24,908 research outputs found
Lepton flavour violation in future linear colliders in the long-lived stau NLSP scenario
We analyze the prospects of observing lepton flavour violation in future e-e-
and e+e- linear colliders in scenarios where the gravitino is the lightest
supersymmetric particle, and the stau is the next-to-lightest supersymmetric
particle. The signals consist of multilepton final states with two heavily
ionizing charged tracks produced by the long-lived staus. The Standard Model
backgrounds are very small and the supersymmetric backgrounds can be kept well
under control by the use of suitable kinematical cuts. We discuss in particular
the potential of the projected International Linear Collider to discover lepton
flavour violation in this class of scenarios, and we compare the estimated
sensitivity with the constraints stemming from the non-observation of rare
decays.Comment: 30 pages, 12 figures. Discussion extended to include the efficiency
of identifying long-lived staus, references added. To appear in JHE
Observations of transients and pulsars with LOFAR international stations
The LOw FRequency ARray - LOFAR is a new radio telescope that is moving the
science of radio pulsars and transients into a new phase. Its design places
emphasis on digital hardware and flexible software instead of mechanical
solutions. LOFAR observes at radio frequencies between 10 and 240 MHz where
radio pulsars and many transients are expected to be brightest. Radio frequency
signals emitted from these objects allow us to study the intrinsic pulsar
emission and phenomena such as propagation effects through the interstellar
medium. The design of LOFAR allows independent use of its stations to conduct
observations of known bright objects, or wide field monitoring of transient
events. One such combined software/hardware solution is called the Advanced
Radio Transient Event Monitor and Identification System (ARTEMIS). It is a
backend for both targeted observations and real-time searches for millisecond
radio transients which uses Graphical Processing Unit (GPU) technology to
remove interstellar dispersion and detect millisecond radio bursts from
astronomical sources in real-time using a single LOFAR station.Comment: To appear in the proceedings of the Electromagnetic Radiation from
Pulsars and Magnetars conference, Zielona Gora, 2012. 4 pages, 1 figur
Non-universal gauge boson and the spin correlation of top quark pair production at colliders
In the off-diagonal basis, we discuss the contributions of the non-universal
gauge boson predicted by the topcolor-assisted technicolor () model
to the spin configurations and the spin correlation observable of the top quark
pair production via the process . Our numerical results
show that the production cross sections for the like-spin states, which vanish
in the standard model, can be significantly large as .
With reasonable values of the mass and the coupling parameter
,
exchange can generate large corrections to the spin correlation
observable.Comment: 16 pages, 5 figure
Squark anti-squark pair production at the LHC: the electroweak contribution
We present the complete NLO electroweak contribution of
to the production of diagonal
squark--anti-squark pairs in proton--proton collisions. Compared to the
lowest-order electroweak terms, the
NLO contributions are also significant. We discuss the LO and NLO electroweak
effects in cross sections and distributions at the LHC for the production of
squarks different from top squarks, in various supersymmetric benchmark
scenarios.Comment: 38 pages, 21 figures. Replaced with the version published in JHE
Radiative corrections to the semileptonic and hadronic Higgs-boson decays H -> W W/Z Z -> 4 fermions
The radiative corrections of the strong and electroweak interactions are
calculated for the Higgs-boson decays H -> WW/ZZ -> 4f with semileptonic or
hadronic four-fermion final states in next-to-leading order. This calculation
is improved by higher-order corrections originating from heavy-Higgs-boson
effects and photonic final-state radiation off charged leptons. The W- and
Z-boson resonances are treated within the complex-mass scheme, i.e. without any
resonance expansion or on-shell approximation. The calculation essentially
follows our previous study of purely leptonic final states. The electroweak
corrections are similar for all four-fermion final states; for integrated
quantities they amount to some per cent and increase with growing Higgs-boson
mass M_H, reaching 7-8% at M_H \sim 500 GeV. For distributions, the corrections
are somewhat larger and, in general, distort the shapes. Among the QCD
corrections, which include corrections to interference contributions of the
Born diagrams, only the corrections to the squared Born diagrams turn out to be
relevant. These contributions can be attributed to the gauge-boson decays, i.e.
they approximately amount to \alpha_s/\pi for semileptonic final states and
2\alpha_s/\pi for hadronic final states. The discussed corrections have been
implemented in the Monte Carlo event generator PROPHECY4F.Comment: 29 pages, LaTeX, 30 postscript figure
NLO electroweak contributions to gluino pair production at hadron colliders
We calculate the full corrections to the
process of gluino pair production at hadron colliders in the framework of the
real MSSM. We show that these contributions can be neglected at the LHC
performing a scan over a wide region of the parameter space. The impact of
these corrections in the parameter range investigated at the Tevatron is small.Comment: 26 pages, 12 figure
CP violation in the secluded U(1)'-extended MSSM
We study the Higgs sector of the secluded -extended MSSM (sMSSM)
focusing on CP violation. Using the one-loop effective potential that includes
contributions from quarks and squarks in the third generation, we search for
the allowed region under theoretical and experimental constraints. It is found
that the possible region for the electroweak vacuum to exist is quite limited,
depending on the parameters in the model. The masses and couplings of the Higgs
bosons are calculated with/without CP violation. Even at the tree level, CP
violation is possible by complex soft SUSY breaking masses. Similar to the CPX
scenario in the MSSM, the scalar-pseudoscalar mixing enables the lightest Higgs
boson mass to become smaller than the boson mass while the coupling with
the boson is sufficiently suppressed to avoid the LEP experimental
constraints. However, unlike the CPX scenario, large and are not
required for the realization of large CP violation. The typical spectrum of the
SUSY particles is thus different. We also investigate the possible upper bound
of the lightest Higgs boson in the case of spontaneous CP violation. The
maximal value of it can reach above 100 GeV with maximal CP-violating phases.Comment: 28 pages, 16 figures, JHEP styl
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