PaperPanorama

HEP Phenomenology·hep-ph

Mon·Jun 12, 2017

23 papers—14 primary·9 cross-listed·reconstructed*

  1. 01*

    Dark Matter and Neutrino Mass from the Smallest Non-Abelian Chiral Dark Sector

    Jeffrey M. Berryman🇺🇸 · André de Gouvêa🇺🇸 · Kevin J. Kelly🇺🇸 · Yue Zhang🇺🇸

    All pieces of concrete evidence for phenomena outside the standard model (SM) - neutrino masses and dark matter - are consistent with the existence of new degrees of freedom that interact very weakly, if at all, with those in the SM. We propose that these new degrees of freedom organize themselves into a simple dark sector, a chiral SU(3) x SU(2) gauge theory with the smallest nontrivial fermion content. Similar to the SM, the dark SU(2) is spontaneously broken while the dark SU(3) confines at low energies. At the renormalizable level, the dark sector contains massless fermions - dark leptons - and stable massive particles - dark protons. We find that dark protons with masses between 10-100 TeV satisfy all current cosmological and astrophysical observations concerning dark matter even if dark protons are a symmetric thermal relic. The dark leptons play the role of right-handed neutrinos and allow simple realizations of the seesaw mechanism or the possibility that neutrinos are Dirac fermions. In the latter case, neutrino masses are also parametrically different from charged-fermion masses and the lightest neutrino is predicted to be massless. Since the new "neutrino" and "dark matter" degrees of freedom interact with one another, these two new-physics phenomena are intertwined. Dark leptons play a nontrivial role in early universe cosmology while indirect searches for dark matter involve, decisively, dark matter annihilations into dark leptons. These, in turn, may lead to observable signatures at high-energy neutrino and gamma-ray observatories, especially once one accounts for the potential Sommerfeld enhancement of the annihilation cross-section, derived from the low-energy dark-sector effective theory, a possibility we explore quantitatively in some detail.

    hep-phPRD(2017)·56 citations
  2. 02*

    Mass Formula for Light Nonstrange Mesons and Regge Trajectories in Quark Model

    Duojie Jia🇨🇳 · Cheng-Qun Pang🇨🇳 · Atsushi Hosaka🇯🇵

    We study the Regge-like spectra of light mesons in a relativized quark model. An analytical mass formula is presented for the light unflavored mesons with the help of auxiliary field method, by which a quasi-linear Regge-Chew-Frautschi plot is predicted for the orbitally excited states. We show that the trajectory slope is proportional to the inverse confining parameter up to a factor depending on the strong coupling when the orbital quantum number is large. The result is tested against the experimental data of the spectra of the meson families ,, and in the (,) planes, with the fitted parameters consistent with that in the literatures.

    hep-phInt.J.Mod.Phys.A(2017)·13 citations
  3. 03*

    Compressed Stop Searches with Two Leptons and Two b-jets

    Hsin-Chia Cheng🇺🇸 · Christina Gao🇺🇸 · Lingfeng Li🇺🇸

    In top squark (stop) searches with a compressed spectrum, it is very helpful to consider the stop production recoiling against a hard jet from the initial state radiation to obtain a significant amount of missing transverse energy. In particular, the kinematic variable which measures the ratio of the lightest neutralino mass and the stop mass proved to be crucial in separating the signals from the backgrounds in both the all-hadronic decay and the semileptonic decay of the stops. Here we generalize the search method to the dileptonic stop decays. In this case, due to the two missing neutrinos, there are not enough kinematic constraint equations to solve for the variable exactly, but only render an allowed interval consistent with the event. However, we show that the minimum and the maximum values of this allowed interval still provide useful variables in discriminating signals from the backgrounds. Although in the traditional stop decay to a top quark and the lightest neutralino, the dileptonic mode is not as competitive due to its small branching ratio, it becomes the main search mode if the stops decay through the charginos and sleptons with a compressed spectrum. We show that with the new variables, the dileptonic search of the stop can cover regions of the parameter space which have not been constrained before.

