PaperPanorama

HEP Phenomenology·hep-ph

Fri·May 21, 2021

32 papers23 primary·9 cross-listed·reconstructed*

  1. 01*

    Jet quenching from heavy to light ion collisions

    B.G. Zakharov🇷🇺

    We perform an analysis of jet quenching in heavy and light ion collisions for scenarios without and with quark-gluon plasma formation in collisions. We find that the results for these scenarios are very similar, and both of them are in reasonable agreement with data for heavy ion collisions. However, their results become differ significantly for light nuclei. Using the parameters fitted to heavy ion data on the nuclear modification factor , we make predictions for 0.2 and 7 TeV O+O collisions that can be verified by future experiments at RHIC and the LHC.

    hep-phnucl-thJHEP(2021)·41 citations
  2. 02*

    Heavy Neutrino searches through Double-Bang Events at Super-Kamiokande, DUNE, and Hyper-Kamiokande

    Mack Atkinson🇨🇦 · Pilar Coloma🇪🇸 · Ivan Martinez-Soler🇺🇸 · Noemi Rocco🇺🇸 · Ian M. Shoemaker🇺🇸

    A variety of new physics scenarios allow for neutrinos to up-scatter into a heavy neutral lepton state. For a range of couplings and neutrino energies, the heavy neutrino may travel some distance before decaying to visible final states. When both the up-scattering and decay occur within the detector volume, these "double bang" events produce distinctive phenomenology with very low background. In this work, we first consider the current sensitivity at Super-Kamiokande via the atmospheric neutrino flux, and find current data may already provide new constraints. We then examine projected future sensitivity at DUNE and Hyper-Kamiokande, including both atmospheric and beam flux contributions to double-bang signals.

    hep-phhep-exJHEP(2022)·49 citations
  3. 03*

    Impact of the LHCb fixed-target data on the intrinisic component in the nucleon

    Rafal Maciula🇵🇱 · Antoni Szczurek🇵🇱

    We discuss the impact of the new LHCb fixed-target data for production on the intrinsic component in the nucleon wave function. Within the scenario presented here neither the traditional gluon-gluon fusion or quark-antiquark annihilation mechanisms calculated in the -factorization approach nor their counterparts from the collinear next-to-leading order collinear framework are sufficient to describe the transverse momentum and rapidity distributions of mesons. First the -pair production within the standard frameworks is considered. Here a crucial role of the hadronization effects at low energies and low transverse momenta is found and discussed, which was not analyzed in previous studies. A contribution related to intrinsic component in the nucleon wave function is included in addition. Two models of the symmetric () intrinsic charm (IC) component are considered. The intrinsic charm (or ) contribution needs to be regularized in order to obtain a suppression of the minijet spectrum present in the phenomenological minijet model, commonly used in Monte Carlo generators. We show that in our model the regularization parameter can be obtained from the fit to the LHCb fixed-target data under consideration here. We discuss uncertainties of our calculations (scale, charm quark mass, fragmentation function) as well as set limits on the IC probability. According to our model the intrinsic charm probability allows to significantly improve description of the LHCb data but the number is rather uncertain.

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

    Interpolating 't Hooft model between instant and front forms

    Bailing Ma🇺🇸 · Chueng-Ryong Ji🇺🇸

    The 't Hooft model, i.e. the two-dimensional quantum chromodynamics in the limit of infinite number of colors, is interpolated by an angle parameter between for the instant form dynamics (IFD) and for the light-front dynamics (LFD). With this parameter , we formulate the interpolating mass gap equation which takes into account the non-trivial vacuum effect on the bare fermion mass to find the dressed fermion mass. Our interpolating mass gap solutions link the IFD and LFD results with the parameter. We find the interpolation angle independent characteristic energy function which satisfies the energy-momentum dispersion relation of the dressed fermion, identifying the renormalized fermion mass function and the wave function renormalization factor. Using the dressed fermion propagator interpolating between IFD and LFD, we derive the corresponding quark-antiquark bound-state equation in the interpolating formulation. The mass spectra of mesons bearing the feature of the Regge trajectories are found independent of the -parameter for the equal mass quark and antiquark bound-states. The Gell-Mann - Oakes - Renner relation for the pionic ground-state in the zero fermion mass limit is confirmed indicating that the spontaneous breaking of the chiral symmetry occurs regardless of the quantization for . We obtain the corresponding bound-state wave functions and discuss their reference frame dependence. Applying them for the computation of the so-called quasi parton distribution functions, we note a possibility of utilizing not only the reference frame dependence but also the interpolation angle dependence to get an alternative effective approach to the LFD-like results.

