PaperPanorama

HEP Phenomenology·hep-ph

Wed·Jan 19, 2022

33 papers24 primary·9 cross-listed·reconstructed*

  1. 01*

    The cosmological moduli problem and naturalness

    Kyu Jung Bae🇰🇷 · Howard Baer🇺🇸 · Vernon Barger🇺🇸 · Robert Wiley Deal🇺🇸

    The cosmological moduli problem (CMP) comes in three parts: 1. potential violation of BBN constraints from late decaying moduli fields, 2. the moduli-induced gravitino problem wherein gravitinos are overproduced and 3. the moduli-induced lightest SUSY particle (LSP) overproduction problem. We examine the cosmological moduli problem and its connection to electroweak naturalness. We calculate the various two-body decay widths of a light modulus field into MSSM particles and gravitinos within general supersymmetric models. We include both phase space and mixing effects. We examine cases without and with helicity suppression of modulus decays to gravitinos (cases 1 & 2) and/or gauginos (cases A & B). For case B1, we evaluate regions of gravitino mass m_{3/2} vs. modulus mass m_\phi parameter space constrained by BBN, by overproduction of gravitinos and by overproduction of neutralino dark matter, along with connections to naturalness. For this case, essentially all of parameter space is excluded unless m_\phi >~ 2.5\times 10^3 TeV with m_\phi<2m_{3/2}. For a potentially most propitious case B2 with \phi decay to Higgs and matter turned off, then modulus branching fractions to SUSY and to gravitinos become highly suppressed at large m_\phi. But since the modulus number density increases faster than the branching fractions decrease, there is still gross overproduction of neutralino dark matter. We also show that in this scenario the thermally produced gravitino problem is fixed by huge entropy dilution, but non-thermal gravitino production from moduli decay remains a huge problem unless it is kinematically suppressed with m_\phi < 2m_{3/2}. In a pedagogical appendix, we present detailed calculations of modulus field two-body decay widths.

    hep-phJHEP(2022)·29 citations
  2. 02*

    TRISTAN

    Yu Hamada🇯🇵 · Ryuichiro Kitano🇯🇵 · Ryutaro Matsudo🇯🇵 · Hiromasa Takaura🇯🇵 · Mitsuhiro Yoshida🇯🇵

    The ultra-cold muon technology developed for the muon experiment at J-PARC provides a low emittance beam which can be accelerated and used for realistic collider experiments. We consider the possibility of new collider experiments by accelerating the beam up to 1 TeV. Allowing the beam to collide with a high intensity beam at the TRISTAN energy, GeV, in the storage ring with the same size as TRISTAN (the circumference of 3 km), one can realize a collider experiment with the center-of-mass energy GeV, which allows productions of the Higgs bosons through the vector boson fusion processes. We estimate the deliverable luminosity with existing accelerator technologies to be at the level of cm s, with which the collider can be a good Higgs boson factory. The colliders up to TeV are also possible by using the same storage ring. They have a capability of producing the superpartner of the muon up to TeV masses.

    hep-phhep-exPTEP(2022)·87 citations
  3. 03*

    Family of New Exact Solutions for Longitudinally Expanding Ideal Fluids

    Shuzhe Shi🇨🇦 · Sangyong Jeon🇨🇦 · Charles Gale🇨🇦

    We report on the discovery of new analytical solutions of the equations of relativistic ideal hydrodynamics. In this solution, the fluid expands in the longitudinal direction and contains a plateau structure that extends over a finite range in rapidity and can be either symmetric or asymmetric in that variable. We further calculate the corresponding pseudo-rapidity distribution of hadron yields, and find decent agreement with experimental measurements in high-energy Pb+Pb, Au+Au, p+Pb, and d+Au collisions.

    hep-phnucl-thPRC(2022)·13 citations
  4. 04*

    Isospin eigenstates of the color singlet-singlet type pentaquark states

    Xiu-Wu Wang🇨🇳 · Zhi-Gang Wang🇨🇳 · Guo-Liang Yu🇨🇳 · Qi Xin🇨🇳

    In this article, we construct the color singlet-singlet type five-quark currents with the isospins and unambiguously to explore the , , and pentaquark states via the QCD sum rules for the first time, where the , , represent the color-singlet clusters having the same quantum numbers as the corresponding physical mesons or baryons. The numerical results support assigning the , , and as the , , and pentaquark states with the isospin , respectively. The corresponding , , and pentaquark states with the isospin have slightly larger masses, the observations of the higher pentaquark candidates in the invariant mass spectrum would shed light on the nature of the states, and make contributions in distinguishing the scenarios of color antitriplet-antitriplet-antitriplet type and color singlet-singlet type pentaquark states.

