PaperPanorama

HEP Phenomenology·hep-ph

Thu·Oct 19, 2017

27 papers—17 primary·10 cross-listed·reconstructed*

  1. 01*

    Cosmological Bounds on Non-Abelian Dark Forces

    Lindsay Forestell🇨🇦 · David E. Morrissey🇨🇦 · Kris Sigurdson🇨🇦

    Non-Abelian dark gauge forces that do not couple directly to ordinary matter may be realized in nature. The minimal form of such a dark force is a pure Yang-Mills theory. If the dark sector is reheated in the early universe, it will be realized as a set of dark gluons at high temperatures and as a collection of dark glueballs at lower temperatures, with a cosmological phase transition from one form to the other. Despite being dark, the gauge fields of the new force can connect indirectly to the Standard Model through non-renormalizable operators. These operators will transfer energy between the dark and visible sectors, and they allow some or all of the dark glueballs to decay. In this work we investigate the cosmological evolution and decays of dark glueballs in the presence of connector operators to the Standard Model. Dark glueball decays can modify cosmological and astrophysical observables, and we use these considerations to put very strong limits on the existence of pure non-Abelian dark forces. On the other hand, if one or more of the dark glueballs are stable, we find that they can potentially make up the dark matter of the universe.

    hep-phPRD(2018)·62 citations
  2. 02*

    Next-to-leading order correction to the factorization limit of the radiation spectrum

    M.V. Bondarenco🇺🇦

    A next-to-leading order correction to the high-energy factorization limit of radiation spectrum from an ultrarelativistic electron scattering in an external field is evaluated. Generally, it does not express through scattering characteristics, and accounts for smoothness of the crossover between the initial and final electron asymptotes. A few examples of application of this formula are given, including bremsstrahlung in amorphous matter and undulator radiation.

    hep-phPRD(2017)·4 citations
  3. 03*

    Flavour-symmetric type-II Dirac neutrino seesaw mechanism

    Cesar Bonilla🇪🇸 · J. M. Lamprea🇲🇽 · Eduardo Peinado🇲🇽 · Jose W. F. Valle🇪🇸

    We propose a Standard Model extension with underlying A4 flavour symmetry where small Dirac neutrino masses arise from a Type-II seesaw mechanism. The model predicts the "golden" flavour-dependent bottom-tau mass relation, requires an inverted neutrino mass ordering and non-maximal atmospheric mixing angle. Using the latest neutrino oscillation global fit we derive restrictions on the oscillation parameters, such as a correlation between Dirac CP phase and the lightest neutrino mass.

    hep-phPLB(2018)·48 citations
  4. 04*

    Theoretical Implications of Precision Measurements

    Jens Erler🇲🇽

    Results of an updated global electoweak fit to the Standard Model (SM) are presented, where special attention is paid to some key observables, such as the weak mixing angle, the boson mass, and the anomalous magnetic moment of the muon. Implications for new physics beyond the SM are also discussed.

    hep-phhep-ex2 citations
  5. 05*

    FIMP Dark Matter Freeze-in Gauge Mediation and Hidden Sector

    Kuo-Hsing Tsao🇺🇸

    We explore the dark matter freeze-in mechanism within the gauge mediation framework, which involves a hidden Feebly Interacting Massive Particle (FIMP) coupling feebly with the messenger fields while the messengers are still in the thermal bath. The FIMP is the fermionic component of the pseudo-moduli in a generic metastable supersymmetry (SUSY) breaking model and resides in the hidden sector. The relic abundance and the mass of the FIMP are determined by the SUSY breaking scale and the feeble coupling. The gravitino, which is the canonical dark matter candidate in the gauge mediation framework, contributes to the dark matter relic abundance along with the freeze-in of the FIMP. The hidden sector thus becomes two- component with both the FIMP and gravitino lodging in the SUSY breaking hidden sector. We point out that the ratio between the FIMP and the gravitino is determined by how SUSY breaking is communicated to the messengers. In particular when the FIMP dominates the hidden sector, the gravitino becomes the minor contributor in the hidden sector. Meanwhile, the neutralino is assumed to be both the Weakly Interacting Massive Particle (WIMP) dark matter candidate in the freeze-out mechanism and the Lightest Observable SUSY Particle (LOSP). We further find out the neutralino has the sub-leading contribution to the current dark matter relic density in the parameter space of our freeze-in gauge mediation (FIGM) model. Our result links the SUSY breaking scale in the gauge mediation framework with the FIMP freeze-in production rate leading to a natural and predicting scenario for the studies of the dark matter in the hidden sector.

