PaperPanorama

HEP Phenomenology·hep-ph

Tue·Oct 3, 2023

39 papers21 primary·18 cross-listed·reconstructed*

  1. 01*

    Beyond-DFT Calculations for Accurate Prediction of Sub-GeV Dark Matter Experimental Reach

    Elizabeth A. Peterson🇺🇸 · Samuel L. Watkins🇺🇸 · Christopher Lane🇺🇸 · Jian-Xin Zhu🇺🇸

    As the search space for light dark matter (DM) has shifted to sub-GeV DM candidate particles, increasing attention has turned to solid state detectors built from quantum materials. While traditional solid state detector targets (e.g. Si or Ge) have been utilized in searches for dark matter (DM) for decades, more complex, anisotropic materials with narrow band gaps are desirable for detecting sub-MeV dark matter through DM-electron scattering and absorption channels. In order to determine if a novel target material can expand the search space for light DM it is necessary to determine the projected reach of a dark matter search conducted with that material in the DM mass - DM-electron scattering cross-section parameter space. The DM-electron scattering rate can be calculated from first-principles with knowledge of the loss function, however the accuracy of these predictions is limited by the first-principles level of theory used to calculate the dielectric function. Here we perform a case study on silicon, a well-studied semiconducting material, to demonstrate that traditional Kohn-Sham density functional theory (DFT) calculations erroneously overestimate projected experimental reach. We show that for silicon this can be remedied by the incorporation of self-energy corrections as implemented in the GW approximation. Moreover, we emphasize the care that must taken in selecting the appropriate level of theory for predicting experimental reach of next-generation complex DM detector materials.

    hep-phcond-mat.mes-hallhep-ex4 citations
  2. 02*

    On the Quantum Uncertainty of the Neutron Electric Dipole Moment

    Octavio Guerrero🇺🇸 · Libertad Barrón-Palos🇲🇽 · Daniel Sudarsky🇲🇽

    The continued interest in placing bounds on the neutron's Electric Dipole Moment (EDM) is due to the implications regarding the characteristics of the strong interaction and, in particular, its behavior under the CP symmetry. In this work, we discuss the apparent tension resulting from the discrepancy of about 13 orders of magnitude between the current bounds and the expected quantum uncertainty in the relevant quantity. We offer a resolution of the "puzzle" in terms of the notion of a weak measurement, using a version of the corresponding formalism adapted to consideration of the nEDM experiment at the Spallation Neutron Source at the Oak Ridge National Laboratory.

    hep-phquant-phAnnals Phys.(2024)·5 citations
  3. 03*

    Dynamics of heavy quarks in the Fock space

    Kamil Serafin🇨🇳 · María Gómez-Rocha🇪🇸 · Jai More🇮🇳 · S. D. Głazek🇵🇱

    This paper concerns a method of describing hadrons that starts with the canonical front form Hamiltonian of QCD. The method is developed in the relatively simple context of QCD with only heavy quarks. We regulate its canonical Hamiltonian by introducing a vanishingly small gluon mass . For positive , the small- gluon divergences become ultraviolet and hence they are renormalized in the same way the ultraviolet transverse divergences are. This is done using the renormalization group procedure for effective particles. Up to the second order of expansion of the renormalized Hamiltonian in powers of the quark-gluon coupling constant , only the quark mass-squared and gluon-exchange divergences require counter terms. In these circumstances, we calculate an effective potential between quarks in heavy quarkonia in an elementary way, replacing all the quarkonium-state components with gluons of mass by only one component with just one gluon that is assigned a mass , comparable to or exceeding the scale of typical relative momenta of bound quarks. In the limit of and large two results are obtained. (1) While the color-singlet quarkonium mass eigenvalue stays finite and physically reasonable in that limit, the eigenvalues for single quarks and octet quarkonia are infinite. (2) The effective quark-antiquark potential is quadratic as a function of the distance and spherically symmetric for typical separations between quarks but becomes logarithmic and no longer spherically symmetric for large separations. Our conclusion indicates how to systematically improve upon the approximations made in this paper.

    hep-phhep-thPRD(2024)·8 citations
  4. 04*

    Multibaryon configurations in a simple chromomagnetic model

    Aaron Park🇰🇷

    In this work, we study the multibaryon configurations in a simple chromomagnetic model. We first construct the wave function of the multibaryon states using the multiquark configuration. We consider all possible quantum numbers assuming the spatial part of the wave function to be totally symmetric. Then, we calculate the color-spin factors for tetrabaryons, pentabaryons and hexabaryons in the flavor SU(3) breaking case.

    hep-phnucl-thPRD(2024)·0 citations
  5. 05*

    Ratios of Hidden-Charm Compact Pentaquark Decay Widths in Quark-Diquark Model

    Alexandra A. Dobrynina🇷🇺 · Alexander Ya. Parkhomenko🇷🇺 · Alexey V. Zinchenko🇷🇺

    A number of resonances comparable with a hypothesis of hidden-charm pentaquark is observed by the LHCb Collaboration. We interpret these narrow resonances as compact hidden-charm diquark-diquark-antiquark systems. Within this assumption, an interplay between the charmonium and open-charm modes is considered. Ratios of such modes for non-strange pentaquarks are obtained and discussed.

