2,490 research outputs found

    Prospects for Detecting Neutrino Signals from Annihilating/Decaying Dark Matter to Account for the PAMELA and ATIC results

    Full text link
    Recent PAMELA data show that positron fraction has an excess above several GeV while anti-proton one is not. Moreover ATIC data indicates that electron/positron flux have a bump from 300 GeV to 800 GeV. Both annihilating dark matter (DM) with large boost factor and decaying DM with the life around 1026s 10^{26} s can account for the PAMELA and ATIC observations if their main final products are charged leptons (ee, μ\mu and τ\tau). In this work, we calculated the neutrino flux arising from μ\mu and τ\tau which originate from annihilating/decaying DM, and estimated the final muon rate in the neutrino telescopes, namely Antares and IceCube. Given the excellent angular resolution, Antares and IceCube are promising to discover the neutrino signals from Galactic center and/or large DM subhalo in annihilating DM scenario, but very challenging in decaying DM scenario.Comment: 21 pages, 7 figures, 2 tables. V2: references added. V3: the number density of massive subhalo has been discussed in the appendix; accepted by PR

    The behavior of real exchange rates: the case of Japan

    Get PDF
    The study examines the convergence rate of mean reversion by contrasting the estimated half-life of real exchange rate (RER). We employ an extensive monthly consumer price index (CPI)-based product price’s panel for Japan (the U.S. as the num´eraire). We find that the disaggregated RERs are persistent due to the cross-sectional dependence problems. By controlling common correlated effects, the estimated half-life for all goods may fall to as low as 2.54 years, below the consensus view of 3 to 5 years summarized by Rogoff (1996). After correcting the small-sample bias, the estimated half-life of deviations from purchasing power parity (PPP) increase by 1.03 year. Our findings also support that the half-life of mean reversion of RER is about 3.55 years for traded goods, about 0.11 year lower than non-traded goods. We also show that traded goods and non-traded goods perform distinct distributions of persistence

    Investigating the NCQ scaling of elliptic flow at LHC with a multiphase transport model

    Full text link
    The number of constituent quark (NCQ) scaling behavior of elliptic flow has been systematically studied at the LHC energy within the framework of a multiphase transport model (AMPT) in this work. We find that the parameters used to generate the initial states and the collision centrality are important for the existence of NCQ scaling even when hadronic rescattering contribution is off in Pb-Pb collisions of sNN=2.76\sqrt{s_{NN}}=2.76 TeV. By turning on the hadron rescattering process, the hadronic evolution impacts are also found to be significant. Extending the analysis to Pb-Pb collsions of sNN=5.02\sqrt{s_{NN}}=5.02 TeV, one would observe similar qualitative features

    Neutrino Constraints on Inelastic Dark Matter after CDMS II

    Full text link
    We discuss the neutrino constraints from solar and terrestrial dark matter (DM) annihilations in the inelastic dark matter (iDM) scenario after the recent CDMS II results. To reconcile the DAMA/LIBRA data with constraints from all other direct experiments, the iDM needs to be light (mχ<100m_\chi < 100 GeV) and have a large DM-nucleon cross section (σn∼\sigma_n \sim 10−4^{-4} pb in the spin-independent (SI) scattering and σn∼\sigma_n \sim 10 pb in the spin-dependent (SD) scattering). The dominant contribution to the iDM capture in the Sun is from scattering off Fe/Al in the SI/SD case. Current bounds from Super-Kamiokande exclude the hard DM annihilation channels, such as W+W−W^+W^-, ZZZZ, ttˉt\bar{t} and τ+τ−\tau^+ \tau^-. For soft channels such as bbˉb\bar{b} and ccˉc \bar{c}, the limits are loose, but could be tested or further constrained by future IceCube plus DeepCore. For neutrino constraints from the DM annihilation in the Earth, due to the weaker gravitational effect of the Earth and inelastic capture condition, the constraint exists only for small mass splitting δ<\delta < 40 keV and mχ∼(10,50)m_\chi \sim (10, 50) GeV even in the τ+τ−\tau^+ \tau^- channel.Comment: 11 pages, 8 figure