    hep-phJ.Phys.G(2018)·12 citations
  6. 06*

    Tracks of resonances in electroweak effective Lagrangians

    Ignasi Rosell🇪🇸 · Claudius Krause🇪🇸 · Antonio Pich🇪🇸 · Joaquín Santos🇪🇸 · Juan José Sanz-Cillero🇪🇸

    Taking into account the negative searches for New Physics at the LHC, electroweak effective theories are appropriate to deal with current energies. Tracks of new, higher scales can be studied through next-to leading order corrections of the electroweak effective theory. We assume a generic non-linear realization of the electroweak symmetry breaking with a singlet Higgs and a strongly-coupled UV-completion. We further consider a high-energy Lagrangian that incorporates explicitly a general set of new heavy fields. After integrating out these heavy resonances, we study the pattern of low-energy constants among the light fields, which are generated by the massive states.

    hep-phPoS(2018)·7 citations
  7. 07*

    Quark flavour-violating Higgs decays at the ILC

    Daniele Barducci🇮🇹 · Alexander J. Helmboldt🇩🇪

    Flavour-violating Higgs interactions are suppressed in the Standard Model such that their observation would be a clear sign of new physics. We investigate the prospects for detecting quark flavour-violating Higgs decays in the clean ILC environment. Concentrating on the decay to a bottom and a light quark , we identify the dominant Standard Model background channels as coming from hadronic Standard Model Higgs decays with mis-identified jets. Therefore, good flavour tagging capabilities are essential to keep the background rate under control. Through a simple cut-based analysis, we find that the most promising search channel is the two-jet plus missing energy signature . At 500 GeV, the expected % CL upper limit on is of order . Correspondingly, a discovery is expected to be possible for branching ratios as low as a few .

    hep-phhep-exJHEP(2017)·21 citations
  8. 08*

    Rare radiative charm decays in the standard model and beyond

    Stefan de Boer🇩🇪

    Motivated by the recent measurement of improved standard model (SM) predictions for branching ratios and CP asymmetries of radiative charm decay are given. Weak annihilation induced decays are probes of non-perturbative QCD approaches. Rare decays probe the SM and physics beyond the SM, e.g. leptoquark and supersymmetric models. Opportunities with for future polarization measurements are presented.

    hep-phPoS(2017)·2 citations
  9. 09*

    Resumming double non-global logarithms in the evolution of a jet

    Y. Hatta🇯🇵 · E. Iancu🇫🇷 · A.H. Mueller🇺🇸 · D.N. Triantafyllopoulos🇮🇹

    We consider the Banfi-Marchesini-Smye (BMS) equation which resums non-global energy logarithms in the QCD evolution of the energy lost by a pair of jets via soft radiation at large angles. We identify a new physical regime where, besides the energy logarithms, one has to also resum (anti)collinear logarithms. Such a regime occurs when the jets are highly collimated (boosted) and the relative angles between successive soft gluon emissions are strongly increasing. These anti-collinear emissions can violate the correct time-ordering for time-like cascades and result in large radiative corrections enhanced by double collinear logs, making the BMS evolution unstable beyond leading order. We isolate the first such a correction in a recent calculation of the BMS equation to next-to-leading order by Caron-Huot. To overcome this difficulty, we construct a collinearly-improved version of the leading-order BMS equation which resums the double collinear logarithms to all orders. Our construction is inspired by a recent treatment of the Balitsky-Kovchegov (BK) equation for the high-energy evolution of a space-like wavefunction, where similar time-ordering issues occur. We show that the conformal mapping relating the leading-order BMS and BK equations correctly predicts the physical time-ordering, but it fails to predict the detailed structure of the collinear improvement.