    hep-phhep-exJ.Phys.G(2019)·5 citations
  4. 04*

    Top partner production at collider in the littlest Higgs Model with T-parity

    Haiyan Wang🇨🇳 · Bingfang Yang🇨🇳

    In the framework of the littlest Higgs Model with T-parity, we discuss the top partner production at future collider. We calculate the cross sections of the top partner production processes and associated production processes of Higgs and top partner under current constraints. Then, we investigate the observability of the T-odd top partner pair production through the process in the di-lepton channel for two T-odd top partner mass =603(708) GeV at =1.5 TeV. We analyze the signal significance depending on the integrated luminosity and find this signal is promising at the future high energy collider.

    hep-phAdv.High Energy Phys.(2017)·7 citations
  5. 05*

    Color entanglement effect in collinear twist-3 factorization

    Jian Zhou🇨🇳

    We study color entanglement effect for T-odd cases in collinear twist-3 factorization. As an example, we compute the transverse single spin asymmetry for direct photon production in pp collisions in pure collinear twist-3 approach. By analyzing the gauge link structure of the collinear gluon distribution on unpolarized target side, we demonstrate how color entanglement effect arises in the presence of the additional gluon attachment from polarized projectile. The result is consistent with that obtained from a hybrid approach calculation.

    hep-phPRD(2017)·5 citations
  6. 06*

    Baryon asymmetry generation in the E6CHM

    R. Nevzorov🇦🇺 · A. W. Thomas🇦🇺

    In the E6 inspired composite Higgs model (E6CHM) the strongly interacting sector possesses an SU(6) global symmetry which is expected to be broken down to its SU(5) subgroup at the scale f > 10 TeV. This breakdown results in a set of pseudo-Nambu-Goldstone bosons (pNGBs) that includes one Standard Model (SM) singlet scalar, a SM-like Higgs doublet and an SU(3)_C triplet of scalar fields, T. In the E6CHM the Z^L_{2} symmetry, which is a discrete subgroup of the U(1)_L associated with lepton number conservation, can be used to forbid operators which lead to rapid proton decay. The remaining baryon number violating operators are sufficiently strongly suppressed because of the large value of the scale f. We argue that in this variant of the E6CHM a sizeable baryon number asymmetry can be induced if CP is violated. At the same time, the presence of the SU(3)_C scalar triplet with mass in the few TeV range may give rise to spectacular new physics signals that may be detected at the LHC in the near future.

    hep-phPLB(2017)·9 citations
  7. 07*

    Vector Boson Fusion versus Gluon Fusion

    Chen-Hsun Chan🇹🇼 · Kingman Cheung🇹🇼 · Yi-Lun Chung🇹🇼 · Pai-Hsien Hsu🇹🇼

    Vector-boson fusion (VBF) is a clean probe of the electroweak-symmetry breaking (EWSB), which inevitably suffers from some level of contamination due to the gluon fusion (ggF). In addition to the jet variables used in the current experimental analysis, we analyze a few more jet-shape variables defined by the girth and integrated jet-shape. Taking and as examples, we perform the analysis with a new technique of 2-step boosted-decision-tree method, which significantly reduces the contamination of the ggF in the VBF sample, thus, providing a clean environment in probing the EWSB sector.

    hep-phhep-exPRD(2017)·6 citations
  8. 08*

    Waves in magnetized quark matter

    D. A. Fogaça🇧🇷 · S. M. Sanches Jr.🇧🇷 · F. S. Navarra🇧🇷

    We study wave propagation in a non-relativistic cold quark-gluon plasma immersed in a constant magnetic field. Starting from the Euler equation we derive linear wave equations and investigate their stability and causality. We use a generic form for the equation of state, the EOS derived from the MIT bag model and also a variant of the this model which includes gluon degrees of freedom. The results of this analysis may be relevant for perturbations propagating through the quark matter phase in the core of compact stars and also for perturbations propagating in the low temperature quark-gluon plasma formed in low energy heavy ion collisions, to be carried out at FAIR and NICA.