    hep-phhep-thnucl-thPRD(2021)·21 citations
  5. 05*

    The contour gauge in use: telling untold

    I.V. Anikin🇷🇺

    In Quantum Field Theory, we discuss the main features of the (non-local) contour gauge which extends the local axial-type gauge used in most approaches. Based on the gluon geometry, we demonstrate that the contour gauge does not suffer from the residual gauge. We discuss the useful correspondence between the contour gauge conception and the Hamiltonian (Lagrangian) formalism. Having compared the local and non-local gauges, we again advocate the advantage of the contour gauge use.

    hep-phPhys.Part.Nucl.Lett.(2022)·5 citations
  6. 06*

    The Logarithmic Contributions to the Polarized and Operator Matrix Elements in Deeply Inelastic Scattering

    J. Blümlein🇩🇪 · A. De Freitas🇩🇪 · M. Saragnese🇩🇪 · C. Schneider🇦🇹 · K. Schönwald🇩🇪

    We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inelastic scattering in the asymptotic region to 3-loop order in the fixed-flavor number scheme and present the corresponding expressions for the polarized massive operator matrix elements needed in the variable flavor number scheme. The calculation is performed in the Larin scheme. For the massive operator matrix elements and the complete results are presented. The expressions are given in Mellin- space and in momentum fraction -space.

    hep-phhep-thPRD(2021)·31 citations
  7. 07*

    A Unified Yukawa Interaction for the Standard Model of Quarks and Leptons

    Ying Zhang🇨🇳

    To address fermion mass hierarchy and flavor mixings in the quark and lepton sectors, a minimal flavor structure without any redundant parameters beyond phenomenological observables is proposed via decomposition of the Standard Model Yukawa mass matrix into a bi-unitary form. After reviewing the roles and parameterization of the factorized matrix and in fermion masses and mixings, we generalize the mechanism to up- and down-type fermions to unify them into a universal quark/lepton Yukawa interaction. In the same way, a unified form of the description of the quark and lepton Yukawa interactions is also proposed, which shows a similar picture as the unification of gauge interactions.

    hep-phMod.Phys.Lett.A(2021)·2 citations
  8. 08*

    Non-equilibrium dynamics of a scalar field with quantum backreaction

    Kimmo Kainulainen🇫🇮 · Olli Koskivaara🇫🇮

    We study the dynamical evolution of coupled one- and two-point functions of a scalar field in the 2PI framework at the Hartree approximation, including backreaction from out-of-equilibrium modes. We renormalize the 2PI equations of motion in an on-shell scheme in terms of physical parameters. We present the Hartree-resummed renormalized effective potential at finite temperature and critically discuss the role of the effective potential in a non-equilibrium system. We follow the decay and thermalization of a scalar field from an initial cold state with all energy stored in the potential, into a fully thermalized system with a finite temperature. We identify the non-perturbative processes of parametric resonance and spinodal instability taking place during the reheating stage. In particular we study the unstable modes in the region where the vacuum 1PI effective action becomes complex and show that such spinodal modes can have a dramatic effect on the evolution of the one-point function. Our methods can be easily adapted to simulate reheating at the end of inflation.