    hep-phSCPMA(2022)·29 citations
  5. 05*

    Taking Neutrino Pictures via Electrons

    Guey-Lin Lin🇹🇼 · Thi Thuy Linh Nguyen🇹🇼 · Martin Spinrath🇹🇼 · Thi Dieu Hien Van🇹🇼 · Tse-Chun Wang🇹🇼

    In this paper we discuss the prospects to take a picture of an extended neutrino source, i.e., resolving its angular neutrino luminosity distribution. This is challenging since neutrino directions cannot be directly measured but only estimated from the directions of charged particles they interact with in the detector material. This leads to an intrinsic blurring effect. We first discuss the problem in general terms and then apply our insights to solar neutrinos scattering elastically with electrons. Despite the aforementioned blurring we show how with high statistics and precision the original neutrino distributions could be reconstructed.

    hep-phastro-ph.HEastro-ph.SRhep-ex+1JCAP(2022)·2 citations
  6. 06*

    Sensitivity of Parity-violating Electron Scattering to a Dark Photon

    A. W. Thomas🇦🇺 · X. G. Wang🇦🇺 · A. G. Williams🇦🇺

    We explore the sensitivity of the parity-violating electron scattering (PVES) asymmetry in both elastic and deep-inelastic scattering to the properties of a dark photon. Given advances in experimental capabilities in recent years, there are interesting regions of parameter space where PVES offers the chance to discover new physics in the near future. There are also cases where the existence of a dark photon could significantly alter our understanding of the structure of atomic nuclei and neutron stars as well as parton distribution functions.

    hep-phhep-exnucl-thPRL(2022)·27 citations
  7. 07*

    Photoproduction in an effective Lagrangian approach

    Neng-Chang Wei🇨🇳 · Ai-Chao Wang🇨🇳 · Fei Huang🇨🇳

    A gauge-invariant model is constructed for the reaction within a tree-level effective Lagrangian approach with the purpose to understand the underlying production mechanisms and to study the resonance contributions in this reaction. In addition to the -channel and exchanges, the -channel nucleon exchange, and the interaction current, the -channel nucleon resonance exchanges are also included in constructing the reaction amplitudes to describe the data. It is found that the contributions from the -channel exchange are required to describe the most recently measured total cross-section data for from the CLAS Collaboration. Further analysis shows that the interaction current dominates the reaction near the threshold as a result of gauge invariance. The -channel exchange contributes significantly, while the contributions from the -channel exchange as well as the -channel nucleon exchange turn out to be negligible. The contributions from the -channel exchange are found to be responsible for the bump structure shown in the CLAS total cross-section data above the center-of-mass energy GeV. The predictions of the differential cross sections for are shown and discussed, which can provide theoretical guidances for the future experiments.

    hep-phCPC(2022)·0 citations
  8. 08*

    Scalar and Fermion Two-component SIMP Dark Matter with an Accidental Symmetry

    Shu-Yu Ho🇰🇷 · Pyungwon Ko🇰🇷 · Chih-Ting Lu🇰🇷

    In this paper, we construct for the first time a two-component strongly interacting massive particles (SIMP) dark matter (DM) model, where a complex scalar and a vector-like fermion play the role of the SIMP DM candidates. These two particles are stable due to an accidental symmetry after the breaking of a gauge symmetry. By introducing one extra complex scalar as a mediator between the SIMP particles, this model can have processes that determine the DM relic density. On the other hand, the SIMP DM particles can maintain kinetic equilibrium with the thermal bath until the DM freeze-out temperature via the gauge couplings. Most importantly, we find an unavoidable two-loop induced process tightly connecting to the process that would redistribute the SIMP DM number densities after the chemical freeze-out of DM. Moreover, this redistribution would significantly modify the predictions of the self-interacting cross section of DM compared with other SIMP models. It is crucial to include the two-loop induced annihilations to obtain the correct DM phenomenology.