    hep-phhep-thnucl-thNPA(2018)·7 citations
  9. 09*

    A No-Go Theorem for Fully SGUTs with Metastable SUSY Breaking

    Jean-François Fortin🇨🇦 · Jean-Samuel Leboeuf🇨🇦

    We introduce fully SGUTs, SUSY grand unified theories that, upon symmetry breaking through the Higgs mechanism, decompose into a visible sector and an extra sector where the dynamics of the extra sector gauge group is responsible for SUSY breaking. Fully SGUTs thus have the important feature that all gauge groups of the visible sector and the extra sector unify into a simple gauge group at the SGUT scale, therefore generalizing the successful MSSM gauge coupling unification to all the gauge couplings of the theory. By focusing on the ISS SUSY-breaking mechanism in the extra sector, we show that it is impossible to reproduce the MSSM matter content when there exists a metastable ISS SUSY-breaking state.

    hep-phPRD(2017)·0 citations
  10. 10*

    Precision Probes of QCD at High Energies

    Simone Alioli🇨🇭 · Marco Farina🇺🇸 · Duccio Pappadopulo🇺🇸 · Joshua T. Ruderman🇺🇸

    New physics, that is too heavy to be produced directly, can leave measurable imprints on the tails of kinematic distributions at the LHC. We use energetic QCD processes to perform novel measurements of the Standard Model (SM) Effective Field Theory. We show that the dijet invariant mass spectrum, and the inclusive jet transverse momentum spectrum, are sensitive to a dimension 6 operator that modifies the gluon propagator at high energies. The dominant effect is constructive or destructive interference with SM jet production. We compare differential next-to-leading order predictions from POWHEG to public 7 TeV jet data, including scale, PDF, and experimental uncertainties and their respective correlations. We constrain a New Physics (NP) scale of 3.5 TeV with current data. We project the reach of future 13 and 100 TeV measurements, which we estimate to be sensitive to NP scales of 8 and 60 TeV, respectively. As an application, we apply our bounds to constrain heavy vector octet colorons that couple to the QCD current. We project that effective operators will surpass bump hunts, in terms of coloron mass reach, even for sequential couplings.

    hep-phhep-exJHEP(2017)·66 citations
  11. 11*

    The Other Fermion Compositeness

    Brando Bellazzini🇫🇷 · Francesco Riva🇨🇭 · Javi Serra🇨🇭 · Francesco Sgarlata🇮🇹

    We discuss the only two viable realizations of fermion compositeness described by a calculable relativistic effective field theory consistent with unitarity, crossing symmetry and analyticity: chiral-compositeness vs goldstino-compositeness. We construct the effective theory of Goldstini and show how the Standard Model can emerge from this dynamics. We present new bounds on either type of compositeness, for quarks and leptons, using dilepton searches at LEP, dijets at the LHC, as well as low-energy observables and precision measurements. Remarkably, a scale of compositeness for Goldstino-like electrons in the 2 TeV range is compatible with present data, and so are Goldstino-like first generation quarks with a compositeness scale in the 10 TeV range. Moreover, assuming maximal -symmetry, goldstino-compositeness of both right- and left-handed quarks predicts exotic spin-1/2 colored sextet particles that are potentially within the reach of the LHC.

    hep-phhep-thJHEP(2017)·57 citations
  12. 12*

    Dynamics of Relaxed Inflation

    Walter Tangarife🇮🇱 · Kohsaku Tobioka🇮🇱 · Lorenzo Ubaldi🇮🇱 · Tomer Volansky🇮🇱

    The cosmological relaxation of the electroweak scale has been proposed as a mechanism to address the hierarchy problem of the Standard Model. A field, the relaxion, rolls down its potential and, in doing so, scans the squared mass parameter of the Higgs, relaxing it to a parametrically small value. In this work, we promote the relaxion to an inflaton. We couple it to Abelian gauge bosons, thereby introducing the necessary dissipation mechanism which slows down the field in the last stages. We describe a novel reheating mechanism, which relies on the gauge-boson production leading to strong electromagnetic fields, and proceeds via the vacuum production of electron-positron pairs through the Schwinger effect. We refer to this mechanism as Schwinger reheating. We discuss the cosmological dynamics of the model and the phenomenological constraints from CMB and other experiments. We find that a cutoff close to the Planck scale may be achieved. In its minimal form, the model does not generate sufficient curvature perturbations and additional ingredients, such as a curvaton field, are needed.