    hep-ph0 citations
  6. 06*

    Ultralight Dirac neutrinos from nearly degenerate Higgs doublets

    Pei-Hong Gu🇨🇳

    Two Higgs doublets respect a mirror symmetry with spontaneous violation so that their vacuum expectation values can realize a small difference. Under this symmetry, three newly introduced right-handed neutrinos rather than the standard model fermions perform an odd transformation. Accordingly the neutrino masses and the charged fermion masses respectively are proportional to the difference and sum of the vacuum expectation values of two Higgs doublets. From a phenomenological perspective, such nearly degenerate Higgs doublets with large cancellation are equivalent to a Dirac seesaw mechanism with high suppression.

    hep-phNPB(2025)·1 citation
  7. 07*

    On the Observables of Renormalizable Interactions

    Kang-Sin Choi🇰🇷

    We reconsider the renormalization of scalar mass and point out that the quantum correction to the physical observable, as opposed to the bare parameter, of a renormalizable operator, is technically insensitive to ultraviolet physics and independent of the regularization scheme. It is expressed as the difference in the same quantities at different energy scales, maintaining the same asymptotics. Thus, any sensible regularization cancels out the divergences, including the quadratic ones, and yields the same finite corrections. To this end, we first show that the vacuum polarization of quantum electrodynamics is independent of the regularization scheme and a gauge-dependent quadratic divergence is canceled in the observable. We then calculate the quantum correction to the Higgs mass squared by the top-quark loop. It is again finite and regularization-scheme independent. For large external momentum, the correction of the pole mass-squared is dominated by power running, resulting in an order of 1 percent correction. In particular, the effect of heavy fields on the scalar mass correction is suppressed.

    hep-phhep-thJ.Korean Phys.Soc.(2024)·9 citations
  8. 08*

    Gluon TMDs from J/ production in longitudinally polarized deeply inelastic scattering

    Huachao liu🇨🇳 · Xiupeng xie🇨🇳 · Zhun Lu🇨🇳

    We investigate the feasibility of exploring the gluon transverse-momentum-dependent distribution functions (TMDs) inside a longitudinally polarized nucleon. We utilize quarkonium production via the color-octet mechanism combined with TMD formalism in semi-inclusive deeply inelastic scattering (SIDIS) at low transverse momentum as a tool to access polarized gluon TMDs. The corresponding cross-section of the process is expressed in terms of gluon TMDs and non-relativistic QCD matrix elements. We provide the expressions for the azimuthal asymmetries of production in SIDIS with a unpolarized beam colliding on longitudinally polarized nucleon. The asymmetry is contributed by the time-reversal-odd gluon TMD . The maximum possible asymmetry deduced from the positivity bound is sizable and could be measured. We also estimate the double longitudinal spin asymmetry of production using a spectator model result for .

    hep-phPLB(2024)·4 citations
  9. 09*

    Jet Lorentz factor constraint for GRB 221009A based on the optical depth of the TeV photons

    Duan-yuan Gao🇨🇳 · Yuan-Chuan Zou🇨🇳

    The recent detection of tera-electronvolt (TeV) photons from the record-breaking gamma-ray burst GRB 221009A during its prompt phase poses challenges for constraining its Lorentz factor. We re-evaluate the constraints on the jet Lorentz factor considering a two-zone model, wherein the TeV photons originate from the external shock region while the lower energy MeV photons come from the internal prompt emission region. By properly accounting for the evolution of the MeV photon spectrum and light curve, we calculate the optical depth for TeV photons and derive a minimum Lorentz factor about 300. It is consistent with the afterglow modeling for the TeV emission.

    hep-phastro-ph.HEApJL(2023)·7 citations
  10. 10*

    Exclusive production of in hadron-hadron ultraperipheral collisions

    Xiao-Peng Wang🇨🇳 · Ya-Ping Xie🇨🇳 · Yin Huang🇨🇳 · Xu-Rong Chen🇨🇳

    Understanding the production mechanisms and utilizing them as probes to investigate the structure of exotic states represent some of the most actively studied research areas in particle physics. In this study, we present a theoretical analysis of the charmed meson in the and reactions, considering as a molecule. The differential cross-section and total cross-section for the photoproduction of in the and reactions are presented for nucleus-nucleus (nucleon-nucleon) ultraperipheral collisions at HL-LHC and RHIC, respectively. Taking into account the integrated luminosity per typical run and the luminosity of photons from the nucleus (nucleon), we observe a significant event count for production in p-p ultraperipheral collisions at HL-LHC.

