PaperPanorama

HEP Phenomenology·hep-ph

Wed·Sep 23, 2015

25 papers17 primary·8 cross-listed·reconstructed*

  1. 01*

    Hadron Collider Tests of Neutrino Mass-Generating Mechanisms

    Richard E. Ruiz🇺🇸

    The Standard Model of particle physics (SM) is presently the best description of nature at small distances and high energies. However, with tiny but nonzero neutrino masses, a Higgs boson mass unstable under radiative corrections, and little guidance on understanding the hierarchy of fermion masses, the SM remains an unsatisfactory description of nature. Well-motivated scenarios that resolve these issues exist but also predict extended gauge (e.g., Left-Right Symmetric Models), scalar (e.g., Supersymmetry), and/or fermion sectors (e.g., Seesaw Models). Hence, discovering such new states would have far-reaching implications. After reviewing basic tenets of the SM and collider physics, several beyond the SM (BSM) scenarios that alleviate these shortcomings are investigated. Emphasis is placed on the production of a heavy Majorana neutrinos at hadron colliders in the context of low-energy, effective theories that simultaneously explain the origin of neutrino masses and their smallness compared to other elementary fermions, the so-called Seesaw Mechanisms. As probes of new physics, rare top quark decays to Higgs bosons in the context of the SM, the Types I and II Two Higgs Doublet Model (2HDM), and the semi-model independent framework of Effective Field Theory (EFT) have also been investigated. Observation prospects and discovery potentials of these models at current and future collider experiments are quantified.

    hep-phhep-ex15 citations
  2. 02*

    Vector boson scattering at the LHC. A study of the WW -> WW channels with the Warsaw cut

    Marco Fabbrichesi🇮🇹 · Michele Pinamonti🇮🇹 · Alberto Tonero🇧🇷 · Alfredo Urbano🇮🇹

    We study W boson scattering in the same- and opposite-sign channels under the assumption that no resonances are present in the collider processes and , respectively. Basic selection cuts together with a restriction on the combination of the final lepton and jet momenta (the Warsaw cut) makes it possible to argue that at the LHC a luminosity of 100 fb and a center-of-mass energy of TeV will allow to constrain the leading effective lagrangian coefficients at the permil level. We also discuss limits on the other coefficients of the effective lagrangian as well as stronger constraints provided by higher energy and luminosity. We show that the same-sign channel suffices in providing the most stringent constraints.

    hep-phhep-exPRD(2016)·32 citations
  3. 03*

    The Transverse Momentum Dependent Fragmentation Function at NNLO

    Miguel G. Echevarria🇳🇱 · Ignazio Scimemi🇪🇸 · Alexey Vladimirov🇩🇪

    We calculate the unpolarized transverse momentum dependent fragmentation function (TMDFF) at next-to-next-to-leading order (NNLO), evaluating separately TMD soft factor and TMD collinear correlator. For the first time the cancellation of spurious rapidity divergences in a properly defined individual TMD beyond the first non-trivial order is shown. This represents a strong check of the given TMD definition. We extract the matching coefficient necessary to perform the transverse momentum resummation at next-to-next-to-next-to-leading-logarithmic accuracy. The universal character of the soft function, which enters the definition of all (un)polarized TMD distribution/fragmentation functions, facilitates the future calculation of all the other TMDs and their coefficients at NNLO, pushing forward the accuracy of theoretical predictions for the current and next generation of high energy colliders.

    hep-phPRD(2016)·84 citations
  4. 04*

    Limits on the anomalous couplings

    R. Romero Aguilar🇲🇽 · Antonio O. Bouzas🇲🇽 · F. Larios🇲🇽

    Within the model-independent framework of gauge-invariant dimension-six operators, we study flavor-changing couplings () and related four-quark contact interactions involving the top. We obtain bounds on those couplings from Tevatron and LHC data for single-top production and branching fractions in top decays, as well as other experimental results on flavor-changing neutral-current processes including and decays (). We also update the bounds on flavor-diagonal couplings using the most recent measurement of -helicity fractions in top decays from top-pair production.

