4,243 research outputs found
Higgs decays in supersymmetric models with light neutralinos
In the Minimal Supersymmetric Standard Model, neutralinos lighter than 50 GeV
are compatible with all accelerator, precision, and cosmological bounds. Such
neutralinos might constitute a relevant decay channel for the Higgs boson,
modifying its expected signatures at hadron colliders. We study the branching
ratio h --> \chi\chi and determine the region in the supersymmetric parameter
space where it is sizable. We have found that, in fact, the Higgs may
dominantly decay into neutralino pairs. Besides, as a result of this new
channel, the branching ratio into visible modes, such as h --> \gamma\gamma,
gets suppressed.Comment: 9 pages, 5 figure
Equilibrium random-field Ising critical scattering in the antiferromagnet Fe(0.93)Zn(0.07)F2
It has long been believed that equilibrium random-field Ising model (RFIM)
critical scattering studies are not feasible in dilute antiferromagnets close
to and below Tc(H) because of severe non-equilibrium effects. The high magnetic
concentration Ising antiferromagnet Fe(0.93)Zn(0.07)F2, however, does provide
equilibrium behavior. We have employed scaling techniques to extract the
universal equilibrium scattering line shape, critical exponents nu = 0.87 +-
0.07 and eta = 0.20 +- 0.05, and amplitude ratios of this RFIM system.Comment: 4 pages, 1 figure, minor revision
Some remarks on the GNS representations of topological -algebras
After an appropriate restatement of the GNS construction for topological
-algebras we prove that there exists an isomorphism among the set
\cycl(A) of weakly continuous strongly cyclic -representations of a
barreled dual-separable -algebra with unit , the space \hilb_A(A^*) of
the Hilbert spaces that are continuously embedded in and are
-invariant under the dual left regular action of and the set of the
corresponding reproducing kernels. We show that these isomorphisms are cone
morphisms and we prove many interesting results that follow from this fact. We
discuss how these results can be used to describe cyclic representations on
more general inner product spaces.Comment: 34 pages. Minor changes. To appear in J. Math. Phys. 49 (4) Apr-0
How light can the lightest neutralino be?
In this talk we summarize previous work on mass bounds of a light neutralino
in the Minimal Supersymmetric Standard Model. We show that without the GUT
relation between the gaugino mass parameters M_1 and M_2, the mass of the
lightest neutralino is essentially unconstrained by collider bounds and
precision observables. We conclude by considering also the astrophysics and
cosmology of a light neutralino.Comment: 6 pages, 3 figures, to appear in the proceedings of the 16th
International Symposium on Particles, Strings and Cosmology (PASCOS2010),
Valencia (Spain), July 19th - 23rd, 201
Two Higgs Bosons at the Tevatron and the LHC?
The best fit to the Tevatron results in the bb channel and the mild excesses
at CMS in the gamma-gamma channel at 136 GeV and in the tau-tau channel above
132 GeV can be explained by a second Higgs state in this mass range, in
addition to the one at 125 GeV recently discovered at the LHC. We show that a
scenario with two Higgs bosons at 125 GeV and 136 GeV can be consistent with
practically all available signal rates, including a reduced rate in the tau-tau
channel around 125 GeV as reported by CMS. An example in the parameter space of
the general NMSSM is given where, moreover, the signal rates of the 125 GeV
Higgs boson in the gamma-gamma channels are enhanced relative to the
expectation for a SM Higgs boson of this mass.Comment: 13 pages, 4 Table
Global fit to Higgs signal strengths and couplings and implications for extended Higgs sectors
The most recent LHC data have provided a considerable improvement in the
precision with which various Higgs production and decay channels have been
measured. Using all available public results from ATLAS, CMS and the Tevatron,
we derive for each final state the combined confidence level contours for the
signal strengths in the (gluon fusion + ttH associated production) versus
(vector boson fusion + VH associated production) space. These "combined signal
strength ellipses" can be used in a simple, generic way to constrain a very
wide class of New Physics models in which the couplings of the Higgs boson
deviate from the Standard Model prediction. Here, we use them to constrain the
reduced couplings of the Higgs boson to up-quarks, down-quarks/leptons and
vector boson pairs. We also consider New Physics contributions to the
loop-induced gluon-gluon and photon-photon couplings of the Higgs, as well as
invisible/unseen decays. Finally, we apply our fits to some simple models with
an extended Higgs sector, in particular to Two-Higgs-Doublet models of Type I
and Type II, the Inert Doublet model, and the Georgi-Machacek triplet Higgs
model.Comment: 31 pages, 15 figures; v2: fixed important factor of 2 missing in Eq.