    hep-phPRD(2024)·4 citations
  11. 11*

    Secluded Scalar Dark Matter and the Muon Anomalous Magnetic Moment

    Karim Ghorbani🇮🇷

    We consider a dark matter model with a singlet scalar, , as our dark matter (DM) candidate which is secluded from the Standard Model (SM) and annihilates to the singlet scalar, , via a contact interaction. The singlet scalar, , has a leptophilic interaction with the SM leptons and may decay leptonically at tree level, and decays into a pair of photons at loop level. The focus in this work is to consider DM masses below 10 GeV. It is found a viable secluded region in the parameter space after imposing the observed relic density. There is a one-loop interaction between scalar dark matter and the atomic electron in this model. We then apply the available direct detection bounds from Xenon10, Xenon1T, and DarkSide on the DM-electron elastic scattering cross section. While the model can explain the muon anomalous magnetic moment, we put bounds from current and future lepton collider experiments.

    hep-phJ.Phys.G(2024)·2 citations
  12. 12*

    Look how it runs!

    Siegfried Bethke🇩🇪

    Quantum Chromodynamics predicts that the strong coupling strength decreases with increasing energy or momentum transfer, and vanishes at asymptotically high energies. The history and the status of experimental tests of asymptotic freedom are summarised in this review.

    hep-phhep-exInt.J.Mod.Phys.A(2024)·0 citations
  13. 13*

    The double fermionic contribution to the four-loop quark-to-gluon splitting function

    G. Falcioni (Zurich U. and Turin U.)🇮🇹 · F. Herzog (U. Edinburgh, Higgs Ctr. Theor. Phys.)🇬🇧 · S. Moch (Hamburg U., Inst. Theor. Phys. II)🇩🇪 · J. Vermaseren (Nikhef, Amsterdam)🇳🇱 · A. Vogt (Liverpool U., Dept. Math.)🇬🇧

    We have computed the first 30 even-N moments for the double fermionic (nf^2) part of the quark-to-gluon splitting function P_{gq} at the fourth order of perturbative QCD via the renormalization of off-shell operator matrix elements. From these results we have determined the all-N form, and hence the exact x-space expression, using systems of Diophantine equations for its coefficients. The dominant and subdominant leading small-x nf^2 contributions to P_{gq}^(3)(x) are of the form 1/x ln x and ln^4 x, respectively; the leading large-x term is ln^4 (1-x). The coefficient of the first of these is new, the other two agree with results obtained before and thus provide checks of our results.

    hep-phPLB(2024)·53 citations
  14. 14*

    Broadening of particle distributions in electron- and (anti)neutrino-nucleus scattering from QED interactions

    Oleksandr Tomalak🇺🇸 · Ivan Vitev🇺🇸

    Proper interpretation of past, current, and future data on lepton-nucleus reactions requires a clear separation between quantum electrodynamics (QED) and strong interaction effects inside the nucleus. First studies of QED in-medium lepton dynamics have set a theoretical framework to derive electron-nucleus and (anti)neutrino-nucleus cross-section corrections. We employ this approach to quantitatively compute the effects of Glauber photon-mediated multiple re-scattering within the nuclear medium. We find that the relativistic charged lepton acquires momentum of order transverse to its direction of propagation inside the nucleus. This broadening sizably deflects expected electron tracks and suppresses scattering cross sections. Precise extraction of the nucleon and nuclear structure by electron and muon probes should, thus, take the QED nuclear medium angular redistribution of particles into account. Our results further show that the associated effects in (anti)neutrino-nucleus scattering with measured final-lepton energy are significant only at the kinematical endpoints.

    hep-phhep-exnucl-exnucl-thPRD(2023)·6 citations
  15. 15*

    Stringy phenomenology with preon models

    Risto Raitio🇫🇮

    We compare, following Pati, global symmetries our topological supersymmetric preon model with the heterotic E_8 x E_8 string theory. We include Pati's supergravity based preon model in this work and compare the preon interactions of his model to ours. Based on preon-string symmetry comparison and preon phenomenological results we conclude that the fundamental particles are likely preons rather than standard model particles.

    hep-phJHEP Grav.Cosmol.(2024)·2 citations
  16. 16*

    Towards 6D Little String Theory of Particles

    Risto Raitio🇫🇮

    A model for particles based on preons in chiral, vector and tensor/graviton supermultiplets of unbroken global supersymmetry is engineered. The framework of the model is little string theory. Phenomenological predictions are discussed.

    hep-phJHEP Grav.Cosmol.(2024)·0 citations
  17. 17*

    Partial Rate Matrix for Dark Matter Scattering

    Benjamin Lillard🇺🇸

    I present a highly efficient integration method for scattering calculations, and a ``partial rate matrix'' that encodes the scattering rate as a function of the orientation of the detector. This replaces the original multidimensional rate integral with a simple exercise in vector multiplication, speeding up the rate calculation by a factor of around . I include a scheme to fully factorize the dark matter particle model, its astrophysical velocity distribution, and the properties of the target material from each other, enabling efficient calculation of the partial rate matrix even in studies comparing large sets of these input functions. This is now the only sensible way to evaluate the dark matter scattering rate in anisotropic detector materials. It is straightforward to generalize this method to other difficult but linear problems.