    hep-phastro-ph.COhep-thJHEP(2018)·63 citations
  13. 13*

    Constraints from Triple Gauge Couplings on Vectorlike Leptons

    Enrico Bertuzzo🇧🇷 · Pedro A. N. Machado🇺🇸 · Yuber F. Perez-Gonzalez🇧🇷 · Renata Zukanovich Funchal🇧🇷

    We study the contributions of colorless vectorlike fermions to the triple gauge couplings and . We consider models in which their coupling to the Standard Model Higgs boson is allowed or forbidden by quantum numbers. We assess the sensitivity of the future accelerators FCC-ee, ILC and CLIC to the parameters of these models, assuming they will be able to constrain the anomalous triple gauge couplings with a precision , . We show that the combination of measurements at different center-of-mass energies helps to improve the sensitivity to the contribution of vectorlike fermions, in particular when they couple to the Higgs. In fact, the measurements at the FCC-ee and, especially, the ILC and the CLIC, may turn the triple gauge couplings into a new set of precision parameters able to constrain the models better than the oblique parameters or the decay, even assuming the considerable improvement of the latter measurements achievable at the new machines.

    hep-phPRD(2017)·5 citations
  14. 14*

    Probing the electromagnetic dipole moments of the tau-neutrino in the model at the ILC and CLIC energies

    A. Llamas-Bugarin🇲🇽 · A. Gutiérrez-Rodríguez🇲🇽 · M. A. Hernández-Ruíz🇲🇽

    In this work we study the sensitivity on the anomalous magnetic and electric dipole moments of the tau-neutrino in the framework of the electroweak model at future linear colliders as the ILC and CLIC. For our study we consider the process . For center-of-mass energies of and integrated luminosities of , we derive C.L. limits on the dipole moments and improve the existing limits by two or three orders of magnitude. Our study complements other studies on the dipole moments of the tau-neutrino at hadron and colliders.

    hep-phPRD(2017)·8 citations
  15. 15*

    Deep-Learning the Landscape

    Yang-Hui He🇬🇧

    We propose a paradigm to deep-learn the ever-expanding databases which have emerged in mathematical physics and particle phenomenology, as diverse as the statistics of string vacua or combinatorial and algebraic geometry. As concrete examples, we establish multi-layer neural networks as both classifiers and predictors and train them with a host of available data ranging from Calabi-Yau manifolds and vector bundles, to quiver representations for gauge theories. We find that even a relatively simple neural network can learn many significant quantities to astounding accuracy in a matter of minutes and can also predict hithertofore unencountered results. This paradigm should prove a valuable tool in various investigations in landscapes in physics as well as pure mathematics.

    ↳ hep-thhep-phmath.AGstat.ML127 citations
  16. 16*

    On the Chiral Ring and Vacua of Adjoint SQCD

    Ke Ye🇺🇸

    We analyze classical and quantum chiral ring relations of four dimensional adjoint SQCD with superpotential turned on for the adjoint field. In particular, for the mass deformed theory we obtain the complete on shell vacuum expectation value for various gauge invariant chiral operators and find non-trivial gaugino condensations. When approaching to massless limit nontrivial flat directions in the moduli space of vacua appear, where the Coulomb branch can be naturally classified and the Higgs branch receives quantum corrections. We argue that the solution of the chiral ring is in one-to-one correspondence with supersymmetric vacua, provided that an additional Konishi anomaly equation is included.