    hep-phastro-ph.COgr-qchep-thJHEP(2021)·29 citations
  9. 09*

    Contact Interactions at Future Circular Collider based Muon-Proton Colliders

    Gural Aydin (Hatay Mustafa Kemal University)🇹🇷 · Yusuf Oguzhan Günaydin (Kahramanmaras Sütcü Imam University)🇹🇷 · Mehmet Sahin (Usak University)🇹🇷 · Saleh Sultansoy (TOBB ETU)🇹🇷 · Mehmet Türker Tarakcioglu (Kahramanmaras Sütcü Imam University)🇹🇷

    Recently proposed Future Circular Collider based muon-proton colliders will allow investigating lepton-hadron interactions at the highest center-of-mass energy. In this study, we investigate the potential of these colliders for a four-fermion contact interactions search. Regarding the constructive and destructive interferences of contact interactions, we estimated discovery, observation, and exclusion limits on the compositeness scale for the left-left, right-right, left-right, and right-left helicity structures. This study's findings show that the FCC-based {\mu}p colliders have great potential for investigating four-fermion contact interactions.

    hep-phhep-exActa Phys.Polon.B(2022)·6 citations
  10. 10*

    Implications of constraints on and

    Sébastien Descotes-Genon🇫🇷 · Svjetlana Fajfer🇸🇮 · Jernej F. Kamenik🇸🇮 · Martín Novoa-Brunet🇫🇷

    We investigate the consequences of deviations from the Standard Model observed in transitions for flavour-changing neutral-current processes involving down-type quarks and neutrinos, under generic assumptions concerning the structure of New Physics. We derive the relevant Wilson coefficients within an effective field theory approach respecting the SM gauge symmetry, including right-handed currents and assuming a flavour structure based on approximate symmetry, and only SM-like light neutrinos. We discuss correlations among and branching ratios in the case of linear Minimal Flavour Violation and in a more general framework, highlighting in each case the role played by various New Physics scenarios proposed to explain deviations. This talk is based on arXiv:2005.03734.

    hep-phhep-ex4 citations
  11. 11*

    Constraining active-sterile neutrino transition magnetic moments at DUNE near and far detectors

    Thomas Schwetz🇩🇪 · Albert Zhou🇩🇪 · Jing-Yu Zhu🇨🇳

    We consider the sensitivity of the DUNE experiment to a heavy neutral lepton, HNL (also known as sterile neutrino) in the mass range from a few MeV to a few GeV, interacting with the Standard Model via a transition magnetic moment to the active neutrinos, the so-called dipole portal. The HNL is produced via the upscattering of active neutrinos, and the subsequent decay inside the detector provides a single-photon signal. We show that the tau-neutrino dipole portal can be efficiently probed at the DUNE far detector, using the tau-neutrino flux generated by neutrino oscillations, while the near detector provides better sensitivity to the electron- and muon-neutrino dipole portal. DUNE will be able to explore large regions of currently unconstrained parameter space and has comparable sensitivity to other planned dedicated experiments, such as SHiP. We also comment briefly on the sensitivity to pure HNL mixing with the tau neutrino at the DUNE far detector.

    hep-phJHEP(2020)·55 citations
  12. 12*

    Study on triple-hadron bound states with Gaussian expansion method

    Tian-Wei Wu🇨🇳 · Li-Sheng Geng🇨🇳

    In recent years, more and more exotic hadronic states have been discovered successively. Many of them can be explained as hadronic molecules, such as , , and pentaquark states. Analogous to the formation of nuclei, we study three-body hadronic molecules with the Gaussian expansion method and predict the existence of the , , and bound states, which are likely to be found in the current and updated facilities.

    hep-phhep-exFew Body Syst.(2021)·7 citations
  13. 13*

    New Physics and Two Boosted W-jets plus Missing Energy

    Qing-Hong Cao🇨🇳 · Nuo Chen🇨🇳 · Hao-Ran Jiang🇨🇳 · Bin Li🇨🇳 · Yandong Liu🇨🇳

    We show that the signature of two boosted -jets plus large missing energy is very promising to probe heavy charged resonances () through the process of where denotes dark matter candidate. The hadronic decay mode of the boson is considered to maximize the number of signal events. When the mass split between and is large, one has to utilize the jet-substructure technique to analyze the boosted -jet. For illustration we consider the process of chargino pair production at the LHC, i.e., , and demonstrate that the proposed signature is able to cover more parameter space of and than the conventional signature of multiple leptons plus missing energy. More importantly, the signature of our interests is not sensitive to the spin of heavy resonances.