    hep-phPRD(2015)·13 citations
  5. 05*

    Analysis of the pentaquark states in the diquark-diquark-antiquark model with QCD sum rules

    Zhi-Gang Wang🇨🇳

    In this article, we construct both the axialvector-diquark-axialvector-diquark-antiquark type and axialvector-diquark-scalar-diquark-antiquark type interpolating currents, then calculate the contributions of the vacuum condensates up to dimension-10 in the operator product expansion, and study the masses and pole residues of the hidden-charm pentaquark states with the QCD sum rules in a systematic way. In calculations, we use the formula to determine the energy scales of the QCD spectral densities. We take into account the breaking effects of the light quarks, and obtain the masses of the hidden charm pentaquark states with the strangeness , which can be confronted with the experimental data in the future.

    hep-phEPJC(2016)·81 citations
  6. 06*

    Non-Hermitian neutrino oscillations in matter with PT symmetric Hamiltonians

    Tommy Ohlsson🇸🇪

    We introduce and develop a novel approach to extend the ordinary two-flavor neutrino oscillation formalism in matter using a non-Hermitian PT symmetric effective Hamiltonian. The condition of PT symmetry is weaker and less mathematical than that of hermicity, but more physical, and such an extension of the formalism can give rise to sub-leading effects in neutrino flavor transitions similar to the effects by so-called non-standard neutrino interactions. We derive the necessary conditions for the spectrum of the effective Hamiltonian to be real as well as the mappings between the fundamental and effective parameters. We find that the real spectrum of the effective Hamiltonian will depend on all new fundamental parameters introduced in the non-Hermitian PT symmetric extension of the usual neutrino oscillation formalism and that either i) the spectrum is exact and the effective leptonic mixing must always be maximal or ii) the spectrum is approximate and all new fundamental parameters must be small.

    hep-phEPL(2016)·37 citations
  7. 07*

    Hidden Ward-Takahashi identities in the spontaneously brokenAbelian Higgs model and the decoupling of certain heavy particles in its simple extensions

    Bryan W. Lynn🇺🇸 · Glenn D. Starkman🇺🇸

    This work is dedicated to the memory of R. Stora. The spontaneously broken (SSB) Abelian Higgs model (AHM) (the gauge theory of a scalar and a transverse vector A) has a massless pseudo-scalar in Lorenz gauge. Physical states have a conserved global current and Goldstone theorem (GT). becomes a Nambu-Goldstone boson (NGB). Slavnov-Taylor identities keep on-shell T-matrix elements of physical states independent of anomaly-free gauge, and global, transformations, yielding towers of -sector Ward-Takahashi Identities (WTI), and constraining external dynamics. Ultraviolet quadratic divergences (UVQD) contribute only to , forced by the GT to 0, so all UVQD vanish. Weak-scale renormalized gauge-independent Higgs pole-mass and VEV are therefore not fine-tuned. The NGB is "eaten" and decouples, hiding the WTI from observable particle physics. Our regularization-scheme-independent results are unchanged by the addition of certain heavy fields as the extended WTI and GT cause all relevant operators to vanish. We prove 5 SSB decoupling theorems, illustrating them with two examples: a heavy -symmetric singlet real scalar field with 0 VEV; and a heavy singlet right-handed type 1 see-saw Majorana neutrino. Including all loops we prove that certain heavy degrees of freedom decouple from the low-energy effective Lagrangian, contributing only irrelevant operators after renormalization. The cannot completely decouple, but becomes invisible in practice. The NGB decouples, but our hidden SSB WTI, and a shift symmetry, protect the low-energy SSB AHM physics from loop contributions of heavy particles! Gauge-independent observable weak-scale and are Goldstone Exceptionally Natural, not fine-tuned.

    hep-ph3 citations
  8. 08*

    Search for associated production of Higgs with Z boson in the noncommutative Standard Model at linear colliders