    hep-phJHEP(2018)·19 citations
  10. 10*

    Testing creation of matter with neutrinoless double beta decay

    Stefano Dell'Oro🇮🇹 · Simone Marcocci🇮🇹 · Francesco Vissani🇮🇹

    In this brief review, the importance of the so called neutrinoless double beta decay transition in the search for physics beyond the Standard Model is emphasized. The expectations for the transition rate are examined in the assumption that ordinary neutrinos have Majorana masses. We stress the relevance of cosmological measurements and discuss the uncertainties implied by nuclear physics.

    hep-phPoS(2018)·4 citations
  11. 11*

    Entanglement, fluctuations and discrete symmetries in particle decays

    Wojciech Wislicki🇵🇱

    Pairs of pseudoscalar neutral mesons from decays of vector resonances are studied as bipartite systems in the framework of density operator. Time-dependent quantum entanglement is quantified in terms of the entanglement entropy and these dependences are demonstrated on data on correlated pairs of K and B mesons, as measured by the KLOE and Belle experiments . Another interesting characteristics of such bipartite systems are moments of the CP distributions. These moments are directly measurable and they appear to be very sensitive to the initial degree of entanglement of a pair.

    hep-phhep-exquant-phActa Phys.Polon.B(2017)·0 citations
  12. 12*

    Spin-dependent Conversion on Light Nuclei

    Sacha Davidson🇫🇷 · Yoshitaka Kuno🇯🇵 · Albert Saporta🇫🇷

    The experimental sensitivity to conversion will improve by four or more orders of magnitude in coming years, making it interesting to consider the "spin-dependent" (SD) contribution to the rate. This process does not benefit from the atomic-number-squared enhancement of the spin-independent (SI) contribution, but probes different operators. We give details of our recent estimate of the spin dependent rate, expressed as a function of operator coefficients at the experimental scale, and explore the prospects for distinguishing coefficients by using different targets. For this purpose, a geometric representation of different targets as vectors in coefficient space is introduced. It is found that comparing the rate on isotopes with and without spin could allow to detect spin dependent coefficients that are at least a factor of few larger than the spin independent ones. Distinguishing among the axial, tensor and pseudoscalar operators that induce the SD rate would require calculating the nuclear matrix elements for the second two. Comparing the SD rate on nuclei with an odd proton vs odd neutron could allow to distinguish operators involving quarks from those involving quarks; this is interesting because the distinction is difficult to make for SI operators.

    hep-phEPJC(2018)·57 citations
  13. 14*

    Renormalization group evolution of Higgs effective field theory

    R. Alonso🇨🇭 · K. Kanshin🇮🇹 · S. Saa🇪🇸

    The one-loop renormalization of the action for a set Dirac fermions and a set of scalars spanning an arbitrary manifold coupled via Yukawa-like and gauge interactions is presented. The computation is performed with functional methods and in a geometric formalism that preserves at all stages the symmetries of the action. The result is then applied to Higgs effective field theory to obtain the renormalization group evolution. In the Standard Model limit of this EFT the RGE equations collapse into a smaller linearly independent set; this allows to probe the dynamics of the scalar discovered at LHC via de-correlations in the running of couplings.

    hep-phPRD(2018)·64 citations
  14. 15*

    Convolved Substructure: Analytically Decorrelating Jet Substructure Observables

    Ian Moult🇺🇸 · Benjamin Nachman🇺🇸 · Duff Neill🇺🇸

    A number of recent applications of jet substructure, in particular searches for light new particles, require substructure observables that are decorrelated with the jet mass. In this paper we introduce the Convolved SubStructure (CSS) approach, which uses a theoretical understanding of the observable to decorrelate the complete shape of its distribution. This decorrelation is performed by convolution with a shape function whose parameters and mass dependence are derived analytically. We consider in detail the case of the observable and perform an illustrative case study using a search for a light hadronically decaying . We find that the CSS approach completely decorrelates the observable over a wide range of masses. Our approach highlights the importance of improving the theoretical understanding of jet substructure observables to exploit increasingly subtle features for performance.

    hep-phhep-exJHEP(2018)·66 citations
  15. 16*

    Massless composite bosons formed by the coupled electron-positron pairs, and two-photon angular correlations in the colliding beam reaction with emission of the massless boson