    hep-phastro-ph.IMmath-phmath.MP+1PRL(2025)·11 citations
  18. 18*

    Wavelet-Harmonic Integration Methods

    Benjamin Lillard🇺🇸

    A new integration method drastically improves the efficiency of the dark matter direct detection calculation. In this work I introduce a complete, orthogonal basis of spherical wavelet-harmonic functions, designed for the new vector space integration method. This factorizes the numeric calculation into a ``vector'' that depends only on the astrophysical velocity distribution; a second vector, depending only on the detector form factor; and a scattering matrix defined on the basis functions, which depends on the details of the dark matter (DM) particle model (e.g.~its mass). For common spin-independent DM--Standard Model interactions, this scattering matrix can be evaluated analytically in the wavelet-harmonic basis. This factorization is particularly helpful for the more complicated analyses that have become necessary in recent years, especially those involving anisotropic detector materials or more realistic models of the local DM velocity distribution. With the new method, analyses studying large numbers of detector orientations and DM particle models can be performed more than 10~million times faster. This paper derives several analytic results for the spherical wavelets, including an extrapolation in the space of wavelet coefficients, and a generalization of the vector space method to a much broader class of linear functional integrals. Both results are highly relevant outside the field of DM direct detection.

    hep-phastro-ph.IMmath-phmath.MP+1PRD(2025)·11 citations
  19. 19*

    Flavor Fragmentation Function Factorization

    Andrew J. Larkoski🇺🇸 · Duff Neill🇺🇸

    A definition of partonic jet flavor that is both theoretically well-defined and experimentally robust would have profound implications for measurements and predictions especially for heavy flavor applications. Recently, a definition of jet flavor was introduced as the net flavor flowing along the direction of the Winner-Take-All axis of a jet which is soft safe to all orders, but not collinear safe. Here, we exploit the lack of collinear safety and propose a factorization theorem of perturbative flavor fragmentation functions that resum collinear divergences and describe the evolution of flavor from the short distance of jet production to the long distance at which hadronization occurs. Collinear flavor evolution is governed by a small modification of the DGLAP equations. We present a detailed all-orders analysis and identify exact relations that must hold amongst the various anomalous dimensions by probability conservation and the existence of fixed points of the renormalization group flow. We explicitly validate the factorization theorem at one-loop order, and demonstrate its consistency at two loops in particular flavor channels. Starting at two-loops, constraints on phase space imposed by flavor measurements potentially allow for non-trivial soft contributions, but we demonstrate that they are scaleless and so explicitly vanish, ensuring that soft particles are summed inclusively and all divergences are exclusively collinear in nature. This factorization theorem opens the door to precision calculations with identified flavor in the infrared.

    hep-phhep-exnucl-exnucl-thJHEP(2024)·4 citations
  20. 20*

    Probing the Short-Distance Structure of the Quark-Gluon Plasma with Energy Correlators

    Zhong Yang🇨🇳 · Yayun He🇨🇳 · Ian Moult🇺🇸 · Xin-Nian Wang🇨🇳

    Energy-energy-correlators (EEC's) are a promising observable to study the dynamics of jet evolution in the quark-gluon plasma (QGP) through its imprint on angular scales in the energy flux of final-state particles. We carry out the first complete calculation of EEC's using realistic simulations of high-energy heavy-ion collisions, and dissect the different dynamics underlying the final distribution through analyses of jet propagation in a uniform medium. The EEC's of -jets in heavy-ion collisions are found to be enhanced by the medium response from elastic scatterings instead of induced gluon radiation at large angles. In the meantime, EEC's are suppressed at small angles due to energy loss and transverse momentum broadening of jet shower partons. These modifications are further shown to be sensitive to the angular scale of the in-medium interaction, as characterized by the Debye screening mass. Experimental verification and measurement of such modifications will shed light on this scale, and the short-distance structure of the QGP in heavy-ion collisions.

    hep-phnucl-thPRL(2024)·109 citations
  21. 21*

    Vortex Effects in Merging Black Holes and Saturons

    Gia Dvali🇩🇪 · Oleg Kaikov🇩🇪 · Florian Kuhnel🇩🇪 · Juan Sebastián Valbuena-Bermúdez🇩🇪 · Michael Zantedeschi🇨🇳

    Vorticity has recently been suggested to be a property of highly-spinning black holes. The connection between vorticity and limiting spin represents a universal feature shared by objects of maximal microstate entropy, so-called saturons. Using -ball-like saturons as a laboratory for black holes, we study the collision of two such objects and find that vorticity can have a large impact on the emitted radiation as well as on the charge and angular momentum of the final configuration. As black holes belong to the class of saturons, we expect that the formation of vortices can cause similar effects in black hole mergers, leading to macroscopic deviations in gravitational radiation. This could leave unique signatures detectable with upcoming gravitational-wave searches, which can thereby serve as a portal to macroscopic quantum effects in black holes.

