45 research outputs found
Constraints on Quartic Vector-Boson Interactions from Z Physics
We obtain the constraints on possible anomalous quartic vector-boson vertices
arising from the precision measurements at the pole. In the framework of
chiral Lagrangians, we examine all effective operators
of order that lead to four-gauge-boson interactions but do not induce
anomalous trilinear vertices. We constrain the anomalous quartic interactions
by evaluating their one-loop corrections to the pole physics. Our analysis
is performed in a generic gauge and it shows that only the operators
that break the custodial symmetry get limits close to the theoretical
expectations. Our results also indicate that these anomalous couplings are
already out of reach of the Next Linear Collider, while the Large
Hadron Collider could be able to further extend the bounds on some of these
couplings.Comment: 16 pages, 1 Postscript figures, uses RevTex and eps.st
Bosonic Quartic Couplings at LHC
We analyze the potential of the CERN Large Hadron Collider (LHC) to study
anomalous quartic vector-boson interactions Z Z gamma gamma, Z Z Z gamma, W+ W-
gamma gamma, and W+ W- Z gamma through the weak boson fusion processes q q -> q
q gamma gamma and q q -> q q gamma Z(-> l+ l-) with l = electron or muon. After
a careful study of the backgrounds and how to extract them from the data, we
show that the process p p -> j j gamma l+ l- is potentially the most sensitive
to deviations from the Standard Model, improving the sensitivity to anomalous
couplings by up to a factor 10^4 (10^2) with respect to the present direct
(indirect) limits.Comment: 18 pages, 2 figures, revised versio
Tests of Anomalous Quartic Couplings at the NLC
We analyze the potential of the Next Linear Collider to study
anomalous quartic vector-boson interactions through the processes and . In the framework of chiral
Lagrangians, we examine all effective operators of order that lead to
four-gauge-boson interactions but do not induce anomalous trilinear vertices.
In our analysis, we take into account the decay of the vector bosons to
fermions and evaluate the efficiency in their reconstruction. We obtain the
bounds that can be placed on the anomalous quartic interactions and we study
the strategies to distinguish the possible couplings.Comment: 18 pages, ReVTeX, 3 figures, typos corrected and references adde
Soft lepton-flavor violation in a multi-Higgs-doublet seesaw model
We consider the Standard Model with an arbitrary number n_H of Higgs doublets
and enlarge the lepton sector by adding to each lepton family \ell a
right-handed neutrino singlet \nu_{\ell R}. We assume that all Yukawa-coupling
matrices are diagonal, but the Majorana mass matrix M_R of the right-handed
neutrino singlets is an arbitrary symmetric matrix, thereby introducing an
explicit but soft violation of all lepton numbers. We investigate
lepton-flavor-violating processes within this model. We pay particular
attention to the large-m_R behavior of the amplitudes for these processes,
where m_R is the order of magnitude of the matrix elements of M_R. While the
amplitudes for processes like tau^- --> mu^- gamma and Z --> tau^+ mu^- drop as
1/m_R^2 for arbitrary n_H, processes like tau^- --> mu^- e^+ e^- and mu^- -->
e^- e^+ e^- obey this power law only for n_H = 1. For n_H \geq 2, on the
contrary, those amplitudes do not fall off when m_R increases, rather they
converge towards constants. This non-decoupling of the right-handed scale
occurs because of the sub-process ell^- --> ell'^- {S_b^0}^*, where S_b^0 is a
neutral scalar which subsequently decays to e^+ e^-. That sub-process has a
contribution from charged-scalar exchange which, for n_H \geq 2, does not
decrease when m_R tends to infinity. We also perform a general study of the
non-decoupling and argue that, after performing the limit m_R --> \infty and
removing the \nu_R from the Lagrangian, our model becomes a multi-Higgs-doublet
Standard Model with suppressed flavor-changing Yukawa couplings. Finally, we
show that, with the usual assumptions about the mass scales in the seesaw
mechanism, the branching ratios of all lepton-flavor-changing processes are
several orders of magnitude smaller than present experimental limits.Comment: 46 pages, 2 figures, Revte
One-Loop Calculation of the Oblique S Parameter in Higgsless Electroweak Models
We present a one-loop calculation of the oblique S parameter within Higgsless
models of electroweak symmetry breaking and analyze the phenomenological
implications of the available electroweak precision data. We use the most
general effective Lagrangian with at most two derivatives, implementing the
chiral symmetry breaking SU(2)_L x SU(2)_R -> SU(2)_{L+R} with Goldstones,
gauge bosons and one multiplet of vector and axial-vector massive resonance
states. Using the dispersive representation of Peskin and Takeuchi and imposing
the short-distance constraints dictated by the operator product expansion, we
obtain S at the NLO in terms of a few resonance parameters. In
asymptotically-free gauge theories, the final result only depends on the
vector-resonance mass and requires M_V > 1.8 TeV (3.8 TeV) to satisfy the