    hep-phastro-ph.COJHEP(2022)·35 citations
  9. 09*

    Resonances and in decays

    Ai-Jun Ma🇨🇳 · Wen-Fei Wang🇨🇳

    The contributions for the kaon pair from the intermediate states and in the decays , , and are analyzed within the perturbative QCD factorization approach. The decay amplitudes for all concerned decays in this work are dominated by the factorizable Feynman diagrams with the emission of the kaon pair, and the charged mesons should be of great importance in the channel of the related three-body decays. Moreover, these quasi-two-body decays are CKM-favored, and the relevant branching ratios are predicted to be in the order of , which have the potential to be measured by experiments. It is also shown that the contributions of the subprocesses for the three-body meson decays are considerable according to the total three-body branching fractions presented by Belle. Therefore, the decays , , and can be employed to study the properties of and in the LHCb and Belle-II experiments.

    hep-phCPC(2022)·10 citations
  10. 10*

    Comprehensive study of the light charged Higgs boson in the type-I two-Higgs-doublet model

    Kingman Cheung🇹🇼 · Adil Jueid🇰🇷 · Jinheung Kim🇰🇷 · Soojin Lee🇰🇷 · Chih-Ting Lu🇰🇷 · Jeonghyeon Song🇰🇷

    In the type-I two-Higgs-doublet model, existing theoretical and experimental constraints still permit the light charged Higgs boson with a mass below the top quark mass. We present a complete roadmap for the light charged Higgs boson at the LHC through the comprehensive phenomenology study, focusing on the normal scenario where the lighter \textit{CP}-even Higgs boson is the observed Higgs boson. In type-I, it is challenging to simultaneously accommodate the light mass of the charged Higgs boson and the constraints from theory, electroweak precision data, Higgs data, , and direct search bounds. Consequently, the parameter space is extremely curtailed, which predicts somewhat definite phenomenological signatures. We find that the mass of the pseudoscalar Higgs boson, , is the most crucial factor in the phenomenology of the charged Higgs boson. If is light, the charged Higgs boson decays mainly into . When is above the threshold, the dominant decay mode is into . Over the whole viable parameter space, we study all the possible production and decay modes of charged Higgs bosons at the LHC, and suggest three efficient channels: (i) ; (ii) ; (iii) . Based on the sophisticated signal-background analyses including detector simulation, we showed that the significance of the first final state is large, that of the second one is marginal around three, but the third one suffers from huge related backgrounds.

    hep-phPRD(2022)·36 citations
  11. 12*

    Photon Fragmentation in the Antenna Subtraction Formalism

    Thomas Gehrmann🇨🇭 · Robin Schürmann🇨🇭

    The theoretical description of photon production at particle colliders combines direct photon radiation and fragmentation processes, which can not be separated from each other for definitions of photon isolation used in experimental measurements. The theoretical description of these processes must account for collinear parton-photon configurations, retaining the dependence on the photon momentum fraction, and includes the parton-to-photon fragmentation functions. We extend the antenna subtraction method to include photon fragmentation processes up to next-to-next-to-leading order (NNLO) in QCD. Collinear photon radiation is handled using newly introduced fragmentation antenna functions and associated phase space mappings. We derive the integrated forms of the fragmentation antenna functions and describe their interplay with the mass factorisation of the photon fragmentation functions. The construction principles of antenna subtraction terms up to NNLO for identified photons are outlined, thereby enabling the application of the method to different photon production processes at colliders.

    hep-phJHEP(2022)·40 citations
  12. 13*

    Effect of electron spin polarization in laser-assisted electron-proton scattering

    I. Dahiri🇲🇦 · M. Baouahi🇲🇦 · M. Jakha🇲🇦 · S. Mouslih🇲🇦 · B. Manaut🇲🇦 · S. Taj🇲🇦

    This work aims to study theoretically the electron-proton scattering for initially spin-polarized electrons in the presence of a circularly polarized electromagnetic field. Using the first Born approximation and the Dirac-Volkov states for dressed electrons, we derive an analytic expression for the differential cross-section with the help of the spin-helicity formalism. Meanwhile, a well-known concept of spin-flip and spin non-flip differential cross sections is applied. The influence of the electromagnetic field on the degree of polarization of the scattered electron is investigated, and the effect of electron spin polarization is examined. We found that the initial spin of the electron can be affected depending on its kinetic energy during the scattering process. This work is a continuation of a recent paper in which we studied the unpolarized electron-proton scattering in the presence of a laser field (Dahiri, et al., Laser Phys. Lett. 18 (2021) 096001).