    A.I. Agafonov🇷🇺

    The approach in which the electron and positron are treated as ordinary, different particles, each being characterized by the complete set of the Dirac plane waves, is examined. This completely symmetric representation that is beyond the standard QED, makes it necessary to choose another solution of the Dirac equation for the free particle propagator as compared to that used currently. The Bethe-Salpeter equation with these particle propagators is studied in the ladder approximation. A new branch of the massless composite bosons formed by the coupled electron-positron pairs with the coupling equal to the fine structure constant, has been found. It has been obtained that: 1) the massless bosons have the normalized complex wave functions, which are transversely compressed plane waves; 2) the transverse radius of the wave functions diverges as the boson energy goes to zero that is, the composite bosons cannot be at rest; 3) the extension of the transverse wave function in the momentum space and the compression of the coordinate wave function are continuously occurred with increasing the boson energy. The reaction products of which are the massless composite boson and two photons, is investigated. The cross-section of this reaction is derived for the non-relativistic colliding beams of the spin-polarized electrons and positrons. In this case the angular correlation spectrum is characterized by a narrow peak with the full-width-at-half-maximum not exceeding 0.2 mrad. It is shown that to establish whether there is the conventional annihilation of singlet electron-positron pair with the two-photon emission or the investigated reaction, products of which are the three particles, experiments with the extremely non-relativistic colliding beams should be conducted.

    hep-phAdv.High Energy Phys.(2018)·0 citations
  16. 17*

    The Tensor and the Scalar Charges of the Nucleon from Hadron Phenomenology

    A. Courtoy🇲🇽

    We discuss the impact of the determination of the nucleon tensor charge on searches for physics Beyond the Standard Model. We also comment on the future extraction of the subleading-twist PDF from Jefferson Lab soon-to-be-released Beam Spin Asymmetry data as well as from the expected data of CLAS12, as the latter is related to the scalar charge. These analyses are possible through the phenomenology of Dihadron Fragmentation Functions related processes, which we report on here as well.

    hep-phEPJ Web Conf.(2018)·1 citation
  17. 18*

    Measurement of -weighted TSAs in 2015 COMPASS Drell-Yan data

    Jan Matousek🇨🇿

    In the polarised Drell-Yan experiment at the COMPASS facility at CERN the beam of negatively-charged pions with 190 GeV/c momentum and intensity about pions/s interacted with transversely polarised NH target. Muon pairs produced in Drell-Yan process (DY) were detected. Recently, the first ever Transverse Spin Asymmetries (TSAs) measurement in DY has been presented by COMPASS. A complementary analysis of the TSAs weighted by powers of the dimuon transverse momentum are presented. In the Transverse Momentum Dependent (TMD) PDF formalism, the -weighted TSAs can be written in terms of products of the TMD PDFs of two colliding hadrons, unlike the conventional TSAs, which are their convolutions over quarks transverse momenta. The results are compared in a straightforward way with the weighted Sivers asymmetry in the SIDIS process, released by COMPASS in 2016.

    ↳ hep-exhep-phJ.Phys.Conf.Ser.(2017)·6 citations
  18. 19*

    On the representation (in)dependence of -strings in pure Yang-Mills theory via supersymmetry

    Mohamed M. Anber🇺🇸 · Vito Pellizzani🇨🇭

    We exploit a conjectured continuity between super Yang-Mills on and pure Yang-Mills to study -strings in the latter theory. As expected, we find that Wilson-loop correlation functions depend on the N-ality of a representation to the leading order. However, the next-to-leading order correction is not universal and is given by the group characters, in the representation , of the permutation group. We also study W-bosons in super Yang-Mills and show that they are deconfined on the string worldsheet, and therefore, can change neither the string N-ality nor its tension. This phenomenon mirrors the fact that soft gluons do not screen probe charges with non-zero N-ality in pure Yang-Mills. Finally, we comment on the scaling law of -strings in super Yang-Mills and compare our findings with strings in Seiberg-Witten theory, deformed Yang-Mills theory, and holographic studies that were performed in the 't Hooft large- limit.