    hep-phhep-exCPC(2021)·0 citations
  14. 14*

    StringSpinner -- adding spin to the PYTHIA string fragmentation

    Albi Kerbizi🇮🇹 · Leif Lönnblad🇸🇪

    StringSpinner is a plugin for the introduction of the spin effects in the hadronization part of the PYTHIA 8 event generator. The spin effects are generated for pseudoscalar meson production by propagating the quark polarization along the fragmentation chain according to the rules of the quantum mechanical string+ model. By using parametrizations for the transversity parton distribution functions, StringSpinner allows to simulate the polarized semi inclusive deep inelastic scattering process on protons and neutrons. The instructions to use StringSpinner and to modify the parametrizations of the transversity distribution functions are presented, as well as an example of the calculation of the Collins asymmetries as obtained from simulations of the transversely polarized semi inclusive deep inelastic scattering process.

    hep-phComput.Phys.Commun.(2022)·27 citations
  15. 15*

    Density perturbations in axion-like particles: classical vs quantum field treatment

    Sankha Subhra Chakrabarty🇮🇹

    Axions and axion-like particles are bosonic quantum fields. They are often assumed to follow classical field equations due to their high degeneracy in the phase space. In this work, we explore the disparity between classical and quantum field treatments in the context of density and velocity fields of axions. Once the initial density and velocity field are specified, the evolution of the axion fluid is unique in the classical field treatment. However, in the quantum field treatment, there are many quantum states consistent with the given initial density and velocity field. We show that evolutions of the density perturbations for these quantum states are not necessarily identical and, in general, differ from the unique classical evolution. To illustrate the underlying physics, we consider a system of large number of bosons in a one-dimensional box, moving under the gravitational potential of a heavy static point-mass. We ignore the self-interactions between the bosons here. Starting with homogeneous number density and zero velocity field, we determine the density perturbations in the linear regime in both quantum and classical field theories. We find that classical and quantum evolutions are identical in the linear regime if only one single-particle state is occupied by all the bosons and the self-interaction is absent. If more than one single-particle states are occupied, the density perturbations in quantum evolutions differ from the classical prediction after a certain time which depends upon the parameters of the system.

    hep-phastro-ph.COhep-thPRD(2021)·9 citations
  16. 16*

    Event topology and constituent-quark scaling of elliptic flow in heavy-ion collisions at the Large Hadron Collider using a multiphase transport model

    Neelkamal Mallick🇮🇳 · Sushanta Tripathy🇮🇹 · Raghunath Sahoo🇮🇳

    Transverse spherocity is an event shape observable, which separates the events based on their geometrical shapes. In this work, we use transverse spherocity to study the identified light flavor production in heavy-ion collisions using A Multi-Phase Transport (AMPT) model. We obtain the elliptic flow coefficients for pions, kaons and protons in Pb+Pb collisions at TeV as a function of transverse spherocity and collision centrality. Also, we study the number of constituent-quark (NCQ) scaling of elliptic flow which interprets the dominance of the quark degrees of freedom at the early stages of the collision. We observe a clear dependence of the elliptic flow for identified particles on transverse spherocity. It is found that the NCQ-scaling is strongly violated in events with low transverse spherocity compared to transverse spherocity-integrated events, confirming the fragmentation-based hadronization mechanism for high-momentum partons involved in the dynamics of jetty-like events.

    hep-phhep-exhep-thnucl-ex+1EPJC(2022)·19 citations
  17. 17*

    Higgs boson decays with lepton flavor violation in the symmetric SSM

    Ze-Ning Zhang🇨🇳 · Hai-Bin Zhang🇨🇳 · Jin-Lei Yang🇨🇳 · Shu-Min Zhao🇨🇳 · Tai-Fu Feng🇨🇳

