre A. M. Guichon🇦🇺

    The equation of state for dense nuclear matter in -equilibrium is explored including the possibility of a doubly-strange H-particle. Consistent with experimental constraints, the mass of the H in free space is taken to be near the threshold. Within the quark-meson coupling model, which we use, no new parameters are required to describe the interaction between the H-dibaryon and the other baryons. The maximum mass is only slightly reduced, and the tidal deformability is essentially unchanged with this addition. In heavy neutron stars the H is abundant and extends as far as 6 km from the center of the core.

    nucl-thastro-ph.HEhep-phPRC(2026)·2 citations
  33. 33*

    Are Neutron Stars Rich in H-dibaryons?

    Jesper Leong🇦🇺 · Anthony W. Thomas🇦🇺 · Pierre A. M. Guichon🇦🇺

    The possible existence of an H-dibaryon near the threshold has still not been decided experimentally. This raises the question of the potential effects on neutron stars if it does exist. We explore the consequences within the quark-meson coupling model, using the excluded volume formalism. While the H is abundant in heavy stars the maximum mass is only lowered slightly by its presence.

    nucl-thastro-ph.HEhep-phPoS(2025)·1 citation
  34. 34*

    AliCPT Sensitivity to Cosmic Reheating

    Yang Liu🇨🇳 · Lei Ming🇨🇳 · Marco Drewes🇧🇪 · Hong Li🇨🇳

    We present the first assessment of the Ali Cosmic Microwave Background Polarization Telescope's (AliCPT) sensitivity to the reheating epoch after cosmic inflation, based on its ability to detect primordial gravitational waves. We consider three models of inflation, an -attractor T-model, RGI inflation and QCD-driven warm inflation. Assuming a fiducial value of , we find that AliCPT-1, in its fully loaded focal plane detector configuration and combined with Planck, can provide measurements of the order of magnitude of the reheating temperature with an accuracy around . For QCD-driven warm inflation this can be translated into a constraint on the inflaton coupling to gluons, which can be probed independently in axion search experiments. Our results constitute the first demonstration of AliCPT's ability to probe the initial temperature of the hot big bang and the microphysical parameter connecting cosmic inflation and particle physics.

    astro-ph.COhep-phPRD(2026)·5 citations
  35. 35*

    Lower bound on the orbital period of Kerr-Newman black holes

    Yan Peng🇨🇳

    Based on the orbital period of Kerr black holes, Hod proposed a conjecture that a general lower bound on the orbital period may exist. In this work, we examined this bound by exploring the orbital period of Kerr-Newman black holes using analytical and numerical methods. By choosing different charge and spin of Kerr-Newman black holes, we found a lower bound for the orbital period of Kerr-Newman black holes as , where is the orbital radius, is the orbital period observed from infinity and is the black hole mass. This bound is just the same as Hod's conjectured lower bound. So our results further demonstrated that Hod's lower bound may be a general property in black hole spacetimes.

    gr-qchep-phhep-th4 citations
  36. 36*

    Long-Baseline Atom Interferometry

    Antun Balaz🇷🇸 · Diego Blas🇪🇸 · Oliver Buchmueller🇬🇧 · Sergio Calatroni🇨🇭 · Laurentiu-Ioan Caramete🇷🇴 · David Cerdeno🇪🇸 · Maria Luisa Chiofalo🇮🇹 · Fabio Di Pumpo🇩🇪 · Goran Djordjevic🇷🇸 · John Ellis🇬🇧 · Pierre Fayet🇫🇷 · Chris Foot🇬🇧 and 41 other authors

    Long-baseline atom interferometry is a promising technique for probing various aspects of fundamental physics, astrophysics and cosmology, including searches for ultralight dark matter (ULDM) and for gravitational waves (GWs) in the frequency range around 1~Hz that is not covered by present and planned detectors using laser interferometry. The MAGIS detector is under construction at Fermilab, as is the MIGA detector in France. The PX46 access shaft to the LHC has been identified as a very suitable site for an atom interferometer of height m, sites at the Boulby mine in the UK and the Canfranc Laboratory are also under investigation, and possible sites for km-class detectors have been suggested. The Terrestrial Very-Long-Baseline Atom Interferometry (TVLBAI) Proto-Collaboration proposes a coordinated programme of interferometers of increasing baselines.

    hep-exastro-ph.IMgr-qchep-ph+19 citations
  37. 37*

    Effects of superradiance on relativistic Foldy-Wouthuysen densities

    F. Daem🇫🇷 · A. Matzkin🇫🇷

    Recent interest in the studies of structured states obtained in relativistic electron beams has highlighted the use of two alternative descriptions, each based on a different wavefunction and the related space-time density. Although both wavefunctions obey the Dirac equation (one directly and the other through a Foldy-Wouthuysen transformation) they lead to different dynamics and properties, such as the presence or absence of spin-orbit interactions. In this work we investigate wavepacket dynamics for the Klein-Gordon equation, which displays the same ambiguity regarding the choice of different densities, in a setting involving Klein tunneling across a series of supercritical potential barriers. Relying on the superradiant character of this setting, we obtain solutions to the wavepacket dynamics indicating that the density based on a Foldy-Wouthuysen transformation of the wavefunction can be locally amplified outside the light-cone. In principle, the exponential increase of the charge due to the field inhomogeneities can lead to an arbitrarily large amplification over macroscopic distances. These results question the interpretation of the Foldy-Wouthuysen density as a fundamentally correct probability or charge density.