(1) (results unchanged), extended discussion in the next-to-last paragraph of
Section 3, some references added; v3: appendices and references added,
matches version accepted by PR
Light mixed sneutrinos as thermal dark matter
In supersymmetric models with Dirac neutrino masses, a left-right mixed
sneutrino can be a viable dark matter candidate. We examine the
MSSM+ parameter space where this is the case with particular
emphasis on light sneutrinos with masses below 10 GeV. We discuss implications
for direct and indirect dark matter searches, including the relevant
uncertainties, as well as consequences for collider phenomenology.Comment: 33 pages, 14 figures; one figure and references adde
Higgs Couplings at the End of 2012
Performing a fit to all publicly available data, we analyze the extent to
which the latest results from the LHC and Tevatron constrain the couplings of
the Higgs boson-like state at ~ 125 GeV. To this end we assume that only
Standard Model (SM) particles appear in the Higgs decays, but tree-level Higgs
couplings to the up-quarks, down-quarks and vector bosons, relative to the SM
are free parameters. We also assume that the leptonic couplings relative to the
SM are the same as for the down-quark, and a custodial symmetry for the V=W,Z
couplings. In the simplest approach, the effective Higgs couplings to gluons
and photons are computed in terms of the previous parameters. This approach is
also applied to Two-Higgs-Doublet Models of Type I and Type II. However, we
also explore the possibility that the net Higgs to gluon-gluon and gamma-gamma
couplings have extra loop contributions coming from Beyond-the-Standard Model
physics. We find that the SM p-value ~ 0.5 is more than 2 sigma away from fits
in which: a) there is some non-SM contribution to the gamma-gamma coupling of
the Higgs; or b) the sign of the top quark coupling to the Higgs is opposite
that of the W coupling. In both these cases p-values ~ 0.9 can be achieved.
Since option b) is difficult to realize in realistic models, it would seem that
new physics contributions to the effective couplings of the Higgs are
preferred.Comment: 25 pages, 11 figures; v2: minor corrections, references added; v3:
acknowledgement adde
Status of invisible Higgs decays
We analyze the extent to which the LHC and Tevatron results as of the end of
2012 constrain invisible (or undetected) decays of the Higgs boson-like state
at ~ 125 GeV. To this end we perform global fits for several cases: 1) a Higgs
boson with Standard Model (SM) couplings but additional invisible decay modes;
2) SM couplings to fermions and vector bosons, but allowing for additional new
particles modifying the effective Higgs couplings to gluons and photons; 3) no
new particles in the loops but tree-level Higgs couplings to the up-quarks,
down-quarks and vector bosons, relative to the SM, treated as free parameters.
We find that in the three cases invisible decay rates of 23%, 61%, 88%,
respectively, are consistent with current data at 95% confidence level (CL).
Limiting the coupling to vector bosons, CV, to CV < 1 in case 3) reduces the
allowed invisible branching ratio to 56% at 95% CL. Requiring in addition that
the Higgs couplings to quarks have the same sign as in the SM, an invisible
rate of up to 36% is allowed at 95% CL. We also discuss direct probes of
invisible Higgs decays, as well as the interplay with dark matter searches.Comment: 14 pages, 8 figures; v2: extended discussion on ZH associated
production, references added, minor corrections; v4: matches final version
published in Phys. Lett.
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