    Recently, the ATLAS and CMS Collaborations reported the latest experimental upper limits on the branching ratios of the lepton flavor violating (LFV) 125 GeV Higgs boson decays, , , and . In this paper, we mainly investigate the LFV Higgs boson decays , , and in the minimal supersymmetric extension of the Standard Model with local gauge symmetry. At the same time, the corresponding constraints from the LFV rare decays , , , and muon are considered to analyze the numerical results.

    hep-phPRD(2021)·16 citations
  18. 18*

    Impact of inclusive hadron production data on nuclear gluon PDFs

    nCTEQ Collaboration: P. Duwentäster🇩🇪 · L. A. Husová🇩🇪 · T. Ježo🇩🇪 · M. Klasen🇩🇪 · K. Kovařík🇩🇪 · A. Kusina🇵🇱 · K. F. Muzakka🇩🇪 · F. I. Olness🇺🇸 · I. Schienbein🇫🇷 · J. Y. Yu🇺🇸

    A precise knowledge of nuclear parton distribution functions (nPDFs) is -- among other things -- important for the unambiguous interpretation of hard process data taken in pA and AA collisions at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC). The available fixed target data for deep inelastic scattering (DIS) and Drell-Yan (DY) lepton pair production mainly constrain the light quark distributions. It is hence crucial to include more and more collider data in global analyses of nPDFs in order to better pin down the different parton flavors, in particular the gluon distribution at small x. To help constrain the nuclear gluon PDF, we extend the nCTEQ15 analysis by including single inclusive hadron (SIH) production data from RHIC (PHENIX and STAR) and LHC (ALICE). In addition to the DIS, DY and SIH data sets, we will also include LHC W/Z production data. As the SIH calculation is dependent on hadronic fragmentation functions (FFs), we use a variety of FFs available in the literature to properly estimate this source of uncertainty. We study the impact of these data on the PDFs, and compare with both the nCTEQ15 and nCTEQ15WZ sets. The calculations are performed using a new implementation of the nCTEQ code (nCTEQ++) including a modified version of INCNLO which allows faster calculations using pre-computed grids. The extension of the nCTEQ15 analysis to include the SIH data represents an important step toward the next generation of PDFs.

    hep-phnucl-thPRD(2021)·50 citations
  19. 19*

    Four-Loop Gauge and Three-Loop Yukawa Beta-Functions in a General Renormalizable Theory

    Alexander Bednyakov🇷🇺 · Andrey Pikelner🇷🇺

    We present the beta functions of gauge and Yukawa couplings in general four-dimensional quantum field theory, at four and three loops, respectively. The essence of our approach is fixing unknown coefficients in the most general ansatz for beta-functions by direct calculation in several simplified models. We apply our results to the Standard Model and its extension with an arbitrary number of Higgs doublets and provide expressions for all four-loop gauge couplings beta-functions with matrix Yukawa interactions.

    hep-phhep-thPRL(2021)·36 citations
  20. 20*

    Preserving New Physics while Simultaneously Unfolding All Observables

    Patrick Komiske🇺🇸 · W. Patrick McCormack🇺🇸 · Benjamin Nachman🇺🇸

    Direct searches for new particles at colliders have traditionally been factorized into model proposals by theorists and model testing by experimentalists. With the recent advent of machine learning methods that allow for the simultaneous unfolding of all observables in a given phase space region, there is a new opportunity to blur these traditional boundaries by performing searches on unfolded data. This could facilitate a research program where data are explored in their natural high dimensionality with as little model bias as possible. We study how the information about physics beyond the Standard Model is preserved by full phase space unfolding using an important physics target at the Large Hadron Collider (LHC): exotic Higgs boson decays involving hadronic final states. We find that if the signal cross section is high enough, information about the new physics is visible in the unfolded data. We will show that in some cases, quantifiably all of the information about the new physics is encoded in the unfolded data. Finally, we show that there are still many cases when the unfolding does not work fully or precisely, such as when the signal cross section is small. This study will serve as an important benchmark for enhancing unfolding methods for the LHC and beyond.