experimental limits at the 3 \sigma (1\sigma) level; the axial state is always
heavier, we obtain M_A > 2.5 TeV (6.6 TeV) at 3\sigma (1\sigma). In
strongly-coupled models, such as walking or conformal technicolour, where the
second Weinberg sum rule does not apply, the vector and axial couplings are not
determined by the short-distance constraints; but one can still derive a lower
bound on S, provided the hierarchy M_V < M_A remains valid. Even in this less
constrained situation, we find that in order to satisfy the experimental limits
at 3\sigma one needs M_{V,A} > 1.8 TeV.Comment: 34 pages, 9 figures. Version published in JHEP. Some references and
sentences have been added to facilitate the discussio
Strongly Interacting Vector Bosons at the LHC: Quartic Anomalous Couplings
We analyze the potential of the CERN Large Hadron Collider to study anomalous
quartic vector--boson interactions through the production of vector--boson
pairs accompanied by jets. In the framework of chiral
Lagrangians, we examine all effective operators of order that lead to new
four--gauge--boson interactions but do not alter trilinear vertices. In our
analyses, we perform the full tree level calculation of the processes leading
to two jets plus vector--boson pairs, , , , or
, taking properly into account the interference between the standard model
and the anomalous contributions. We obtain the bounds that can be placed on the
anomalous quartic interactions and we study the strategies to distinguish the
possible new couplings.Comment: 12 pages, ReVTeX, 5 figure
Virtual Effects of Split SUSY in Higgs Productions at Linear Colliders
In split supersymmetry the gauginos and higgsinos are the only supersymmetric
particles possibly accessible at foreseeable colliders like the CERN Large
Hadron Collider (LHC) and the International Linear Collider (ILC). In order to
account for the cosmic dark matter measured by WMAP, these gauginos and
higgsinos are stringently constrained and could be explored at the colliders
through their direct productions and/or virtual effects in some processes. The
clean environment and high luminosity of the ILC render the virtual effects of
percent level meaningful in unraveling the new physics effects. In this work we
assume split supersymmetry and calculate the virtual effects of the
WMAP-allowed gauginos and higgsinos in Higgs productions e+e- -> Z h and e+e-
-> \nu_e \bar_\nu_e h through WW fusion at the ILC. We find that the production
cross section of e+e- -> Zh can be altered by a few percent in some part of the
WMAP-allowed parameter space, while the correction to the WW-fusion process
e+e- -> \nu_e \bar_\nu_e h is below 1%. Such virtual effects are correlated
with the cross sections of chargino pair productions and can offer
complementary information in probing split supersymmetry at the colliders.Comment: more discussions added (7 pages, 10 figs
Thermodynamic analysis of black hole solutions in gravitating nonlinear electrodynamics
We perform a general study of the thermodynamic properties of static
electrically charged black hole solutions of nonlinear electrodynamics
minimally coupled to gravitation in three space dimensions. The Lagrangian
densities governing the dynamics of these models in flat space are defined as
arbitrary functions of the gauge field invariants, constrained by some
requirements for physical admissibility. The exhaustive classification of these
theories in flat space, in terms of the behaviour of the Lagrangian densities
in vacuum and on the boundary of their domain of definition, defines twelve
families of admissible models. When these models are coupled to gravity, the
flat space classification leads to a complete characterization of the
associated sets of gravitating electrostatic spherically symmetric solutions by
their central and asymptotic behaviours. We focus on nine of these families,
which support asymptotically Schwarzschild-like black hole configurations, for
which the thermodynamic analysis is possible and pertinent. In this way, the
thermodynamic laws are extended to the sets of black hole solutions of these
families, for which the generic behaviours of the relevant state variables are
classified and thoroughly analyzed in terms of the aforementioned boundary
properties of the Lagrangians. Moreover, we find universal scaling laws (which
hold and are the same for all the black hole solutions of models belonging to
any of the nine families) running the thermodynamic variables with the electric
charge and the horizon radius. These scale transformations form a one-parameter
multiplicative group, leading to universal "renormalization group"-like
first-order differential equations. The beams of characteristics of these
equations generate the full set of black hole states associated to any of these
gravitating nonlinear electrodynamics...Comment: 51 single column pages, 19 postscript figures, 2 tables, GRG tex
style; minor corrections added; final version appearing in General Relativity
and Gravitatio
Search for new phenomena in monophoton final states in proton-proton collisions at root s=8 TeV
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