    ↳ hep-thhep-lathep-phPRD(2017)·12 citations
  19. 20*

    Leading isospin-breaking corrections to meson masses on the lattice

    D. Giusti🇮🇹 · V. Lubicz🇮🇹 · G. Martinelli🇮🇹 · F. Sanfilippo🇮🇹 · S. Simula🇮🇹 · N. Tantalo🇮🇹 · C. Tarantino🇮🇹

    We present a study of the isospin-breaking (IB) corrections to pseudoscalar (PS) meson masses using the gauge configurations produced by the ETM Collaboration with dynamical quarks at three lattice spacings varying from 0.089 to 0.062 fm. Our method is based on a combined expansion of the path integral in powers of the small parameters and , where is the renormalized quark mass and the renormalized fine structure constant. We obtain results for the pion, kaon and -meson mass splitting; for the Dashen's theorem violation parameters , , ; for the light quark masses , ; for the flavour symmetry breaking parameters and and for the strong IB effects on the kaon decay constants.

    ↳ hep-lathep-phEPJ Web Conf.(2018)·7 citations
  20. 21*

    Exploring the hidden interior of the Earth with directional neutrino measurements

    Michael Leyton🇪🇸 · Stephen Dye🇺🇸 · Jocelyn Monroe🇬🇧

    Roughly 40% of the Earth's total heat flow is powered by radioactive decays in the crust and mantle. Geo-neutrinos produced by these decays provide important clues about the origin, formation and thermal evolution of our planet, as well as the composition of its interior. Previous measurements of geo-neutrinos have all relied on the detection of inverse beta decay reactions, which are insensitive to the contribution from potassium and do not provide model-independent information about the spatial distribution of geo-neutrino sources within the Earth. Here we present a method for measuring previously unresolved components of Earth's radiogenic heating using neutrino-electron elastic scattering and low-background, direction-sensitive tracking detectors. We calculate the exposures needed to probe various contributions to the total geo-neutrino flux, specifically those associated to potassium, the mantle and the core. The measurements proposed here chart a course for pioneering exploration of the veiled inner workings of the Earth.

    ↳ physics.geo-phhep-exhep-phNature Commun.(2017)·30 citations
  21. 22*

    CP-violating top quark couplings at future linear colliders

    W. Bernreuther · L. Chen · I. García · M. Perelló · R. Poeschl F. Richard · E. Ros · M. Vos

    We study the potential of future lepton colliders to probe violation of the CP symmetry in the top quark sector. In certain extensions of the Standard Model, such as the two-Higgs-doublet model (2HDM), sizeable anomalous top quark dipole moments can arise, that may be revealed by a precise measurement of top quark pair production. We present results from detailed Monte Carlo studies for the ILC at 500~\GeV{} and CLIC at 380~\gev{} and use parton-level simulations to explore the potential of high-energy operation. We find that precise measurements in production with subsequent decay to lepton plus jets final states can provide sufficient sensitivity to detect Higgs-boson-induced CP violation in a viable two-Higgs-doublet model. The potential of a linear collider to detect CP-violating electric and weak dipole form factors of the top quark exceeds the prospects of the HL-LHC by over an order of magnitude.

    ↳ hep-exhep-phEPJC(2018)·36 citations
  22. 23*

    CMB bounds on tensor-scalar-scalar inflationary correlations

    Maresuke Shiraishi🇯🇵 · Michele Liguori🇮🇹 · James R. Fergusson🇬🇧

    The nonlinear interaction between one graviton and two scalars is enhanced in specific inflationary models, potentially leading to distinguishable signatures in the bispectrum of the cosmic microwave background (CMB) anisotropies. We develop the tools to examine such bispectrum signatures, and show a first application using WMAP temperature data. We consider several -ranges, estimating the amplitude parameter, by means of the so-called separable modal methodology. We do not find any evidence of a tensor-scalar-scalar signal at any scale. Our tightest bound on the size of the tensor-scalar-scalar correlator is derived from our measurement including all the multipoles in the range and it reads (CL). This is the first direct observational constraint on the primordial tensor-scalar-scalar correlation, and it will be cross-checked and improved by applying the same pipeline to high-resolution temperature and polarization data from and forthcoming CMB experiments.