    hep-phChin.J.Phys.(2022)·7 citations
  13. 14*

    Competition of chiral soliton lattice and Abrikosov vortex lattice in QCD with isospin chemical potential

    Martin Spillum Grønli🇳🇴 · Tomáš Brauner🇳🇴

    We investigate the thermodynamics of two-flavor quark matter in presence of nonzero isospin chemical potential and external magnetic field. It is known that at sufficiently high isospin chemical potential, charged pions undergo Bose-Einstein condensation (BEC). The condensate behaves as a superconductor, exhibiting Meissner effect in weak external magnetic fields. Stronger fields stress the superconducting state, turning it first into an Abrikosov lattice of vortices, and eventually destroying the condensate altogether. On the other hand, for sufficiently strong magnetic fields and low-to-moderate isospin chemical potential, the ground state of quantum chromodynamics (QCD) is expected to be a spatially modulated condensate of neutral pions, induced by the chiral anomaly: the chiral soliton lattice (CSL). We map the phase diagram of QCD as a function of isospin chemical potential and magnetic field in the part of the parameter space accessible to a low-energy effective field theory description of QCD. Our main result is an explicit account of the competition between the CSL and the Abrikosov vortex lattice. This is accomplished by adopting a fast numerical algorithm for finding the vortex lattice solution of the equation of motion and the corresponding Gibbs energy. We find that the Abrikosov vortex lattice phase persists in the phase diagram, separating the uniform charged pion BEC phase from the CSL phase. The precise layout of the phase diagram depends sensitively on the choice of the vacuum pion mass.

    hep-phnucl-thEPJC(2022)·23 citations
  14. 15*

    PDF bias and flavor dependence in TMD distributions

    Marcin Bury🇵🇱 · Francesco Hautmann🇧🇪 · Sergio Leal-Gomez🇦🇹 · Ignazio Scimemi🇪🇸 · Alexey Vladimirov🇩🇪 · Pia Zurita🇩🇪

    Transverse momentum dependent (TMD) distributions match collinear parton density functions (PDF) in the limit of small transverse distances, which is accounted for by global extractions of TMD distributions. We study the influence of the collinear PDF value and uncertainties on the determination of unpolarized TMD distributions and the description of Drell-Yan (DY) and Z-boson production measurements at low transverse momenta. We take into account, for the first time, flavor-dependent non-perturbative TMD profiles. We carry out a Bayesian analysis to incorporate the propagation of PDF uncertainties into TMD extractions. We find that collinear PDF uncertainties and non-perturbative TMD flavor dependence are both essential to obtain reliable TMD determinations, and should be included in future global analyses.

    hep-phJHEP(2022)·88 citations
  15. 16*

    Pair-production of the charged IDM scalars at high energy CLIC

    Jan Klamka🇵🇱 · Aleksander Filip Zarnecki🇵🇱

    The Inert Doublet Model (IDM) is a simple extension of the Standard Model, introducing an additional Higgs doublet that brings in four new scalar particles. The lightest of the IDM scalars is stable and is a good candidate for a dark matter particle. The potential of discovering the IDM scalars in the experiment at the Compact Linear Collider (CLIC), an ee collider proposed as the next generation infrastructure at CERN, has been tested for two high-energy running stages, at 1.5 TeV and 3 TeV centre-of-mass energy. The CLIC sensitivity to pair-production of the charged IDM scalars was studied using the full detector simulation with GEANT4 for selected high-mass IDM benchmark scenarios and the semi-leptonic final state. To extrapolate full simulation results to a wider range of IDM benchmark scenarios, the CLIC detector model defined in the DELPHES fast simulation framework was modified to take into account the had. beam-induced background. Results of the study indicate that heavy charged IDM scalars can be discovered at CLIC for most of the considered benchmark scenarios, up to masses of the order of 1 TeV.

    hep-phhep-exEPJC(2022)·12 citations
  16. 17*

    NLO quark self-energy and dispersion relation using the hard thermal loop resummation