    ↳ hep-thhep-phmath.QA1 citation
  17. 17*

    The extra scalar degrees of freedom from the two Higgs doublet model for dark energy

    Muhammad Usman🇵🇰 · Asghar Qadir🇵🇰

    In principle a minimal extension of the standard model of Particle Physics, the two Higgs doublet model, can be invoked to explain the scalar field responsible of dark energy. The two doublets are in general mixed. After diagonalization, the lightest CP-even Higgs and CP-odd Higgs are jointly taken to be the dark energy candidate. The dark energy obtained from Higgs fields in this case is indistinguishable from the cosmological constant.

    ↳ physics.gen-phhep-phInt.J.Mod.Phys.D(2017)·2 citations
  18. 18*

    Schwinger Pair Production by Electric Field Coupled to Inflaton

    Jia-Jia Geng🇨🇳 · Bao-Fei Li🇨🇳 · Jiro Soda🇯🇵 · Anzhong Wang🇺🇸 · Qiang Wu🇨🇳 · Tao Zhu🇨🇳

    We analytically investigate the Schwinger pair production in the de Sitter background by using {\em the uniform asymptotic approximation method}, and show that the equation of motion in general has two turning points, and the nature of these points could be single, double, real or complex, depending on the choice of the free parameters involved in the theory. Different natures of these points lead to different electric currents. In particular, when is positive, both turning points are complex, and the electric current due to the Schwinger process is highly suppressed, where and denote, respectively, the mass of the particle and the Hubble parameter. For the turning points to be real, it is necessary to have , and the more negative of , the easier to produce particles. In addition, when , we also study the particle production when the electric field is very weak. We find that the electric current in this case is proportional to , which is strongly enhanced in the weak electric field limit when .

    ↳ gr-qcastro-ph.COhep-phhep-thJCAP(2018)·34 citations
  19. 19*

    Spatially Modulated Vacua in a Lorentz-invariant Scalar Field Theory

    Muneto Nitta🇯🇵 · Shin Sasaki🇯🇵 · Ryo Yokokura🇯🇵

    Spatial modulation has been studied for a long time in condensed matter, nuclear matter and quark matter, so far in non-relativistic field theories. In this paper, spatially modulated vacua at zero temperature and zero density are studied in relativistic field theories. We first propose an adaptation of the Nambu-Goldstone theorem to higher derivative theories under the assumption of the absence of ghosts: when a global symmetry is spontaneously broken due to vacuum expectation values of space-time derivatives of fields, a Nambu-Goldstone (NG) boson appears without a canonical kinetic (quadratic derivative) term with a quartic derivative term in the modulated direction while a Higgs boson appears with a canonical kinetic term. We demonstrate this in a simple model allowing (meta)stable modulated vacuum of a phase modulation (Fulde-Ferrell state), where an NG mode associated with spontaneously broken translational and symmetries appears.

    ↳ hep-thhep-phEPJC(2018)·24 citations
  20. 20*

    The nucleon spin and momentum decomposition using lattice QCD simulations

    C. Alexandrou (Univ. of Cyprus & Cyprus Inst.)🇨🇾 · M. Constantinou (Temple Univ.)🇺🇸 · K. Hadjiyiannakou (Cyprus Inst.)🇨🇾 · K. Jansen (DESY-Zeuthen)🇩🇪 · C. Kallidonis (Cyprus Inst.)🇨🇾 · G. Koutsou (Cyprus Inst.)🇨🇾 · A. Vaquero Avilés-Casco (Univ. of Utah)🇺🇸 · C. Wiese (DESY-Zeuthen)🇩🇪

    We determine within lattice QCD, the nucleon spin carried by valence and sea quarks, and gluons. The calculation is performed using an ensemble of gauge configurations with two degenerate light quarks with mass fixed to approximately reproduce the physical pion mass. We find that the total angular momentum carried by the quarks in the nucleon is and the gluon contribution is giving a total of consistent with the spin sum. For the quark intrinsic spin contribution we obtain . All quantities are given in the scheme at 2~GeV. The quark and gluon momentum fractions are also computed and add up to satisfying the momentum sum.