    ↳ astro-ph.COgr-qchep-phhep-thJCAP(2018)·17 citations
  23. 24*

    Observational signatures of the parametric amplification of gravitational waves during reheating after inflation

    Sachiko Kuroyanagi🇯🇵 · Chunshan Lin🇵🇱 · Misao Sasaki🇯🇵 · Shinji Tsujikawa🇯🇵

    We study the evolution of Gravitational Waves (GWs) during and after inflation as well as the resulting observational consequences in a Lorentz-violating massive gravity theory with one scalar (inflaton) and two tensor degrees of freedom. We consider two explicit examples of the tensor mass that depends either on the inflaton field or on its time derivative , both of which lead to parametric excitations of GWs during reheating after inflation. The first example is Starobinsky's inflation model with a -dependent and the second is a low-energy-scale inflation model with a -dependent . We compute the energy density spectrum today of the GW background. In the Starobinsky's model, we show that the GWs can be amplified up to the detectable ranges of both CMB and DECIGO, but the bound from the big bang nucleosynthesis is quite tight to limit the growth. In low-scale inflation with a fast transition to the reheating stage driven by the potential around (where is the reduced Planck mass), we find that the peak position of induced by the parametric resonance can reach the sensitivity region of advanced LIGO for the Hubble parameter of order 1 GeV at the end of inflation. Thus, our massive gravity scenario offers exciting possibilities for probing the physics of primordial GWs at various different frequencies.

    ↳ gr-qcastro-ph.COhep-phhep-thPRD(2018)·25 citations
  24. 25*

    Fermionic Light Dark Matter particles and the New Physics of Neutron Stars

    M. Cermeño🇪🇸 · M. Ángeles Pérez-García🇪🇸 · Joseph Silk🇫🇷

    Dark Matter constitutes most of the matter in the presently accepted cosmological model for our Universe. The extreme conditions of ordinary baryonic matter, namely high density and compactness, in Neutron Stars make these objects suitable to gravitationally accrete such a massive component provided interaction strength between both, luminous and dark sectors, at current experimental level of sensitivity. We consider several different DM phenomenological models from the myriad of those presently allowed. In this contribution we review astrophysical aspects of interest in the interplay of ordinary matter and a fermionic light Dark Matter component. We focus in the interior nuclear medium in the core and external layers, i.e. the crust, discussing the impact of a novel dark sector in relevant stellar quantities for (heat) energy transport such as thermal conductivity or emissivities.

    ↳ astro-ph.HEhep-phnucl-thPubl.Astron.Soc.Austral.(2017)·21 citations
  25. 26*

    Nuclear medium effects in muonic neutrino interaction with energies from 0.2 GeV to 1.5 GeV

    D. Vargas🇧🇷 · A.R. Samana🇧🇷 · F.G. Velasco🇲🇽 · O.R. Hoyos🇧🇷 · F. Guzmán🇧🇷 · J.L. Bernal-Castillo🇧🇷 · E. Andrade-II🇧🇷 · R. Perez🇧🇷 · A. Deppman🇧🇷 · C.A. Barbero🇦🇷 · A.E. Mariano🇦🇷

    Nuclear reactions induced by muon neutrino with energies in the range from 0.2 to 1.5 GeV in Monte Carlo calculations framework in the intra-nuclear cascade model are studied. This study was done by comparison between the available experimental data and theoretical values of total cross section, and the energy distribution of emitted lepton energy in the reaction muon neutrino-nucleus, using the targets: C, O, Al, Ar, Fe and Pb. A phenomenological toy model of primary neutrino-nucleon interaction gives a good agreement of our theoretical inclusive neutrino nucleus cross in comparison with the available experimental data. Some interesting results on the behavior of the cross section as function of 1p-1n and higher contributions are also sketched. The previous results on the percentage of fake events related in available experiments in C were expanded for the set studied nuclei. With the increase of mass target, the nuclear effects in the cross sections were observed along with the importance to take into account fake events in the reactions.

    ↳ nucl-thhep-phPRC(2017)·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.