    Selvaganapathy J.🇮🇳 · Prasanta Kumar Das🇮🇳 · Partha Konar🇮🇳

    We study the associated Higgs production with Z boson at future linear colliders in the framework of the minimal noncommutative standard model. Using the Seiberg-Witten map, we calculate the production cross-section considering all orders of the noncommutative parameter . We consider the effect of earth's rotation on the orientation of with respect to the laboratory frame and thus on the total cross-section, it's azimuthal distribution and rapidity distribution for the machine energy ranging from 0.5 TeV to 3.0 TeV corresponding to the noncommutative scale 0.5 TeV.

    hep-phInt.J.Mod.Phys.A(2015)·10 citations
  9. 09*

    Unveiling the Proton Spin Decomposition at a Future Electron-Ion Collider

    Elke C. Aschenauer🇺🇸 · R. Sassot🇦🇷 · M. Stratmann🇩🇪

    We present a detailed assessment of how well a future Electron-Ion Collider could constrain helicity parton distributions in the nucleon and, therefore, unveil the role of the intrinsic spin of quarks and gluons in the proton's spin budget. Any remaining deficit in this decomposition will provide the best indirect constraint on the contribution due to the total orbital angular momenta of quarks and gluons. Specifically, all our studies are performed in the context of global QCD analyses based on realistic pseudo-data and in the light of the most recent data obtained from polarized proton-proton collisions at BNL-RHIC that have provided evidence for a significant gluon polarization in the accessible, albeit limited range of momentum fractions. We also present projections on what can be achieved on the gluon's helicity distribution by the end of BNL-RHIC operations. All estimates of current and projected uncertainties are performed with the robust Lagrange multiplier technique.

    hep-phPRD(2015)·52 citations
  10. 10*

    Towards the spectrum of a GUT from gauge invariance

    Pascal Törek🇦🇹 · Axel Maas🇦🇹

    The description of electroweak physics using perturbation theory is highly successful. Though not obvious, this is due to a subtle field-theoretical effect, the Fröhlich-Morchio-Strocchi mechanism, which links the physical spectrum to that of the elementary particles. This works because of the special structure of the standard model, and it is not a priori clear whether it works for structurally different theories. Candidates for conflicts are, e.g., grand unified theories. We study this situation in a toy model, a gauge theory with two Higgs fields and a breaking pattern . This mimics the weak-Higgs sector of the standard model. We determine the leading order predictions for the gauge invariant spectrum in this theory, and discuss a setup to test them using lattice gauge theory.

    hep-phhep-latPoS(2016)·7 citations
  11. 11*

    Decoupling of the DGLAP evolution equations by Laplace method

    G.R.Boroun🇮🇷 · S.Zarrin🇮🇷 · F. Teimoury🇮🇷

    In this paper, we derive two second- order of differential equation for the gluon and singlet distribution functions by using the Laplace transform method. We decoupled the solutions of the singlet and gluon distributions into the initial conditions (function and derivative of the function) at the virtuality separately as these solutions are defined by: \begin{eqnarray} F_{2}^{s}(x,Q^{2}) &=& \mathcal{F}(F_{s0}, \partial F_{s0})\nonumber &&\mathrm{and} \nonumber G(x,Q^{2}) &=& \mathcal{G}(G_{0}, \partial G_{0}).\nonumber \end{eqnarray} We compared our results with the MSTW parameterization and the experimental measurements of .

    hep-phEur.Phys.J.Plus(2015)·14 citations
  12. 12*

    Fluctuations in the Statistical Model of the Early Stage of nucleus-nucleus collisions

    R. V. Poberezhnyuk🇺🇦 · M. I. Gorenstein🇺🇦 · M. Gazdzicki🇩🇪

    Predictions on fluctuations of hadron production properties in central heavy ion collisions are presented. They are based on the Statistical Model of the Early Stage and extend previously published results by considering the strongly intensive measures of fluctuations. In several of the considered cases a significant change in collision energy dependence of calculated quantities as a result of the phase transition is predicted. This provides an opportunity to observe new signals of the onset of deconfinement in heavy ion collisions experiments.