    hep-phastro-ph.HEgr-qchep-thPRL(2024)·22 citations
  22. 22*

    Kinetic relaxation and nucleation of Bose stars in self-interacting wave dark matter

    Mudit Jain🇺🇸 · Wisha Wanichwecharungruang🇺🇸 · Jonathan Thomas🇺🇸

    We revisit kinetic relaxation and soliton/Boson star nucleation in fuzzy scalar dark matter featuring short-ranged self-interactions , alongside gravitational self-interactions. We map out the full curve of nucleation timescale for both repulsive () and attractive () short-ranged self-interaction strength, and in doing so reveal two new points. Firstly, besides the two usual terms, and , in the total relaxation rate , there is an additional cross term arising due to interference between gravitational and short-ranged self-interaction scattering amplitudes. This yields a critical repulsive interaction strength , at which the relaxation rate is smallest and serves as the transition point between typical net attractive self-interaction (), and net repulsive self-interaction (). Secondly, while in the net attractive regime, nucleation time scale is similar to inverse relaxation time scale , in the net repulsive regime nucleation occurs at a delayed time . We confirm our analytical understanding by performing 3D field simulations with varying average mass density , box size and grid size .

    astro-ph.COhep-phnlin.PSPRD(2024)·32 citations
  23. 23*

    The Standard Model and the Lattice

    Michael Creutz🇺🇸

    The standard model maps smoothly onto a conventional lattice gauge formulation, including the parity violation of the weak interactions. The formulation makes use of the pseudo-reality of the weak group and requires the inclusion a full generation of both leptons and quarks. As in continuum discussions, chiral eigenstates of the Dirac operator generate known anomalies, although with rough gauge configurations these are no longer exact zero modes of the Dirac operator.

    hep-lathep-phPRD(2024)·5 citations
  24. 24*

    Determination of the moments of the proton charge density: is there a proton radius puzzle?

    M. Atoui · M.B. Barbaro · M. Hoballah · C. Keyrouz · R. Kunne · M. Lassaut · D. Marchand · G. Quemener · E. Voutier

    The charge radius of the proton can be determined using two different kinds of experiments: the spectroscopy technique, measuring the hyperfine structure of hydrogen atoms, and the scattering technique, deducing the radius from elastic lepton scattering off a proton target. These two methods lead to quite different results, a discrepancy known as the "proton radius puzzle ". To shed light on this problem, we have proposed a novel method for the determination of spatial moments from densities expressed in the momentum space. This method provides a direct access not only to the second order moment, directly related to the proton radius, but to all moments of any real order larger than -3. The method is applied to the global analysis of proton electric form factor experimental data from Rosenbluth separation and low- experiments, paying specific attention to the evaluation of the systematic errors. Within this analysis, the integer order moments of the proton charge density are evaluated, the moment of second order leading to a new determination of the proton charge radius.

    nucl-thhep-phnucl-exNucl.Theor.(2023)·1 citation
  25. 25*

    Topology and geometry of elliptic Feynman amplitudes

    Claude Duhr🇩🇪 · Yu Jiao Zhu🇩🇪

    We report on the analytic computation of the 2-loop amplitude for Bhabha scattering in QED. We study the analytic structure of the amplitude, and reveal its underlying connections to hyperbolic Coxeter groups and arithmetic geometries of elliptic curves.

    hep-thhep-phPoS(2024)·1 citation
  26. 26*

    Quark masses and low energy constants in the continuum from the tadpole improved clover ensembles

    Zhi-Cheng Hu · Bo-Lun Hu · Ji-Hao Wang · Ming Gong · Liuming Liu · Peng Sun · Wei Sun · Wei Wang · Yi-Bo Yang · Dian-Jun Zhao

    We present the light-flavor quark masses and low energy constants using the 2+1 flavor full-QCD ensembles with stout smeared clover fermion action and Symanzik gauge actions. Both the fermion and gauge actions are tadpole improved self-consistently. The simulations are performed on 11 ensembles at 3 lattice spacings fm, 4 spatial sizes fm, 7 pion masses MeV, and several values of the strange quark mass. The quark mass is defined through the partially conserved axial current (PCAC) relation and renormalized to 2 GeV through the intermediate regularization independent momentum subtraction (RI/MOM) scheme. The systematic uncertainty of using the symmetric momentum subtraction (SMOM) scheme is also included. Eventually, we predict MeV, MeV, and MeV with the systematic uncertainties from lattice spacing determination, continuum extrapolation and renormalization constant included. We also obtain the chiral condensate MeV and the pion decay constant MeV in the chiral limit, and the next-to-leading order low energy constants and .