    Sumit🇮🇳 · Najmul Haque🇮🇳 · Binoy Krishna Patra🇮🇳

    Using the hard-thermal-loop (HTL) resummation in real-time formalism, we study the next-to-leading order (NLO) quark self-energy and corresponding NLO dispersion laws. In NLO, we have replaced all the propagators and vertices with the HTL-effective ones in the usual quark self-energy diagram. Additionally, a four-point vertex diagram also contributes to the quark NLO self-energy. We calculate the usual quark self-energy diagram and the four-point vertex diagram separately. Using those, we express the NLO quark self-energy in terms of the three- and four-point HTL-effective vertex functions. Using the Feynman parametrization, we express the integrals containing the three- and four-point HTL effective vertex functions in terms of the solid angles. After completing the solid angle integrals, we numerically calculate the momentum integrals in the NLO quark self-energy and plot them as a function of the ratio of momentum and energy. Using the NLO quark self-energy, we plot the NLO correction to dispersion laws.

    hep-phJHEP(2023)·7 citations
  17. 18*

    Invariant Representation Driven Neural Classifier for Anti-QCD Jet Tagging

    Taoli Cheng🇨🇦 · Aaron Courville🇨🇦

    We leverage representation learning and the inductive bias in neural-net-based Standard Model jet classification tasks, to detect non-QCD signal jets. In establishing the framework for classification-based anomaly detection in jet physics, we demonstrate that, with a \emph{well-calibrated} and \emph{powerful enough feature extractor}, a well-trained \emph{mass-decorrelated} supervised Standard Model neural jet classifier can serve as a strong generic anti-QCD jet tagger for effectively reducing the QCD background. Imposing \emph{data-augmented} mass-invariance (and thus decoupling the dominant factor) not only facilitates background estimation, but also induces more substructure-aware representation learning. We are able to reach excellent tagging efficiencies for all the test signals considered. In the best case, we reach a background rejection rate of 51 and a significance improvement factor of 3.6 at 50 \% signal acceptance, with the jet mass decorrelated. This study indicates that supervised Standard Model jet classifiers have great potential in general new physics searches.

    hep-phcs.LGhep-exJHEP(2022)·5 citations
  18. 19*

    Disentangling Long and Short Distances in Momentum-Space TMDs

    Markus A. Ebert🇩🇪 · Johannes K. L. Michel🇺🇸 · Iain W. Stewart🇺🇸 · Zhiquan Sun🇺🇸

    The extraction of nonperturbative TMD physics is made challenging by prescriptions that shield the Landau pole, which entangle long- and short-distance contributions in momentum space. The use of different prescriptions then makes the comparison of fit results for underlying nonperturbative contributions not meaningful on their own. We propose a model-independent method to restrict momentum-space observables to the perturbative domain. This method is based on a set of integral functionals that act linearly on terms in the conventional position-space operator product expansion (OPE). Artifacts from the truncation of the integral can be systematically pushed to higher powers in . We demonstrate that this method can be used to compute the cumulative integral of TMD PDFs over in terms of collinear PDFs, accounting for both radiative corrections and evolution effects. This yields a systematic way of correcting the naive picture where the TMD PDF integrates to a collinear PDF, and for unpolarized quark distributions we find that when renormalization scales are chosen near , such corrections are a percent-level effect. We also show that, when supplemented with experimental data and improved perturbative inputs, our integral functionals will enable model-independent limits to be put on the nonperturbative OPE contributions to the Collins-Soper kernel and intrinsic TMD distributions.

    hep-phJHEP(2022)·46 citations
  19. 20*

    A new generation of simultaneous fits to LHC data using deep learning

    Shayan Iranipour🇬🇧 · Maria Ubiali🇬🇧

    We present a new methodology that is able to yield a simultaneous determination of the Parton Distribution Functions (PDFs) of the proton alongside any set of parameters that determine the theory predictions; whether within the Standard Model (SM) or beyond it. The SIMUnet methodology is based on an extension of the NNPDF4.0 neural network architecture, which allows the addition of an extra layer to simultaneously determine PDFs alongside an arbitrary number of such parameters. We illustrate its capabilities by simultaneously fitting PDFs with a subset of Wilson coefficients within the Standard Model Effective Field Theory framework and show how the methodology extends naturally to larger subsets of Wilson coefficients and to other SM precision parameters, such as the strong coupling constant or the heavy quark masses.

