513 research outputs found
Higgs triplets at like-sign linear colliders and neutrino mixing
We study the phenomenology of the type-II seesaw model at a linear e^-e^-
collider. We show that the process e^-e^- \rightarrow alpha^-beta^- (alpha,
beta = e, mu, tau being charged leptons) mediated by a doubly charged scalar is
very sensitive to the neutrino parameters, in particular the absolute neutrino
mass scale and the Majorana CP-violating phases. We identify the regions in
parameter space in which appreciable collider signatures in the channel with
two like-sign muons in the final state are possible. This includes Higgs
triplet masses beyond the reach of the LHC.Comment: 8 pages, 6 figure
Thermal leptogenesis in extended supersymmetric seesaw
We consider an extended supersymmetric SO(10) seesaw model with only doublet
Higgs scalars, in which neutrino masses are suppressed by the scale of D-parity
violation. Leptogenesis can occur at the TeV scale through the decay of a
singlet Sigma, thereby avoiding the gravitino crisis. Washout of the asymmetry
can be effectively suppressed by the absence of direct couplings of Sigma to
leptons.Comment: 4 pages, 5 figure
Causal Inference With Outcome-Dependent Missingness And Self-Censoring
We consider missingness in the context of causal inference when the outcome
of interest may be missing. If the outcome directly affects its own missingness
status, i.e., it is "self-censoring", this may lead to severely biased causal
effect estimates. Miao et al. [2015] proposed the shadow variable method to
correct for bias due to self-censoring; however, verifying the required model
assumptions can be difficult. Here, we propose a test based on a randomized
incentive variable offered to encourage reporting of the outcome that can be
used to verify identification assumptions that are sufficient to correct for
both self-censoring and confounding bias. Concretely, the test confirms whether
a given set of pre-treatment covariates is sufficient to block all backdoor
paths between the treatment and outcome as well as all paths between the
treatment and missingness indicator after conditioning on the outcome. We show
that under these conditions, the causal effect is identified by using the
treatment as a shadow variable, and it leads to an intuitive inverse
probability weighting estimator that uses a product of the treatment and
response weights. We evaluate the efficacy of our test and downstream estimator
via simulations.Comment: 15 pages. In proceedings of the 39th Conference on Uncertainty in
Artificial Intelligenc
Some aspects of radiative corrections and non-decoupling effects of heavy Higgs bosons in two Higgs Doublet Model
The possibility of having relatively large non-decoupling effects of the
heavy Higgs particles within the two-Higgs doublet extension of the electroweak
standard model is briefly discussed and demonstrated on an example of the
one-loop amplitude of the process e^+e^- -> W^+W^-Comment: 6 pages, 3 figures; to appear in the proceedings of the AM2003
conferenc
Higgs coupling constants as a probe of new physics
We study new physics effects on the couplings of weak gauge bosons with the
lightest CP-even Higgs boson (), , and the tri-linear coupling of the
lightest Higgs boson, , at the one loop order, as predicted by the two
Higgs doublet model. Those renormalized coupling constants can deviate from the
Standard Model (SM) predictions due to two distinct origins; the tree level
mixing effect of Higgs bosons and the quantum effect of additional particles in
loop diagrams. The latter can be enhanced in the renormalized coupling
constant when the additional particles show the non-decoupling property.
Therefore, even in the case where the coupling is close to the SM value,
deviation in the coupling from the SM value can become as large as plus
100 percent, while that in the coupling is at most minus 1 percent level.
Such large quantum effect on the Higgs tri-linear coupling is distinguishable
from the tree level mixing effect, and is expected to be detectable at a future
linear collider.Comment: 52 pages, 10 figures, revtex
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Synthesis and properties of lanthanide-exchanged Preyssler`s heteropolyanions
Na{sup +} in the Preyssler heteropolytungstate anion [NaP{sub 5}W{sub 30}O{sub 110}]{sup 14{minus}} can be exchanged for a trivalent lanthanide ion. The potential significance of this new class of lanthanide heteropolyanions relates to their applications in catalysis science. This view follows from the fact that Keggin heteropolyanions and their free acids are used as heterogeneous solid catalysts and homogeneous solution catalysts. The authors describe synthetic conditions that lead to the incorporation of Ce{sup 3+} and Pr{sup 3+} within the Preyssler anion, and the coprecipitation of Ce{sup 3+} and the Preyssler anion. Initial studies indicate that the latter, coprecipitated, material deserves study for bifunctional catalytic activity
Low-Energy Thermal Leptogenesis in an Extended NMSSM Model
Thermal leptogenesis in the canonical seesaw model in supersymmetry suffers
from the incompatibility of a generic lower bound on the mass scale of the
lightest right-handed neutrino and the upper bound on the reheating temperature
of the Universe after inflation. This is resolved by adding an extra singlet
superfield, with a discrete symmetry, to the NMSSM (Next to Minimal
Supersymmetric Standard Model). This generic mechanism is applicable to any
supersymmetric model for lowering the scale of leptogenesis.Comment: 16 pages, revtex, 9 eps figure
The Little Review on Leptogenesis
This is a brief review on the scenario of baryogenesis through leptogenesis.
Leptogenesis is an appealing scenario that may relate the observed baryon
asymmetry in the Universe to the low-energy neutrino data. In this review talk,
particular emphasis is put on recent developments on the field, such as the
flavourdynamics of leptogenesis and resonant leptogenesis near the electroweak
phase transition. It is illustrated how these recent developments enable the
modelling of phenomenologically predictive scenarios that can directly be
tested at the LHC and indirectly in low-energy experiments of lepton-number and
lepton-flavour violation.Comment: 15 pages, based on a plenary presentation given at the DISCRETE'08
Symposium, 11-16 December 2008, Valencia, Spai
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