    quant-phhep-phhep-thPRA(2025)·3 citations
  38. 38*

    nuSCOPE: A short-baseline neutrino beam at CERN for high-precision cross-section measurements

    F. Acerbi🇮🇹 · C. Andreopoulos🇬🇧 · I. Angelis🇬🇷 · A. Baratto Roldan🇨🇭 · L. Bomben🇮🇹 · M. Bonesini🇮🇹 · F. Bramati🇮🇹 · A. Branca🇮🇹 · C. Brizzolari🇮🇹 · G. Brunetti🇮🇹 · M. Buizza Avanzini🇫🇷 · S. Capelli🇮🇹 and 72 other authors

    A new generation of neutrino cross-section experiments at the GeV scale is crucial in the precision era of oscillation physics and lepton flavor studies. In this document, we present a novel neutrino beam design that leverages the experience and R&D achievements of the NP06/ENUBET and NuTag Collaborations and explore its potential implementation at CERN. This beam enables flux monitoring at the percent level and provides a neutrino energy measurement independent of final state particle reconstruction at the neutrino detector. As a result, it eliminates the two primary sources of systematic uncertainty in cross-section measurements: flux normalization and energy bias caused by nuclear effects. We provide a detailed description of the beam technology and instrumentation, along with an overview of its physics potential, with particular emphasis on cross-sections relevant to DUNE and Hyper-Kamiokande.

    hep-exhep-phphysics.acc-phphysics.ins-det18 citations
  39. 39*

    Quintessential Inflation in Palatini gravity

    Konstantinos Dimopoulos🇬🇧 · Christian Dioguardi🇪🇪 · Gert Hütsi🇪🇪 · Antonio Racioppi🇪🇪

    Palatini gravity, with the inflaton kinetic term, proved to be a powerful framework for generating asymptotically flat inflaton potentials. Here we show that a quadratic Palatini restores compatibility with the observational data of the Peebles-Vilenkin quintessential inflation model. Moreover, the same can be achieved with an exponential version of the Peebles-Vilenkin potential if embedded in a Palatini of order higher than two.

    gr-qcastro-ph.COhep-phEur.Phys.J.Plus(2025)·12 citations
  40. 40*

    On Measuring Stimulated Photon-photon Scattering using Multiple Ultraintense Lasers

    Hans G. Rinderknecht🇺🇸 · E. Dill🇺🇸 · A. J. MacLeod🇨🇿 · B. King🇬🇧 · K. Sow🇺🇸 · S.-W. Bahk🇺🇸 · I. A. Begishev🇺🇸 · F. Karbstein🇩🇪 · J. Schreiber🇩🇪 · M. Zepf🇩🇪 · A. Di Piazza🇺🇸

    Stimulated photon-photon scattering is a predicted consequence of quantum electrodynamics that has yet to be measured directly. Measuring the cross-section for stimulated photon-photon scattering is the aim of a flagship experiment for NSF OPAL, a proposed laser user facility with two, 25-PW beamlines. We present optimized experimental designs for achieving this challenging and canonical measurement. A family of experimental geometries is identified that satisfies the momentum- and energy-matching conditions for two selected laser frequency options. Numerical models predict a maximum signal exceeding 1000 scattered photons per shot at the experimental conditions envisaged at NSF OPAL. Experimental requirements on collision geometry, polarization, cotiming and copointing, background suppression, and diagnostic technologies are investigated numerically. These results confirm that a beam cotiming shorter than the pulse duration and control of the copointing on a scale smaller than the shortest laser wavelength are needed to robustly scatter photons on a per-shot basis. Finally, we assess the bounds that a successful execution of this experiment may place on the mass scale of Born-Infeld nonlinear electrodynamics beyond the Standard Model of physics.

    hep-exhep-phPhys.Plasmas(2025)·13 citations
  41. 41*

    CLIC Higgs coupling prospects with 100 Hz operation

    A. Robson🇬🇧 · P. Roloff🇨🇭 · J. de Blas🇪🇸

    The staging scenario for CLIC has been updated following new studies of the beam emittance through the accelerator chain, which has resulted in higher expected luminosities, and a change in baseline to a 100 Hz repetition rate at the initial energy stage. Here, the Higgs coupling sensitivities are updated for the new staging plan.

