182 research outputs found
Wino Dark Matter in light of the AMS-02 2015 Data
The AMS-02 collaboration has recently reported the antiproton to proton ratio
with improved accuracy. In view of uncertainties of the production and the
propagation of the cosmic rays, the observed ratio is still consistent with the
secondary astrophysical antiproton to proton ratio. However, it is nonetheless
enticing to examine whether the observed spectrum can be explained by a
strongly motivated dark matter, the wino dark matter. As we will show, we find
that the antiproton flux from the wino annihilation can explain the observed
spectrum well for its mass range 2.5-3 TeV. The fit to data becomes
particularly well compared to the case without the annihilation for the thermal
wino dark matter case with a mass about 3 TeV. The ratio is predicted to be
quickly decreased at the energy several hundreds of GeV, if this possibility is
true, and it will be confirmed or ruled out in near future when the AMS-02
experiment accumulates enough data at this higher energy region.Comment: 6 pages, 2 figures, version accepted for publication in PRD (Rapid
Communication
Mass of Decaying Wino from AMS-02 2014
We revisit the decaying wino dark matter scenario in the light of the updated
positron fraction, electron and positron fluxes in cosmic ray recently reported
by the AMS-02 collaboration. We show the AMS-02 results favor the mass of the
wino dark matter at around a few TeV, which is consistent with the prediction
on the wino mass in the pure gravity mediation model.Comment: 10 pages, 1 figur
A 125GeV Higgs Boson and Muon g-2 in More Generic Gauge Mediation
Recently, the ATLAS and CMS collaborations reported exciting hints of a
Standard Model-like Higgs boson with a mass around 125GeV. A Higgs boson this
heavy is difficult to realize in conventional models of gauge mediation. Here
we revisit the lightest Higgs boson mass in "more generic gauge mediation,"
where the Higgs doublets mix with the messenger doublets. We show that a Higgs
boson mass around 125GeV can be realized in more generic gauge mediation
models, even for a relatively light gluino mass ~1TeV. We also show that the
muon anomalous magnetic moment can be within 1sigma of the experimental value
for these models, even when the Higgs boson is relatively heavy. We also
discuss the LHC constraints and the prospects of discovery.Comment: 28 pages, 7 figures. Corrections and references are adde
Split Generation in the SUSY Mass Spectrum and B_s-{\bar B}_s Mixing
We show that the like-sign di-muon anomaly reported recently by the D0
Collaboration can be explained in the supersymmetric standard model (SM) if the
squarks and the sleptons in the first two generations have relatively small,
but degenerate mass spectrum, and those in the third generation are larger as
O(1-10)TeV. This split generation model provides large contributions to the
B_s-{\bar B}_s mixing, although most of the FCNC's are suppressed due to the
large masses of the third generation squarks or the GIM mechanism partially
acting on the first and second generations.Comment: 15 pages, 1 figur
A Test for Light Gravitino Scenario at the LHC
Supersymmetric (SUSY) standard models in which the lightest SUSY particle
(LSP) is an ultralight gravitino (m_{3/2}=O(1) eV) are very attractive, since
they are free from the cosmological gravitino problems. If the neutralino is
the next lightest SUSY particle (NLSP), it decays into a photon and the
gravitino in collider experiments. We propose a simple test for the lightness
of gravitino at the LHC.Comment: 9 pages, 2 figure
Resonant Leptogenesis in the Minimal B-L Extended Standard Model at TeV
We investigate the resonant leptogenesis scenario in the minimal B-L extended
standard model(SM) with the B-L symmetry breaking at the TeV scale. Through
detailed analysis of the Boltzmann equations, we show how much the resultant
baryon asymmetry via leptogenesis is enhanced or suppressed, depending on the
model parameters, in particular, the neutrino Dirac Yukawa couplings and the
TeV-scale Majorana masses of heavy degenerate neutrinos. In order to consider a
realistic case, we impose a simple ansatz for the model parameters and analyze
the neutrino oscillation parameters and the baryon asymmetry via leptogenesis
as a function of only a single CP-phase. We find that for a fixed CP-phase all
neutrino oscillation data and the observed baryon asymmetry of the present
universe can be simultaneously reproduced.Comment: 25 pages, 15 figures, version to be published in Phys. Rev.
Gauge Mediation with Sequestered Supersymmetry Breaking
Gauge mediation models have two drawbacks, that is, the so-called \mu-problem
and a lack of predictability of the gravitino dark matter abundance. We show
that conformal sequestering in the supersymmetry breaking sector offers
attractive solutions to both problems. The correct mass scale of the \mu and
B_\mu terms is generated by taking the gravitino mass of O(100) GeV without
causing the flavor-changing neutral-current problem. Moreover, a large
anomalous dimension of the supersymmetry breaking field naturally realizes the
small stau and neutralino mass difference required for the coannihilation to
work yielding the right dark matter abundance.Comment: 23 pages, 4 figures, 2 table
Fluorescent nuclear track images of Ag-activated phosphate glass irradiated with photons and heavy charged particles
In this paper we report about the demonstration of the nuclear track imaging capabilities of Ag-activated phosphate glass. A 375 nm laser and confocal laser scanning microscopy (CLSM) were respectively used for track excitation and detection. Specifically, the blue and orange radiophotoluminescent (RPL) tracks and dose distributions observed after irradiation with soft X-rays, gamma rays and heavy charged particles (HCPs) are examined. In addition, the origins of the reductions in RPL efficiency for high-dose X-ray irradiation and for irradiation with HCPs with high linear energy transfer (LET) values are investigated via a CLSM and a conventional fluorescent reader and discussed. © 2017 Elsevier B.V.Embargo Period 12 month
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