    hep-phnucl-thActa Phys.Polon.B(2016)·4 citations
  13. 13*

    Strategies for an accurate determination of the X(3872) energy from QCD lattice simulations

    E. J. Garzon🇪🇸 · R. Molina🇺🇸 · A. Hosaka🇯🇵 · E. Oset🇪🇸

    We develop a method to determine accurately the binding energy of the X(3872) from lattice data for the DD* interaction. We show that, because of the small difference between the neutral and charged components of the X(3872), it is necessary to distinguish them in the energy levels of the lattice spectrum if one wishes to have a precise determination of the the binding energy of the X(3872). The analysis of the data requires the use of coupled channels. Depending on the number of levels available and the size of the box we determine the precision needed in the lattice energies to finally obtain a desired accuracy in the binding energy.

    hep-ph1 citation
  14. 14*

    Resurrecting the minimal renormalizable supersymmetric SU(5) model

    Borut Bajc🇸🇮 · Stéphane Lavignac🇫🇷 · Timon Mede🇨🇿

    It is a well-known fact that the minimal renormalizable supersymmetric SU(5) model is ruled out assuming superpartner masses of the order of a few TeV. Giving up this constraint and assuming only SU(5) boundary conditions for the soft terms, we find that the model is still alive. The viable region of the parameter space typically features superpartner masses of order to TeV, with tan beta values between 2 and 5, but lighter spectra with single states around 10 TeV are also possible. The main constraints come from proton decay, the Higgs mass, the requirement of the SU(5) spectrum being reasonably below the Planck scale, and the lifetime of the universe. A generic feature of the model is metastability of the electroweak vacuum. In the absence of a suitable dark matter particle in the neutralino sector, a light (order GeV or smaller) gravitino is a natural candidate.

    hep-phJHEP(2016)·28 citations
  15. 15*

    Warped flavor symmetry predictions for neutrino physics

    Peng Chen🇨🇳 · Gui-Jun Ding🇨🇳 · Alma. D. Rojas🇪🇸 · C. A. Vaquera-Araujo🇪🇸 · J. W. F. Valle🇪🇸

    A realistic five-dimensional warped scenario with all standard model fields propagating in the bulk is proposed. Mass hierarchies would in principle be accounted for by judicious choices of the bulk mass parameters, while fermion mixing angles are restricted by a flavor symmetry broken on the branes by flavon fields. The latter gives stringent predictions for the neutrino mixing parameters, and the Dirac CP violation phase, all described in terms of only two independent parameters at leading order. The scheme also gives an adequate CKM fit and should be testable within upcoming oscillation experiments.

    hep-phhep-thJHEP(2016)·86 citations
  16. 16*

    Strangeness production and long-range correlations in pp collisions in string fusion approach

    Vladimir Kovalenko🇷🇺 · Vladimir Vechernin (Saint Petersburg State University, Russia)🇷🇺

    The effects of string fusion on the correlations in strange particles production in proton-proton collisions at high energy are studied in the framework of a Monte Carlo string-parton model. The model is based on the strings formation in elementary dipole-dipole collisions. The hardness of the elementary interaction is defined by a transverse size of the colliding dipoles. The interaction between strings is realized in the accordance with the string fusion model prescriptions by the introduction of the lattice in the impact parameter plane and taking into account the finite rapidity length of strings. The particles species differentiation is implemented according to Schwinger mechanism. The parameters of the model are fixed with the experimental data on total inelastic cross section and charged multiplicity. In the framework of the model the long-range correlation functions with an accounting of strangeness have been studied. A new intensive event-by-event observable has been proposed, which characterizes the fraction of strange particles in the event. The predictions on the correlations between strangeness, multiplicity and mean transverse momentum are obtained for pp collisions at 7 TeV.