    hep-exhep-ph3 citations
  42. 42*

    Wave Interference in Self-Interacting Fuzzy Dark Matter

    Christian Capanelli🇨🇦 · Wayne Hu🇺🇸 · Evan McDonough🇨🇦

    In the Fuzzy Dark Matter (FDM) scenario, the dark matter is composed of an ultra-light scalar field with coherence length and wave interference on astrophysical scales. Scalar fields generically have quartic self-interactions that modify their dispersion relation and the associated evolution of density perturbations. We perform the first dedicated analysis of the role of wave interference on this evolution due to self-interactions in FDM and vice versa, developing a perturbative treatment applicable at early times and then comparing against a suite of fully nonlinear benchmark simulations, varying the dark matter density, interaction strength, and fiducial momentum scale. We explicitly simulate the limit where this momentum scale is relatively high compared with the scale of the simulation volume, applicable to cases where the dark matter is initially ``warm" due to causal constraints on a post-inflationary production or in virialized halos and other ``thermalized" cases with initially cold production. We find that in such scenarios, density perturbations are unable to grow on the expected self interaction time scale because of interference effects, instead saturating on the much shorter de Broglie crossing time, with a dependence on the sign of the interaction. Finally, we comment on the implications of our results for astrophysical systems such as high-density ultra-faint dwarf galaxies where wave interference plays an important role.

    astro-ph.COgr-qchep-phhep-thPRD(2025)·10 citations
  43. 43*

    Conformal Collider Physics at Large Charge

    Gabriel Cuomo🇺🇸 · Eren Firat🇨🇭 · Filippo Nardi🇨🇭 · Lorenzo Ricci🇺🇸

    We study energy correlators and other event shapes in states created by operators with large global charge in Conformal Field Theories. Focusing on theories whose large charge sector is described by the superfluid Effective Field Theory (EFT), we develop a systematic framework to compute event shapes within the EFT. As formerly observed, event shapes at leading order in factorize into a product of classical expectation values determined by symmetry. In contrast, the subleading contribution to energy-energy and charge-charge correlators is a nontrivial prediction of the EFT, which we compute explicitly. Our results reveal a sharp collinear enhancement of the correlation between detectors, induced by the propagation of sound. We also generalize our findings to a broad class of event shapes.

    hep-thhep-phJHEP(2026)·15 citations
  44. 44*

    Generalizing the Bogoliubov vs Boltzmann approaches in gravitational production

    Ayan Chakraborty🇮🇳 · Simon Clery🇫🇷 · Md Riajul Haque🇮🇳 · Debaprasad Maity🇮🇳 · Yann Mambrini🇫🇷

    We investigate the spectral behavior of scalar fluctuations generated by gravity during inflation and the subsequent reheating phase. We consider a non-perturbative Bogoliubov treatment within the context of pure gravitational reheating. We compute both long and short-wavelength spectra, first for a massless scalar field, revealing that the spectral index in part of the infrared (IR) regime varies between and , depending on the post-inflationary equation of state (EoS), . Furthermore, we study the mass-breaking effect of the IR spectrum by including finite mass, , of the daughter scalar field. We show that for , where is the Hubble parameter during inflation, the IR spectrum of scalar fluctuations experiences exponential mass suppression, while for smaller masses, , the spectrum remains flat in the IR regime regardless of the post-inflationary EoS. For any general EoS, we also compute a specific IR scale, , of fluctuations below which the IR spectrum will suffer from this finite mass effect. In the UV regime, oscillations of the inflaton background lead to interference terms that explain the high-frequency oscillations in the spectrum. Interestingly, we find that for any EoS, , the spectral behavior turns out to be independent of the EoS, with a spectral index . We have compared this Bogoliubov treatment for the UV regime to perturbative computations with solutions to the Boltzmann equation and found an agreement between the two approaches for any EoS, . We also explore the relationship between the gravitational reheating temperature and the reheating EoS employing the non-perturbative analytic approach, finding that reheating can occur for .

    gr-qcastro-ph.COhep-phhep-thPRD(2025)·8 citations
  45. 45*

    Singularities in Cosmological Loop Correlators

    Supritha Bhowmick🇮🇳 · Mang Hei Gordon Lee🇹🇼 · Diptimoy Ghosh🇮🇳 · Farman Ullah🇮🇳

    In this work we perform a systematic study of the singularity structure of inflationary correlations at 1-loop. We explicitly compute a few diagrams and find a pattern emerging in the singularities produced. Motivated by this, we derive diagrammatic rules to extract the singularities of any two-site 1-loop diagram. Using these rules, the poles and branch cuts produced can be predicted by simply identifying the energies flowing through certain subgraphs, without having to perform complicated integrals. We demonstrate how these rules follow by analyzing the general structure of the time and momentum integrals of the correlators. An interesting feature of de-Sitter correlators at 1-loop is the presence of an off-shell total energy branch point, which is present in dimensional regularization as well as cutoff regularization. We probe the source of this branch cut in detail, while revisiting the cosmological KLN theorem (arXiv:2308.00680) in this context. Finally, we show that the branch cuts produced in a renormalised correlator always repackage themselves in a dilatation invariant form to produce logarithms of ratios of comoving scales.

    hep-thgr-qchep-phJHEP(2026)·12 citations

* Reconstructed cohort: no mailing for this day survives in the archive. Papers are grouped by their submission times and arXiv's announcement cut-off, assuming announcement without delay; positions follow identifier order. Validated at ~91% exact-day agreement against the archived era.