    hep-lathep-phPRD(2024)·71 citations
  27. 27*

    Modeling the Beam of Gravitational Radiation from a Cosmic String Loop

    Namitha Suresh🇺🇸 · David F. Chernoff🇺🇸

    We investigate exact and approximate techniques to calculate the emission of gravitational radiation from cosmic string loops in order to generate beam models covering the entire celestial sphere for a wide range of modes . One approach entails summing over contributions of stationary and nearly-stationary points of individual, factorized, left- and right-moving modes. This "multipoint method" generalizes traditional methods that rely on expansions around exact stationary points of mode products. A second complementary approach extends the method of steepest descent to generate an asymptotic description of the beam as . We present example calculations of the emission of power from cusp-containing loops and compare the results with those obtained by numerically exact techniques as well as by previous approaches. The multipoint method achieves its best results at an intermediate range of modes, improving over previous methods in terms of accuracy. It handles the emission from all regions of the loop not just those near cusps. We demonstrate this capability by making a detailed study of the "pseudocusp" phenomenon.

    astro-ph.COgr-qchep-phPRD(2024)·3 citations
  28. 28*

    Charged spinning fermionic configurations and a mass gap

    Vladimir Dzhunushaliev🇰🇿 · Vladimir Folomeev🇰🇬

    We consider a self-consistent axially symmetric system supported by a classical nonlinear spinor field minimally coupled to electric and magnetic Maxwell fields. The presence of the nonlinearity of the spinor field ensures the existence of a minimum positive energy of the system (a mass gap), of a minimum charge (a charge gap), and of a minimum magnetic moment. In turn, the presence of the electric charge results in qualitative changes in the behavior of physical characteristics of the systems under consideration as compared with the case of an electrically neutral spinor field. It is shown that, with a suitable choice of free system parameters, there exists a regular finite-energy particlelike solution describing a localized spinning object whose physical parameters correspond to the main characteristics of an electron/positron (including the spin equal to ), but with the characteristic size comparable to the corresponding Compton wavelength. Also, we show that four local Dirac equations are equivalent to two nonlocal equations.

    hep-thhep-phEPJC(2024)·3 citations
  29. 29*

    Nucleon electric polarizabilities and nucleon-pion scattering at physical pion mass

    Xuan-He Wang🇨🇳 · Zhao-Long Zhang🇨🇳 · Xiong-Hui Cao🇨🇳 · Cong-Ling Fan🇨🇳 · Xu Feng🇨🇳 · Yu-Sheng Gao🇨🇳 · Lu-Chang Jin🇺🇸 · Chuan Liu🇨🇳

    We present a lattice QCD calculation of the nucleon electric polarizabilities at the physical pion mass. Our findings reveal the substantial contributions of the states to these polarizabilities. Without considering these contributions, the lattice results fall significantly below the experimental values, consistent with previous lattice studies. This observation has motivated us to compute both the parity-negative scattering up to a nucleon momentum of GeV in the center-of-mass frame and corresponding matrix elements using lattice QCD. Our results confirm that incorporating dynamic contributions is crucial for a reliable determination of the polarizabilities from lattice QCD. This methodology lays the groundwork for future lattice QCD investigations into various other polarizabilities.

    hep-lathep-exhep-phnucl-exPRL(2024)·22 citations
  30. 30*

    Gluon PDF of the proton using twisted mass fermions

    Joseph Delmar🇺🇸 · Constantia Alexandrou🇨🇾 · Krzysztof Cichy🇵🇱 · Martha Constantinou🇺🇸 · Kyriakos Hadjiyiannakou🇨🇾

    In this paper, we present lattice QCD results for the -dependence of the unpolarized gluon PDF for the proton. We use one ensemble of maximally twisted mass fermions with a clover improvement, and the Iwasaki improved gluon action. The quark masses are tuned to produce a pion with a mass of 260 MeV. The ensemble has a lattice spacing of fm and a spatial extent of 3 fm. We employ the pseudo-distribution approach, which relies on matrix elements of non-local operators that couple to momentum-boosted hadrons. In this work, we use five values of the momentum boost between 0 and 1.67 GeV. The gluon field strength tensors of the non-local operator are connected with straight Wilson lines of varying length . The light-cone Ioffe time distribution (ITD) is extracted utilizing data with up to 0.56 fm and a quadratic parametrization in terms of the Ioffe time at fixed values of . We explore systematic effects, such as the effect of the stout smearing for the gluon operator, excited states effects, and the dependence on the maximum value of entering the fits to obtain the gluon PDF. Also, for the first time, the mixing with the quark singlet PDFs is eliminated using matrix elements with non-local quark operators that were previously analyzed within the quasi-PDF framework on the same ensemble. Here, we expand the data set for the quark singlet and reanalyze within the pseudo-PDFs method eliminating the corresponding mixing in the gluon PDF.