    hep-phnucl-thJ.Phys.Conf.Ser.(2016)·6 citations
  17. 17*

    Introduction to SARAH and related tools

    Florian Staub🇨🇭

    I give in this lecture an overview of the features of the Mathematica package SARAH, and explain how it can be used together with other codes to study all aspects of a BSM model. The focus will be on the description of the analytical calculations which SARAH can perform and how this information is used to generate automatically a spectrum generator based on SPheno. I also summarize the main aspects of the other interfaces to public codes like HiggsBounds/HiggsSignals, FeynArts/FormCalc, CalcHep, MicrOmegas, WHIZARD, Vevacious or MadGraph. The appendix contains a short tutorial about the implementation and usage of a new model.

    hep-phPoS(2016)·13 citations
  18. 18*

    Topological Susceptibility from Slabs

    Wolfgang Bietenholz🇲🇽 · Philippe de Forcrand🇨🇭 · Urs Gerber🇲🇽

    In quantum field theories with topological sectors, a non-perturbative quantity of interest is the topological susceptibility chi_t. In principle it seems straightforward to measure chi_t by means of Monte Carlo simulations. However, for local update algorithms and fine lattice spacings, this tends to be difficult, since the Monte Carlo history rarely changes the topological sector. Here we test a method to measure chi_t even if data from only one sector are available. It is based on the topological charges in sub-volumes, which we denote as slabs. Assuming a Gaussian distribution of these charges, this method enables the evaluation of chi_t, as we demonstrate with numerical results for non-linear sigma-models.

    hep-lathep-phJHEP(2015)·31 citations
  19. 19*

    Photoproduction of the and

    Ju-Jun Xie🇨🇳 · Eulogio Oset🇪🇸 · Li-Sheng Geng🇨🇳

    Assuming that the and resonances are dynamically generated states from the vector meson-vector meson interactions in -wave with spin , we study the and reactions. These reactions proceed in the following way: the incoming photon first mutates into a , , or meson via vector meson dominance, which then interacts with the , or emitted by the incoming proton to form the tensor mesons and . The picture is simple and has no free parameters, as all the parameters of the mechanism have been fixed in previous studies. We predict the differential and total cross sections of these reactions. The results can be tested in future experiments and therefore offer new clues on the nature of these tensor states.

    nucl-thhep-exhep-phnucl-exPRC(2016)·17 citations
  20. 20*

    Properties of light (anti)nuclei and (anti) hypertriton production in Pb-Pb collisions at = 2.76 TeV

    Zhi-Lei She🇨🇳 · Gang Chen🇨🇳 · Hong-ge Xu🇨🇳 · Ting-ting Zeng🇨🇳 · Di-Kai Li🇨🇳

    We investigate the properties of light (anti)nuclei and (anti)hypertriton production in Pb-Pb collisions at TeV, based on the parton and hadron cascade and dynamically constrained phase-space coalescence (PACIAE + DCPC) model. We found that the yields of light (anti)nuclei and (anti)hypertriton strongly depend on the centrality, i.e., their yields decrease rapidly with the increase of centrality bins, but their yield ratios are independent of centrality. The results of theoretical model are well consistent with ALICE data. Furthermore, we found that the integrated yields of (anti)nuclei per participant nucleon increase from peripheral to central collisions more rapidly with increasing mass number. The transverse momentum distributions of and are also discussed in the 0-10% most central Pb-Pb collisions.The coalescence parameters of light (anti)nuclei and (anti)hypernuclei are analyzed.

    nucl-thhep-phEPJA(2016)·19 citations
  21. 21*

    Recent studies of CP violation in bottom meson decays at Belle

    P. Vanhoefer🇩🇪

    We present a summary of recent studies on violation with the Belle experiment using the final data sample of B\bar{B} pairs produced at the Ypsilon(4S) resonance at the KEK asymmetric e^+ e^- collider. We discuss preliminary measurements of the branching fraction, the polarization and the asymmetries of the decay and an updated constraint on the CKM angle from the system. Being also related to , we present a preliminary measurement of the branching fraction of decays. Last, a preliminary model independent dalitz plot analysis of the decay is presented and its sensitivity to the CKM angle is discussed.