    ↳ hep-lathep-exhep-phnucl-ex+1PRL(2017)·174 citations
  21. 21*

    Scalar and vector form factors of decays with twisted fermions

    V. Lubicz🇮🇹 · L. Riggio🇮🇹 · G. Salerno🇮🇹 · S. Simula🇮🇹 · C. Tarantino🇮🇹

    We present a lattice determination of the vector and scalar form factors of the semileptonic decays, which are relevant for the extraction of the CKM matrix elements and from experimental data. Our analysis is based on the gauge configurations produced by the European Twisted Mass Collaboration with flavors of dynamical quarks, at three different values of the lattice spacing and with pion masses as small as 210 MeV. The matrix elements of both vector and scalar currents are determined for a plenty of kinematical conditions in which parent and child mesons are either moving or at rest. Lorentz symmetry breaking due to hypercubic effects is clearly observed in the data and included in the decomposition of the current matrix elements in terms of additional form factors. After the extrapolations to the physical pion mass and to the continuum limit we determine the vector and scalar form factors in the whole kinematical region from up to accessible in the experiments, obtaining a good overall agreement with experiments, except in the region at high values of where some deviations are visible. A set of synthetic data points, representing our results for and for several selected values of , is provided and also the corresponding covariance matrix is available. At zero 4-momentum transfer we get: and . Using the experimental averages for and , we extract and , respectively. The second-row of the CKM matrix is found to be in agreement with unitarity within the current uncertainties: .

    ↳ hep-lathep-exhep-phPRD(2017)·150 citations
  22. 22*

    Limits on Brane-World and Particle Dark Radiation from Big Bang Nucleosynthesis and the CMB

    Nishanth Sasankan🇺🇸 · Mayukh. R. Gangopadhyay🇺🇸 · Grant. J. Mathews🇺🇸 · Motohiko Kusakabe🇺🇸

    The term dark radiation is used both to describe a noninteracting neutrino species and as a correction to the Friedmann Equation in the simplest five-dimensional RS-II brane-world cosmology. In this paper we consider the constraints on both meanings of dark radiation based upon the newest results for light-element nuclear reaction rates, observed light-element abundances and the power spectrum of the Cosmic Microwave Background (CMB). Adding dark radiation during big bang nucleosynthesis (BBN) alters the Friedmann expansion rate causing the nuclear reactions to freeze out at a different temperature. This changes the final light element abundances at the end of BBN. Its influence on the CMB is to change the effective expansion rate at the surface of last scattering. We find that the BBN constraint reduces the allowed range for both types of dark radiation at 10 Mev to between and of the {\bf total} background energy density at 10 Mev. Combining this result with fits to the CMB power spectrum, produces different results for particle vs. brane-world dark radiation. In the brane-world, the range decreases to to . Thus, we find, that the ratio of dark radiation to the background total relativistic mass energy density is consistent with zero although there remains a very slight preference for a positive (rather than negative) contribution.

    ↳ astro-ph.COhep-phIJMPE(2017)·18 citations
  23. 23*

    Description of Charged Particle Pseudorapidity Distributions in Pb+Pb Collisions with Tsallis Thermodynamics

    Y. Gao🇨🇳 · H. Zheng🇮🇹 · L.L. Zhu🇨🇳 · A. Bonasera🇺🇸

    The centrality dependence of pseudorapidity distributions for charged particles produced in Au+Au collisions at GeV and 200 GeV at RHIC, and in Pb+Pb collisions at TeV at LHC are investigated in the fireball model, assuming that the rapidity axis is populated with fireballs following one distribution function. We assume that the particles in the fireball fulfill the Tsallis distribution. The theoretical results are compared with the experimental measurements and a good agreement is found. Using these results, the pseudorapidity distributions of charged particles produced in Pb+Pb central collisions at TeV and 10 TeV are predicted.

    ↳ nucl-thhep-phEPJA(2017)·14 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.