    hep-phhep-exphysics.data-anPRD(2021)·14 citations
  21. 21*

    Ultralight dark photon and Casimir effect

    Abdaljalel Alizzi🇷🇺 · Z.K. Silagadze🇷🇺

    We investigate the influence of a dark photon on the Casimir effect and calculate the corresponding leading contribution to the Casimir energy. For expected magnitudes of the photon - dark photon mixing parameter, the influence turns out to be negligible. The plasmon dispersion relation is also not noticeably modified by the presence of a dark photon.

    hep-phhep-thquant-phInt.J.Theor.Phys.(2022)·1 citation
  22. 22*

    Axion Mass from Magnetic Monopole Loops

    JiJi Fan🇺🇸 · Katherine Fraser🇺🇸 · Matthew Reece🇺🇸 · John Stout🇺🇸

    We show that axions interacting with abelian gauge fields obtain a potential from loops of magnetic monopoles. This is a consequence of the Witten effect: the axion field causes the monopoles to acquire an electric charge and alters their energy spectrum. The axion potential can also be understood as a type of instanton effect due to a Euclidean monopole worldline winding around its dyon collective coordinate. We calculate this effect, which has features in common with both nonabelian instantons and Euclidean brane instantons. To provide consistency checks, we argue that this axion potential vanishes in the presence of a massless charged fermion and that it is robust against the presence of higher-derivative corrections in the effective Lagrangian. Finally, as a first step toward connecting with particle phenomenology and cosmology, we discuss the regime in which this potential is important in determining the dark matter relic abundance in a hidden sector containing an abelian gauge group, monopoles, and axions.

    hep-phhep-thPRL(2021)·55 citations
  23. 23*

    Smoke and mirrors: Neutron star internal heating constraints on mirror matter

    David McKeen🇨🇦 · Maxim Pospelov🇺🇸 · Nirmal Raj🇨🇦

    Mirror sectors have been proposed to address the problems of dark matter, baryogenesis, and the neutron lifetime anomaly. In this work we study a new, powerful probe of mirror neutrons: neutron star temperatures. When neutrons in the neutron star core convert to mirror neutrons during collisions, the vacancies left behind in the nucleon Fermi seas are refilled by more energetic nucleons, releasing immense amounts of heat in the process. We derive a new constraint on the allowed strength of neutron--mirror-neutron mixing from observations of the coldest (sub-40,000 Kelvin) neutron star, PSR 21443933. Our limits compete with laboratory searches for neutron--mirror-neutron transitions but apply to a range of mass splittings between the neutron and mirror neutron that is 19 orders of magnitude larger. This heating mechanism, also pertinent to other neutron disappearance channels such as exotic neutron decay, provides a compelling physics target for upcoming ultraviolet, optical and infrared telescopes to study thermal emissions of cold neutron stars.

    hep-phastro-ph.HEastro-ph.SRhep-exPRL(2021)·55 citations
  24. 24*

    Cosmic Expansion: A mini review of the Hubble-Lemaitre tension

    Francis-Yan Cyr-Racine🇺🇸

    We present here a lightning review of the status of the Hubble-Lemaître tension. Instead of discussing the broad array of proposed solutions found in the literature, we focus here on the assumptions made to measure the Hubble constant from cosmic microwave background and baryon acoustic oscillation data on the one hand, and from a cepheid-calibrated distance ladder on the other hand. From this discussion, we extract two important lessons that inform which kind of physics-based solutions could plausibly resolve this tension.