    Gamma rays and neutrinos from dark matter annihilation in galaxy clusters

    Full text link
    The γ\gamma-ray and neutrino emissions from dark matter (DM) annihilation in galaxy clusters are studied. After about one year operation of Fermi-LAT, several nearby clusters are reported with stringent upper limits of GeV γ\gamma-ray emission. We use the Fermi-LAT upper limits of these clusters to constrain the DM model parameters. We find that the DM model distributed with substructures predicted in cold DM (CDM) scenario is strongly constrained by Fermi-LAT γ\gamma-ray data. Especially for the leptonic annihilation scenario which may account for the e±e^{\pm} excesses discovered by PAMELA/Fermi-LAT/HESS, the constraint on the minimum mass of substructures is of the level 102−10310^2-10^3 M⊙_{\odot}, which is much larger than that expected in CDM picture, but is consistent with a warm DM scenario. We further investigate the sensitivity of neutrino detections of the clusters by IceCube. It is found that neutrino detection is much more difficult than γ\gamma-rays. Only for very heavy DM (∼10\sim 10 TeV) together with a considerable branching ratio to line neutrinos the neutrino sensitivity is comparable with that of γ\gamma-rays.Comment: 21 pages, 8 figures and 1 table; extended discussion about the uncertainties of concentration and subhalo models, figures replotted for better read; references updated; accepted for publication by Phys. Rev.

    Finite volume effects of the Nambu-Jona-Lasinio model with the running coupling constant

    Full text link
    With the Schwinger's proper-time formalism of the Nambu-Jona-Lasinio model, we investigate the finite volume effects in the presence of magnetic fields. Since the coupling constant GG can be influenced by strong magnetic fields, the model is solved with a running coupling constant G(B)G(B) which is fitted by the lattice average (Σu+Σd)/2(\Sigma_u+\Sigma_d)/2 and difference Σu−Σd\Sigma_u-\Sigma_d. The investigation mainly focuses on the constituent quark mass and the thermal susceptibility depending on the magnetic fields, the temperatures and the finite sizes. For the model in finite or infinite volume, the magnetic fields can increase the constituent quark mass while the temperatures can decrease it inversely. There is a narrow range of the box length that makes the effects of finite volume perform prominently. The model will behave close to infinite volume limit for larger box length. It is shown that the influence of finite volume can be changed by magnetic fields and temperatures. Finally, we discuss the thermal susceptibility depending on the temperature in finite volume in the presence of magnetic fields.Comment: 13 pages, 6 figure

    H\to hh in the Mirror Model at the CERN Large Hadron Collider

    Full text link
    The Higgs sector may play an important role in detecting the mirror particles, which can be the candidates of the dark matter and appear as missing energy in the detectors at the LHC. In this paper we worked out the Higgs boson spectrum and the Higgs couplings for the symmetric vacuum, namely v1=v2=vv_1=v_2=v, in the mirror model, and investigated the constraints from electro-weak precision observable (EWPO). Our study showed that the EWPO has already constrained the Higgs boson sector severely. We then explored the Higgs boson phenomenology, and focused on the scenario that the heavier Higgs boson HH can decay into a pair of lighter Higgs boson hh. We proposed to study the invisible decay of the Higgs boson via the pair production of them, in which one Higgs boson decays into bottom quarks and the other decays invisibly. Our detail simulation for signals and backgrounds showed that the observation of signal can reach 5σ5\sigma significance for mH=260m_H=260 GeV and mh=115m_h=115 GeV with 10fb−110 fb^{-1}integrated luminosity at the LHC. Moreover the possible method to further suppress dominant ZbbˉZb\bar{b} background was discussed. We also simulated the signals and backgrounds for H→hh→4bH \to h h \to 4b. Our results showed that it is very difficult to isolate the signals from huge QCD continuum backgrounds.Comment: 9 pages, revtex4, typo correcte

    End-to-end speech recognition modeling from de-identified data

    Full text link
    De-identification of data used for automatic speech recognition modeling is a critical component in protecting privacy, especially in the medical domain. However, simply removing all personally identifiable information (PII) from end-to-end model training data leads to a significant performance degradation in particular for the recognition of names, dates, locations, and words from similar categories. We propose and evaluate a two-step method for partially recovering this loss. First, PII is identified, and each occurrence is replaced with a random word sequence of the same category. Then, corresponding audio is produced via text-to-speech or by splicing together matching audio fragments extracted from the corpus. These artificial audio/label pairs, together with speaker turns from the original data without PII, are used to train models. We evaluate the performance of this method on in-house data of medical conversations and observe a recovery of almost the entire performance degradation in the general word error rate while still maintaining a strong diarization performance. Our main focus is the improvement of recall and precision in the recognition of PII-related words. Depending on the PII category, between 50%−90%50\% - 90\% of the performance degradation can be recovered using our proposed method.Comment: Accepted to INTERSPEECH 202
    • …
    corecore