    hep-lathep-exhep-phnucl-thPRD(2023)·33 citations
  31. 31*

    Quantum Scales of Galaxies from Ultralight Dark Matter

    Jae-Weon Lee🇰🇷

    We propose that the ultralight dark matter (ULDM) model, in which dark matter particles have a tiny mass of , has characteristic scales for physical quantities of observed galaxies such as mass, size, acceleration, mass flux, and angular momentum from quantum mechanics. The typical angular momentum per dark matter particle is and the typical physical quantities are functions of specific angular momentum and average background density of the particles. If we use the Compton wavelength instead for the length scale, we can obtain bounds for these physical quantities. For example, there is an upper bound for acceleration of ULDM dominated objects, . We suggest that the physical scales of galaxies depend on the time of their formation and that these characteristic scales are related to some mysteries of observed galaxies. Future observations from the James Webb Space Telescope and NANOGrav can provide evidences for the presence and evolution of these scales.

    astro-ph.GAhep-phJ.Korean Phys.Soc.(2023)·4 citations
  32. 32*

    Localization of scalar field on the brane-world by coupling with gravity

    Heng Guo🇨🇳 · Yong-Tao Lu🇨🇳 · Cai-Ling Wang🇨🇳 · Yue Sun🇨🇳

    In this paper, we consider a coupling mechanism between the kinetic term and the gravity, in which a coupling function is introduced into the kinetic term of the five-dimensional scalar field. Based on this scenario, we investigate the localization of scalar fields in three specific braneworld models: the Minkowski brane, the de Sitter brane, and the Anti-de Sitter brane. The brane models considered here are regular with no singularity for scalar curvature. For the Minkowshi brane case, the zero mode can always be localized on the brane, and the massive modes can be localized or quasi-localized on the brane. For the dS brane case, two forms of factor is considered. The zero mode can always be localized, and the massive modes could be quasi-localized on the brane. Besides, with the second coupling factor, the scalar zero mode could be localized on the both sides of the origin of extra dimension, while the massive modes could be quasi-localized on the origin. Lastly, for the AdS brane case, the localization of the scalar zero mode requires the consideration of a coupling potential , while the massive modes can still be localized on the brane with an infinite number.

    hep-thgr-qchep-phJHEP(2024)·13 citations
  33. 33*

    Zero Modes of Massive Fermions Delocalize from Axion Strings

    Hengameh Bagherian🇺🇸 · Katherine Fraser🇺🇸 · Samuel Homiller🇺🇸 · John Stout🇺🇸

    Massless chiral excitations can arise from the interactions between a fermion and an axion string, propagating along the string and allowing it to superconduct. The properties of these excitations, or zero modes, dictate how the string interacts with light and can thus have important phenomenological consequences. In this paper, we add a nowhere-vanishing Dirac mass for the fermion in the usual model of axion electrodynamics. We find that the zero modes exhibit an interesting phase structure in which they delocalize from the string's core as the mass increases, up until a critical value past which they disappear. We study this structure from an analytic perspective, with explicit numerical solutions, and via anomaly inflow arguments. Finally, we derive the two-dimensional effective theory of the zero mode and its interactions with the four-dimensional gauge field and show how this effective theory breaks down as the zero modes delocalize.

    hep-thhep-phJHEP(2024)·8 citations
  34. 34*

    Three-body Entanglement in Particle Decays

    Kazuki Sakurai🇵🇱 · Michael Spannowsky🇬🇧

    Quantum entanglement has long served as a foundational pillar in understanding quantum mechanics, with a predominant focus on two-particle systems. We extend the study of entanglement into the realm of three-body decays, offering a more intricate understanding of quantum correlations. We introduce a novel approach for three-particle systems by utilising the principles of entanglement monotone concurrence and the monogamy property. Our findings highlight the potential of studying deviations from the Standard Model and emphasise its significance in particle phenomenology. This work paves the way for new insights into particle physics through multi-particle quantum entanglement, particularly in decays of heavy fermions and hadrons.

    quant-phhep-exhep-phhep-thPRL(2024)·41 citations
  35. 35*

    Complexity in Tame Quantum Theories

    Thomas W. Grimm🇳🇱 · Lorenz Schlechter🇳🇱 · Mick van Vliet🇳🇱

    Inspired by the notion that physical systems can contain only a finite amount of information or complexity, we introduce a framework that allows for quantifying the amount of logical information needed to specify a function or set. We then apply this methodology to a variety of physical systems and derive the complexity of parameter-dependent physical observables and coupling functions appearing in effective Lagrangians. In order to implement these ideas, it is essential to consider physical theories that can be defined in an o-minimal structure. O-minimality, a concept from mathematical logic, encapsulates a tameness principle. It was recently argued that this property is inherent to many known quantum field theories and is linked to the UV completion of the theory. To assign a complexity to each statement in these theories one has to further constrain the allowed o-minimal structures. To exemplify this, we show that many physical systems can be formulated using Pfaffian o-minimal structures, which have a well-established notion of complexity. More generally, we propose adopting sharply o-minimal structures, recently introduced by Binyamini and Novikov, as an overarching framework to measure complexity in quantum theories.