    hep-phJHEP(2022)·53 citations
  20. 21*

    Primordial black holes from an electroweak phase transition

    Peisi Huang🇺🇸 · Ke-Pan Xie🇺🇸

    We propose a mechanism that forms primordial black holes (PBHs) via a first-order electroweak phase transition (FOEWPT). The FOEWPT is realized by extending the Standard Model with a real singlet scalar, while the PBH formation is achieved by the collapse of non-topological solitons called Fermi-balls. Such solitons form via trapping fermions in the false vacuum during the FOEWPT, and they eventually collapse into PBHs due to the internal Yukawa attractive force. We demonstrate that a scenario with PBH dark matter candidate can exist, and the typical experimental signals include FOEWPT gravitational waves and the multi-lepton/jet or displaced vertex final states at the LHC.

    hep-phastro-ph.COPRD(2022)·76 citations
  21. 22*

    Electroweak flavour unification

    Joe Davighi🇨🇭 · Joseph Tooby-Smith🇬🇧

    We propose that the electroweak and flavour quantum numbers of the Standard Model (SM) could be unified at high energies in an anomaly-free gauge model. All the SM fermions are packaged into two fundamental fields, and , thereby explaining the origin of three families of fermions. The SM Higgs, being electroweakly charged, necessarily becomes charged also under flavour when embedded in the UV model. It is therefore natural for its vacuum expectation value to couple only to the third family. The other components of the UV Higgs fields are presumed heavy. Extra scalars are needed to break this symmetry down to the SM, which can proceed via `flavour-deconstructed' gauge groups; for instance, we propose a pattern for the left-handed factor. When the heavy Higgs components are integrated out, realistic quark Yukawa couplings with in-built hierarchies are naturally generated without any further ingredients, if we assume the various symmetry breaking scalars condense at different scales. The CKM matrix that we compute is not a generic unitary matrix, but it can precisely fit the observed values.

    hep-phhep-thJHEP(2022)·52 citations
  22. 23*

    Signatures of leptophilic t-channel dark matter from active galactic nuclei

    Marina Cermeño🇧🇪 · Céline Degrande🇧🇪 · Luca Mantani🇬🇧

    In this work, we study indirect photon signatures of leptophilic dark matter (DM) coming from Centaurus A, where a DM density spike is believed to have survived to date contrary to the case of our galaxy. We consider a model where DM is a Majorana fermion which interacts with right-handed electrons via a scalar mediator. Assuming that the photons measured from the core of Cen A are coming from SM processes, we derive constraints on the average annihilation cross section which are 7 orders of magnitude stronger than the ones from measurements of the Galactic Center. Focusing on the allowed parameter space range, we calculate the flux of photons coming from the radiative DM-electron scattering in the AGN jets and the circular polarisation asymmetry of these photons. We find that this flux is two orders of magnitude lower than the background but its circular polarisation asymmetry can reach values close to , indicating the need to experimentally exploit the high fraction of circular polarisation in order to detect these interactions. Since the origin of the photons in the GeV-TeV range from Cen A is not completely clear and an exotic origin is compatible with the measurements as well, we also consider the scenario in which synchrotron radiation can only partially explain the photon flux and we fit the excess with signals coming from DM annihilation, finding a best fit for a DM candidate with a mass GeV and a coupling .

    hep-phPRD(2022)·12 citations
  23. 24*

    Empirical capture cross sections for cosmic neutrino detection with and

    Vedran Brdar🇺🇸 · Ryan Plestid🇺🇸 · Noemi Rocco🇺🇸

    The nuclei Sm and Tm have been identified as attractive candidates for the detection of the cosmic neutrino background. Both isotopes undergo first-forbidden non-unique beta decays which inhibits a prediction of their spectral shape using symmetries alone and this has, so far, obstructed a definitive prediction of their neutrino capture cross sections. In this work we point out that for both elements the so-called "-approximation" is applicable and this effectively reduces the spectral shape to deviate by at most from the one that would arise if beta decays were of the allowed type. Using measured half-lives we extract the relevant nuclear matrix element and predict the neutrino capture cross sections for both isotopes at level, accounting for a number of relevant effects including radiative corrections and the finite size of the nuclei. We obtained for Tm and for Sm. This method is robust as it does not rely on the data points near the end-point of the beta spectrum which may be contaminated by atomic physics effects, namely shake-up and shake-off. Finally, we calculate the target mass which is necessary for cosmic neutrino discovery and discuss several bottlenecks and respective solutions associated to the experimental program. We conclude that the detection of cosmic neutrino background by neutrino capture on Sm and Tm is achievable and free from theoretical limitations but still subject to technical issues that should be further investigated by the experimentalists in the context of the proposed PTOLEMY project.

