1,507 research outputs found
Resurrecting light stops after the 125 GeV Higgs in the baryon number violating CMSSM
In order to accommodate the observed Higgs boson mass in the CMSSM, the stops
must either be very heavy or the mixing in the stop sector must be very large.
Lower stop masses, possibly more accessible at the LHC, still give the correct
Higgs mass only if the trilinear stop mixing parameter is in the
multi-TeV range. Recently it has been shown that such large stop mixing leads
to an unstable electroweak vacuum which spontaneously breaks charge or colour.
In this work we therefore go beyond the CMSSM and investigate the effects of
including baryon number violating operators on the stop and Higgs sectors. We find that for light stop masses as low as 220 GeV are consistent
with the observed Higgs mass as well as flavour constraints while allowing for
a stable vacuum. The light stop in this scenario is often the lightest
supersymmetric particle. We furthermore discuss the importance of the one-loop
corrections involving R-parity violating couplings for a valid prediction of
the light stop masses.Comment: 26 pages, 9 figures; v2: slightly extended discussion about bounds
from flavour observables; matches published versio
Chiral properties of hematite ({\alpha}-Fe2O3) inferred from resonant Bragg diffraction using circularly polarized x-rays
Chiral properties of the two phases - collinear motif (below Morin transition
temperature, TM=250 K) and canted motif (above TM) - of magnetically ordered
hematite ({\alpha}-Fe2O3) have been identified in single crystal resonant x-ray
Bragg diffraction, using circular polarized incident x-rays tuned near the iron
K-edge. Magneto-electric multipoles, including an anapole, fully characterize
the high-temperature canted phase, whereas the low-temperature collinear phase
supports both parity-odd and parity-even multipoles that are time-odd. Orbital
angular momentum accompanies the collinear motif, while it is conspicuously
absent with the canted motif. Intensities have been successfully confronted
with analytic expressions derived from an atomic model fully compliant with
chemical and magnetic structures. Values of Fe atomic multipoles previously
derived from independent experimental data, are shown to be completely
trustworthy
General MSSM signatures at the LHC with and without R-parity
We present the possible signatures appearing in general realizations of the
MSSM based on 14 unrelated mass parameters at the SUSY scale. The parameters of
the general MSSM are reduced by assuming a degeneracy of the sfermions of the
first two generations with the same quantum numbers. We also assume no
mass-splitting between neutral and charged Higgsinos. We do allow for separate
soft breaking terms for the third generation sfermons. We consider all possible
resulting relevant mass orderings and check for
the dominant decay cascades and the corresponding collider signatures. In
determining the dominant decay modes we assume that mixing between sparticles
is sub-dominant. As preferred signatures, we consider charged leptons, missing
transverse momentum, jets, and or Higgs bosons. We include also the
cases of bi- and trilinear R-parity violation and show that specific signatures
can be used to distinguish the different scenarios.Comment: 18 pages, 14 tables. v2: Minor changes to improve readability of the
result
New bounds on trilinear R-parity violation from lepton flavor violating observables
Many extensions of the leptonic sector of the Minimal Supersymmetric Standard
Model (MSSM) are known, most of them leading to observable flavor violating
effects. It has been recently shown that the 1-loop contributions to lepton
flavor violating three-body decays involving the boson
may be dominant, that is, much more important than the usual photonic penguins.