    astro-ph.COhep-ph3 citations
  25. 25*

    Ferromagnetic instability in PAAI in the sky

    R. B. MacKenzie🇨🇦 · M. B. Paranjape🇨🇦 · U. A. Yajnik🇮🇳

    We study an idealised plasma of fermions, coupled through an abelian gauge force , and which is asymmetric in that the masses of the oppositely charged species are greatly unequal. The system is dubbed PAAI, plasma asymétrique, abélien et idéalisé. It is argued that due to the ferromagnetic instability that arises, the ground state gives rise to a complex of domain walls. This complex being held together by stresses much stronger than cosmic gravity, does not evolve with the scale factor and along with the heavier oppositely charged partners simulates the required features of Dark Energy with mass scale for the lighter fermions in the micro-eV to nano-eV range. Further, residual -magnetic fields through mixture with standard magnetic fields, can provide the seed for cosmic-scale magnetic fields. Thus the scenario can explain several cosmological puzzles including Dark Energy.

    hep-thastro-ph.COcond-mat.str-elhep-phM. B. Paranjape et al. (eds.), Quantum Th…·0 citations
  26. 26*

    Comment on Straight lightning as a signature of macroscopic dark matter By Nathaniel Starkman, Harrison Winch, Jagjit Singh Sidhu, and Glenn Starkman

    V. Cooray🇸🇪 · G. Cooray🇸🇪 · M. Rubinstein🇨🇭 · F. Rachidi🇨🇭

    In this short paper, we present some comments on the paper: Straight lightning as a signature of macroscopic dark matter, by Nathaniel Starkman, Harrison Winch, Jagjit Singh Sidhu, and Glenn Starkman, Phys. Rev. D 103, 063024, Published 18 March 2021.

    physics.app-phhep-ph1 citation
  27. 27*

    An analytic model for gravitational collapse of spherical matter under mixed pressure

    Shuichi Yokoyama🇯🇵

    We investigate spherically symmetric gravitational collapse of thick matter shell without radiation in the Einstein gravity with cosmological constant. The orbit of the infalling thick matter is determined by imposing an equation of state for the matter near interface, where pressure constituted of the transverse component and the longitudinal one is proportional to energy density. We present analytic solutions for the equation of state and discuss parameter region to satisfy physical conditions such as the absence of the shell crossing singularity, the monotonic increase of the emergent infinite redshift surface and energy conditions. We finally show that adopting the definition presented in arXiv:2005.13233 the total energy in this time-dependent system is invariant under the given time evolution.

    gr-qchep-phhep-thInt.J.Mod.Phys.D(2023)·3 citations
  28. 28*

    Multicomponent multiscatter capture of Dark Matter

    Cosmin Ilie🇺🇸 · Caleb Levy🇺🇸

    In recent years, the usefulness of astrophysical objects as Dark Matter (DM) probes has become more and more evident, especially in view of null results from direct detection and particle production experiments. The potentially observable signatures of DM gravitationally trapped inside a star, or another compact astrophysical object, have been used to forecast stringent constraints on the nucleon-Dark Matter interaction cross section. Currently, the probes of interest are: at high red-shifts, Population III stars that form in isolation, or in small numbers, in very dense DM minihalos at , and, in our own Milky Way, neutron stars, white dwarfs, brown dwarfs, exoplanets, etc. Of those, only neutron stars are single-component objects, and, as such, they are the only objects for which the common assumption made in the literature of single-component capture, i.e. capture of DM by multiple scatterings with one single type of nucleus inside the object, is valid. In this paper, we present an extension of this formalism to multi-component objects and apply it to Pop III stars, thereby investigating the role of He on the capture rates of Pop III stars. As expected, we find that the inclusion of the heavier He nuclei leads to an enhancement of the overall capture rates, further improving the potential of Pop III stars as Dark Matter probes.

    astro-ph.COhep-phPRD(2021)·22 citations
  29. 29*

    Does Hubble Tension Signal a Breakdown in FLRW Cosmology?