    hep-thhep-phmath.AGmath.LO+1JHEP(2024)·17 citations
  36. 36*

    First constraints on non-minimally coupled Natural and Coleman-Weinberg inflation and massive neutrino self-interactions with Planck+BICEP/Keck

    Nilay Bostan🇺🇸 · Shouvik Roy Choudhury🇹🇼

    In this work, for the first time in literature, we study the predictions of non-minimally coupled Natural and Coleman-Weinberg potentials in the plane, and an extended CDM model where we include non-standard self-interactions among massive neutrinos, mediated by a heavy scalar or vector boson. Constraints were derived using the Planck 2018 + BICEP/Keck 2018 datasets along with other data. For the inflationary potentials, we consider two different formulations in gravity that are non-minimally coupled to the scalar field of the inflaton: \textit{Metric and Palatini.} We only consider the self-interaction to be present among -neutrinos and only at moderate strengths. This is because strong interactions among -neutrinos, or any strength self-interaction among electron- and muon-neutrinos, as well as any strength flavor-universal interactions, are strongly disfavoured from particle physics experiments. In terms of cosmological data, we use the latest public CMB datasets from Planck 2018 and BICEP/Keck 2018 collaborations, along with other data from CMB lensing, BAO, RSD, and SNe Ia luminosity distance measurements. We find that there are some situations where predictions from the inflationary models are ruled out at more than 2 by the minimal CDM model, but they are allowed in the self-interacting neutrino scenario.

    astro-ph.COhep-phJCAP(2024)·21 citations
  37. 37*

    Light Scalars at the Cosmological Collider

    Priyesh Chakraborty🇺🇸 · John Stout🇺🇸

    We study the self-energies of weakly interacting scalar fields in de Sitter space with one field much lighter than the Hubble scale. We argue that self-energies drastically simplify in this light limit. We illustrate this in theories with two scalar fields, one heavy and one light, interacting with one another through either cubic or quartic interactions. To regulate infrared divergences, we compute these self-energies in Euclidean de Sitter space and then carefully analytically continue to Lorentzian signature. In particular, we do this for the most general renormalizable theory of two scalar fields with even interactions to leading order in the coupling and the mass of the light field. These self-energies are determined by de Sitter sunset diagrams, whose analytic structure and UV divergences we derive. Even at very weak couplings, the light field can substantially change how the heavy field propagates over long distances. The light field's existence may then be inferred from how it modifies the heavy field's oscillatory contribution to the primordial bispectrum in the squeezed limit, i.e. its cosmological collider signal.

    hep-thhep-phJHEP(2024)·43 citations
  38. 38*

    The Optimal use of Segmentation for Sampling Calorimeters

    Fernando Torales Acosta🇺🇸 · Bishnu Karki🇺🇸 · Piyush Karande🇺🇸 · Aaron Angerami🇺🇸 · Miguel Arratia🇺🇸 · Kenneth Barish🇺🇸 · Ryan Milton🇺🇸 · Sebastián Morán🇺🇸 · Benjamin Nachman🇺🇸 · Anshuman Sinha🇺🇸

    One of the key design choices of any sampling calorimeter is how fine to make the longitudinal and transverse segmentation. To inform this choice, we study the impact of calorimeter segmentation on energy reconstruction. To ensure that the trends are due entirely to hardware and not to a sub-optimal use of segmentation, we deploy deep neural networks to perform the reconstruction. These networks make use of all available information by representing the calorimeter as a point cloud. To demonstrate our approach, we simulate a detector similar to the forward calorimeter system intended for use in the ePIC detector, which will operate at the upcoming Electron Ion Collider. We find that for the energy estimation of isolated charged pion showers, relatively fine longitudinal segmentation is key to achieving an energy resolution that is better than 10% across the full phase space. These results provide a valuable benchmark for ongoing EIC detector optimizations and may also inform future studies involving high-granularity calorimeters in other experiments at various facilities.

    physics.ins-detcs.LGhep-exhep-ph+1JINST(2024)·8 citations
  39. 39*

    Proposition of FSR Photon Suppression Employing a Two-Positron Decay Dark Matter Model to Explain Positron Anomaly in Cosmic Rays

    Ramin Barak🇷🇺 · Konstantin Belotsky🇷🇺 · Ekaterina Shlepkina🇷🇺

    The origin of an anomalous excess of high-energy (about 100 GeV and higher) positrons in cosmic rays is one of the rare problems in this field, which is proposed to be solved with dark matter (DM). Attempts to solve this problem are faced with the issue of having to satisfy the data on cosmic positrons and cosmic gamma radiation, which inevitably accompanies positron production, such as FSR (final state radiation), simultaneously. We have been trying to come up with a solution by means of two approaches: making assumptions (*) about the spatial distribution of the dark matter and (**) about the physics of its interactions. This work is some small final step of a big investigation regarding the search for gamma suppression by employing the second approach, and a model with a doubly charged particle decaying into two positrons (X++ e+ e+) is suggested as the most prospective one from those considered before.

    astro-ph.HEhep-phUniverse(2023)·3 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.