Other processes like - conversion in nuclei and flavor violating
decays into mesons are also enhanced by the same effect. This is for instance
also the case in the MSSM with trilinear R-parity violation. The aim of this
work is to derive new bounds on the relevant combinations of R-parity violating
couplings and to compare them with previous results in the literature. For
heavy supersymmetric spectra the limits are improved by several orders of
magnitude. For completeness, also constraints coming from flavor violating
-decays and tree-level decay channels are presented
for a set of benchmark points.Comment: 21 pages; 5 figures; v2: corrected bug, conclusion unchange
A precision study of the fine tuning in the DiracNMSSM
Recently the DiracNMSSM has been proposed as a possible solution to reduce
the fine tuning in supersymmetry. We determine the degree of fine tuning needed
in the DiracNMSSM with and without non-universal gaugino masses and compare it
with the fine tuning in the GNMSSM. To apply reasonable cuts on the allowed
parameter regions we perform a precise calculation of the Higgs mass. In
addition, we include the limits from direct SUSY searches and dark matter
abundance. We find that both models are comparable in terms of fine tuning,
with the minimal fine tuning in the GNMSSM slightly smaller.Comment: 20 pages + appendices, 10 figure
4f-spin dynamics in La(2-x-y)Sr(x)Nd(y)CuO(4)
We have performed inelastic magnetic neutron scattering experiments on
La(2-x-y)Sr(x)Nd(y)CuO(4) in order to study the Nd 4f-spin dynamics at low
energies. In all samples we find at high temperatures a quasielastic line
(Lorentzian) with a line width which decreases on lowering the temperature. The
temperature dependence of the quasielastic line width Gamma/2(T) can be
explained with an Orbach-process, i.e. a relaxation via the coupling between
crystal field excitations and phonons. At low temperatures the Nd-4f magnetic
response S(Q,omega) correlates with the electronic properties of the
CuO(2)-layers. In the insulator La(2-y)Nd(y)CuO(4) the quasielastic line
vanishes below 80 K and an inelastic excitation occurs. This directly indicates
the splitting of the Nd3+ ground state Kramers doublet due to the static
antiferromagnetic order of the Cu moments. In La(1.7-x)Sr(x)Nd(0.3)CuO(4) with
x = 0.12, 0.15 and La(1.4-x)Sr(x)Nd(0.6)CuO(4) with x = 0.1, 0.12, 0.15, 0.18
superconductivity is strongly suppressed. In these compounds we observe a
temperature independent broad quasielastic line of Gaussian shape below T about
30 K. This suggests a distribution of various internal fields on different Nd
sites and is interpreted in the frame of the stripe model. In
La(1.8-y)Sr(0.2)Nd(y)CuO(4) (y = 0.3, 0.6) such a quasielastic broadening is
not observed even at lowest temperature.Comment: 8 pages, 10 figures included, to appear in Phys. Rev.
Studies on X-ray Thomson Scattering from Antiferroquadrupolar Order in TmTe
We study Thomson scattering from the antiferroquadrupole ordering phase in
TmTe. On the basis of the group theoretical treatment, we classify the
selection rules of the scattering intensity governed by the orientation of the
scattering vector G. Then, numerical verification is performed by invoking the
ground states which are deduced from a J=7/2 multiplet model. The obtained
intensity varies drastically depending on the magnitude and direction of G. We
also calculate the scattering intensities under the applied field for H//(001)
and (110). Their results behave differently when the orientation of G is
changed, which is ascribed to the difference of their primary order parameters;
O_{2}^{0} and O_{2}^{2} for H // (001) and (110), respectively. We make
critical comparisons between our results for TmTe and the experimental ones for
CeB_6. First, we assert that the intensities expected from TmTe at several
forbidden Bragg spots are sufficient enough to be experimentally detected.
Second, their intensities at (7/2,1/2,1/2) differ significantly and may be
attributed to the difference of the order parametersbetween the \Gamma_3-type
(O_{2}^{2} and O_{2}^{0}) and \Gamma_5-type (O_{yz}, O_{zx}, and O_{xy})
components, respectively.Comment: 18 pages, 3 figures, to be published in J. Phys. Soc. Jp
Enhancing lepton flavour violation in the supersymmetric inverse seesaw beyond the dipole contribution
In minimal supersymmetric models the -penguin usually provides
sub-dominant contributions to charged lepton flavour violating observables. In
this study, we consider the supersymmetric inverse seesaw in which the
non-minimal particle content allows for dominant contributions of the
-penguin to several lepton flavour violating observables. In particular, and
due to the low-scale (TeV) seesaw, the penguin contribution to, for instance,
\Br(\mu \to 3e) and conversion in nuclei, allows to render some of
these observables within future sensitivity reach. Moreover, we show that in
this framework, the -penguin exhibits the same non-decoupling behaviour
which had previously been identified in flavour violating Higgs decays in the
Minimal Supersymmetric Standard Model.Comment: 29 pages, 9 figures, 4 tables; v2: minor corrections, version to
appear in JHE
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