    hep-phhep-exnucl-exnucl-thPRC(2022)·14 citations
  24. 25*

    Causality constraints on corrections to Einstein gravity

    Simon Caron-Huot🇨🇦 · Yue-Zhou Li🇨🇦 · Julio Parra-Martinez🇺🇸 · David Simmons-Duffin🇺🇸

    We study constraints from causality and unitarity on graviton scattering in four-dimensional weakly-coupled effective field theories. Together, causality and unitarity imply dispersion relations that connect low-energy observables to high-energy data. Using such dispersion relations, we derive two-sided bounds on gravitational Wilson coefficients in terms of the mass of new higher-spin states. Our bounds imply that gravitational interactions must shut off uniformly in the limit , and prove the scaling with expected from dimensional analysis (up to an infrared logarithm). We speculate that causality, together with the non-observation of gravitationally-coupled higher spin states at colliders, severely restricts modifications to Einstein gravity that could be probed by experiments in the near future.

    hep-thgr-qchep-phJHEP(2023)·189 citations
  25. 26*

    Experimental test of the third quantization of the electromagnetic field

    J.D. Franson🇺🇸

    Each mode of the electromagnetic field is mathematically equivalent to a harmonic oscillator described by a wave function in the quadrature representation. An approach was recently introduced in which the wave function was further quantized to produce a field operator [J.D. Franson, Phys. Rev. A 104, 063702 (2021)]. This approach allows a generalization of quantum optics and quantum electrodynamics based on an unknown mixing angle that is somewhat analogous to the Cabibbo angle or the Weinberg angle. The theory is equivalent to conventional quantum electrodynamics if , while it predicts a new form of inelastic photon scattering if . Here we report the results of an optical scattering experiment that set an upper bound of at the 99% confidence level, provided that the particles created by the field operator have negligible mass. High-energy experiments would be required to test the theory if the mass of these particles is very large.

    quant-phhep-exhep-phPRA(2022)·0 citations
  26. 27*

    reaction for studying charge symmetry breaking in the interaction

    Yutaro Iizawa🇯🇵 · Daisuke Jido🇯🇵 · Takatsugu Ishikawa🇯🇵

    We discuss charge symmetry breaking in the interaction. In order to investigate the and interactions at low energies, we propose to utilize the and reactions. They are symmetric under the exchange of both the pion and nucleon isospin partners in the final states. This advantage allows us to study charge symmetry breaking in the interaction. We calculate the differential cross sections of these reactions with stopped kaons theoretically and discuss the possibility to extract the scattering length and effective range of the scattering. With stopped kaons, the interaction takes place dominantly in the spin-triplet state thanks to the deuteron spin and -wave dominance of the scattering amplitudes at the low energy. We find that the ratio of the differential cross sections as a function of the invariant mass between the two reactions is useful for revealing how charge symmetry breaking, or isospin symmetry breaking appears in the low-energy scattering.

    nucl-thhep-phnucl-exPRC(2022)·3 citations
  27. 28*

    Dynamic density correlations in a baryon rich fluid using Mori-Zwanzig-Nakjima projection operator method

    Guruprasad Kadam🇮🇳

    In this work, we calculate the dynamic density correlations using Mori-Zwanzig-Nakajima projection operator method. With a judicious choice of slow variables we derive the evolution equations for these slow variables starting from generalised Langevin equation. We get the hydrodynamic form of density correlations function which consist of two acoustic peaks: also called Brillouin peaks, and one thermal peak: also called Rayleigh peak. We then estimate the dynamic density correlations near the critical point using critical exponents extracted from the statistical bootstrap model of hadronic matter. We find that the bulk viscosity contributes to the sound attenuation at leading order while the thermal conductivity contribute at sub-leading order . On the other hand, only the thermal conductivity contributes at leading order to the thermal diffusivity. We discuss the implications of these results in a search for the QCD critical point in the heavy-ion collision experiments.