    Chethan Krishnan🇮🇳 · Roya Mohayaee🇫🇷 · Eoin Ó Colgáin🇰🇷 · M. M. Sheikh-Jabbari🇮🇷 · Lu Yin🇰🇷

    The tension between early and late Universe probes of the Hubble constant has motivated various new FLRW cosmologies. Here, we reanalyse the Hubble tension with a recent age of the Universe constraint. This allows us to restrict attention to matter and a dark energy sector that we treat without assuming a specific model. Assuming analyticity of the Hubble parameter , and a generic low redshift modification to flat CDM, we find that low redshift data () and well-motivated priors only permit a dark energy sector close to the cosmological constant . This restriction rules out late Universe modifications within FLRW. We show that early Universe physics that alters the sound horizon can yield an upper limit of km/s/Mpc. Since various local determinations may be converging to km/s/Mpc, a breakdown of the FLRW framework is a plausible resolution. We outline how future data, in particular strongly lensed quasar data, could also provide further confirmations of such a resolution.

    astro-ph.COgr-qchep-phhep-thClass.Quant.Grav.(2021)·193 citations
  30. 30*

    Dilatonic (Anti-)de Sitter Black Holes and Weak Gravity Conjecture

    Karim Benakli🇫🇷 · Carlo Branchina🇫🇷 · Gaëtan Lafforgue-Marmet🇫🇷

    Einstein-Maxwell-dilaton theory with non-trivial dilaton potential is known to admit asymptotically flat and (Anti-)de Sitter charged black hole solutions. We investigate the conditions for the presence of horizons as function of the parameters mass , charge and dilaton coupling strength . We observe that there is a value of which separate two regions, one where the black hole is Reissner-Nordström-like from a region where it is Schwarzschild-like. We find that for de Sitter and small non-vanishing , the extremal case is not reached by the solution. We also discuss the attractive or repulsive nature of the leading long distance interaction between two such black holes, or a test particle and one black hole, from a world-line effective field theory point of view. Finally, we discuss possible modifications of the Weak Gravity Conjecture in the presence of both a dilatonic coupling and a cosmological constant.

    hep-thgr-qchep-phJHEP(2021)·16 citations
  31. 31*

    QCD transition at the physical point, and its scaling window from twisted mass Wilson fermions

    A. Yu. Kotov🇩🇪 · M. P. Lombardo🇮🇹 · A. Trunin🇷🇺

    We study the scaling properties of the finite temperature QCD phase transition, for light quark masses ranging from the heavy quark regime to their physical values. The lattice results are obtained in the fixed scale approach from simulations of flavours of Wilson fermions at maximal twist. We identify an order parameter free from the the linear contributions in mass due to additive renormalization and regular terms in the Equation of State, which proves useful for the assessment of the hypothesized universal behaviour. We find compatibility with the 3D universality class for the physical pion mass and temperatures MeV MeV. We discuss violation of scaling at larger masses and a possible cross-over to mean field behaviour. The chiral extrapolation MeV of the pseudocritical temperature is robust against predictions of different universality classes and consistent with its estimate from the Equation of State for the physical pion mass.

    hep-lathep-phhep-thPLB(2021)·83 citations
  32. 32*

    Multiscalar-metric gravity: cosmological constant screening and emergence of massive-graviton dark components

    Yury F. Pirogov🇷🇺

    In the multiscalar-metric frameworks, the issues of the vacuum energy/cosmological constant (CC) screening due to the Weyl-scale enhancement of the Diff gauge symmetry, along with emergence of the massive dark gravity components through the gravitational Higgs mechanism are considered. A generic dark gravity model is developed, with the two extreme versions of the model of particular interest based on General Relativity (GR) and its classically equivalent Weyl transverse alternative being compared and argued to be, generally, inequivalent. The so constructed spontaneously broken Weyl Transverse Relativity (WTR) is proposed as a viable beyond-GR effective field theory of gravity, with screening of the Lagrangian CC, superseded by the induced one, and emergence of the massive tensor and scalar gravitons as the dark gravity components. A basic concept with the spontaneously broken Diff gauge symmetry/relativity -- in particular, WTR vs. GR -- as a principle source of the emergent dark gravity components of the Universe is put forward.

    gr-qcastro-ph.COhep-phGrav.Cosmol.(2022)·3 citations

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