    hep-exhep-phPoS(2015)·3 citations
  22. 22*

    Pseudorapidity dependence of short-range correlations from a multi-phase transport model

    Meijuan Wang🇨🇳 · Gang Chen🇨🇳 · Guoliang Ma🇨🇳 · Yuanfang Wu🇨🇳

    Using a multi-phase transport model (AMPT) that includes both initial partonic and hadronic interactions, we study neighboring bin multiplicity correlations as a function of pseudorapidity in Au+Au collisions at GeV. It is observed that for 19.6GeV Au+Au collisions, the short-range correlations of final particles have a trough at central pseudorapidity, while for 19.6GeV AuAu collisions, the short-range correlations of final particles have a peak at central pseudorapidity. Our findings indicate that the pseudorapidity dependence of short-range correlations should contain some new physical information, and are not a simple result of the pseudorapidity distribution of final particles. The AMPT results with and without hadronic scattering are compared. It is found that hadron scattering can only increase the short-range correlations to some level, but is not responsible for the different correlation shapes for different energies. Further study shows that the different pseudorapidity dependence of short-range correlations are mainly due to partonic evolution and the following hadronization scheme.

    nucl-thhep-phCPC(2016)·0 citations
  23. 23*

    Compact Lumps

    D. Bazeia🇧🇷 · M.A. Marques🇧🇷 · R. Menezes🇧🇷

    We study the presence of lumplike solutions in models described by a single real scalar field with standard kinematics in two-dimensional spacetime. The results show several distinct models that support the presence of bell-shaped, lumplike structures which may live in a compact space.

    hep-thhep-phEPL(2015)·17 citations
  24. 24*

    Precision Electron-Beam Polarimetry using Compton Scattering at 1 GeV

    A. Narayan · D. Jones · J. C. Cornejo · M. M. Dalton · W. Deconinck · D. Dutta · D. Gaskell · J. W. Martin · K.D. Paschke · V. Tvaskis · A. Asaturyan · J. Benesch and 24 other authors

    We report on the highest precision yet achieved in the measurement of the polarization of a low energy, (1 GeV), electron beam, accomplished using a new polarimeter based on electron-photon scattering, in Hall~C at Jefferson Lab. A number of technical innovations were necessary, including a novel method for precise control of the laser polarization in a cavity and a novel diamond micro-strip detector which was able to capture most of the spectrum of scattered electrons. The data analysis technique exploited track finding, the high granularity of the detector and its large acceptance. The polarization of the A, ~GeV electron beam was measured with a statistical precision of ~1\% per hour and a systematic uncertainty of 0.59\%. This exceeds the level of precision required by the \qweak experiment, a measurement of the vector weak charge of the proton. Proposed future low-energy experiments require polarization uncertainty ~0.4\%, and this result represents an important demonstration of that possibility. This measurement is also the first use of diamond detectors for particle tracking in an experiment.

    nucl-exhep-phnucl-thphysics.acc-ph+1PRX(2016)·48 citations
  25. 25*

    Are Electron Scattering Data Consistent with a Small Proton Radius?

    Keith Griffioen🇺🇸 · Carl Carlson🇺🇸 · Sarah Maddox🇺🇸

    We determine the charge radius of the proton by analyzing the published low momentum transfer electron-proton scattering data from Mainz. We note that polynomial expansions of the form factor converge for momentum transfers squared below , where is the pion mass. Expansions with enough terms to fit the data, but few enough not to overfit, yield proton radii smaller than the CODATA or Mainz values and in accord with the muonic atom results. We also comment on analyses using a wider range of data, and overall obtain a proton radius ) fm.

    nucl-exhep-phPRC(2016)·94 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.