    nucl-thhep-phhep-thEPJC(2022)·1 citation
  28. 29*

    A stable and causal model of magnetohydrodynamics

    Jay Armas🇳🇱 · Filippo Camilloni🇮🇹

    We formulate the theory of first-order dissipative magnetohydrodynamics in an arbitrary hydrodynamic frame under the assumption of parity-invariance and discrete charge symmetry. We study the mode spectrum of Alfvén and magnetosonic waves as well as the spectrum of gapped excitations and derive constraints on the transport coefficients such that generic equilibrium states with constant magnetic fields are stable and causal under linearised perturbations. We solve these constraints for a specific equation of state and show that there exists a large family of hydrodynamic frames that renders the linear fluctuations stable and causal. This theory does not require introducing new dynamical degrees of freedom and therefore is a promising and simpler alternative to Müller-Israel-Stewart-type theories. Together with a detailed analysis of transport, entropy production and Kubo formulae, the theory presented here is well suited for studying dissipative effects in various contexts ranging from heavy-ion collisions to astrophysics.

    hep-thastro-ph.HEgr-qchep-ph+1JCAP(2022)·41 citations
  29. 30*

    Standard model parameters from top quark measurements at LHC with ATLAS and CMS

    Sebastian Wuchterl (on behalf of the ATLAS and CMS Collaborations)🇩🇪

    Theoretical predictions for standard model (SM) processes involving top quarks, such as top quark-antiquark pair or single top production, depend on fundamental SM parameters like the strong coupling constant or the top quark mass. By confronting predictions with measurements performed at the ATLAS and CMS Collaboration using data collected at the CERN LHC in the second data taking period, these parameters can be determined precisely. In these proceedings, recent results measuring SM and top quark properties are presented.

    hep-exhep-ph0 citations
  30. 31*

    The holographic space-time and black hole remnants as dark matter

    Aurélien Barrau🇫🇷

    The holographic space-time approach to inflation provides a well defined and self-contained framework to study the early universe. Based on a quasi-local quantum gravity theory generalizing string theory beyond AdS backgrounds, it addresses fundamental questions like the arrow of time and the entropy of the initial cosmological state. It was recently argued that it also provides a naturel explanation for dark matter in the form of primordial black holes. The orignal idea however suffers from troubles that can be cured by considering instead Planck relics. This possibility is investigated and paths for observational confirmation are pointed out.

    gr-qcastro-ph.COhep-phhep-thPLB(2022)·4 citations
  31. 32*

    Vortices in polar and phases of He

    G.E. Volovik🇫🇮

    Recently new topological phase of superfluid He has been discovered -- the phase, which is obtained by strong polarization of the nematic polar phase. We consider half-quantum vortices, which are formed in rotating cryostat, and discuss the evolution of the vortex lattice in the process of the transition from the polar phase to the -phase via the spin-polarized polar phase.

    cond-mat.otherhep-phJETP Lett.(2022)·4 citations
  32. 33*

    Constraints on Single-Field Inflation from the BOSS Galaxy Survey

    Giovanni Cabass🇺🇸 · Mikhail M. Ivanov🇺🇸 · Oliver H. E. Philcox🇺🇸 · Marko Simonović🇨🇭 · Matias Zaldarriaga🇺🇸

    Non-local primordial non-Gaussianity (NLPNG) is a smoking gun of interactions in single-field inflationary models, and can be written as a combination of the equilateral and orthogonal templates. We present the first constraints on these from the redshift-space galaxy power spectra and bispectra of the Baryon Oscillation Spectroscopic Survey (BOSS) data. These are the first such measurements independent of the cosmic microwave background fluctuations. We perform a consistent analysis that includes all necessary nonlinear corrections generated by NLPNG, and vary all relevant cosmological and nuisance parameters in a global fit to the data. Our conservative analysis yields joint limits on the amplitudes of the equilateral and orthogonal shapes, , (both at 68\% CL). These can be used to derive constraints on coefficients of the effective single-field inflationary Lagrangian; in particular, we find that the sound speed of inflaton fluctuations has the bound at 95\% CL. Fixing the quadratic galaxy bias and cosmological parameters, the constraints can be tightened to , (68\% CL).

    astro-ph.COgr-qchep-phhep-thPRL(2022)·176 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.