828 research outputs found
Electroweak and Flavor Physics in Extensions of the Standard Model with Large Extra Dimensions
We study the implications of extra dimensions of size on
electroweak and flavor physics due to the presence of Kaluza-Klein excitations
of the SM gauge-bosons. We consider several scenarios with the SM fermions
either living in the bulk or being localized at different points of an extra
dimension. Global fits to electroweak observables provide lower bounds on 1/R,
which are generically in the 2-5 TeV range. We find, however, certain models
where the fit to electroweak observables is better than in the SM, because of
an improvement in the prediction to the weak charge Q_W. We also consider the
case of softly-broken supersymmetric theories and we find new non-decoupling
effects that put new constraints on 1/R. If quarks of different families live
in different points of the extra dimension, we find that the Kaluza-Klein modes
of the SM gluons generate (at tree level) dangerous flavor and CP-violating
interactions. The lower bounds on 1/R can increase in this case up to 5000 TeV,
disfavoring these scenarios in the context of TeV-strings.Comment: 21 pages, 3 figures, Late
The -Problem in Theories with Gauge-Mediated Supersymmetry Breaking
We point out that the -problem in theories in which supersymmetry
breaking is communicated to the observable sector by gauge interactions is more
severe than the one encountered in the conventional gravity-mediated scenarios.
The difficulty is that once is generated by a one-loop diagram, then
usually \bmu is also generated at the same loop order. This leads to the
problematic relation \bmu \sim \mu \Lambda, where 10--100 TeV
is the effective supersymmetry-breaking scale. We present a class of theories
for which this problem is naturally solved. Here, without any fine tuning among
parameters, is generated at one loop, while \bmu arises only at the
two-loop level. This mechanism can naturally lead to an interpretation of the
Higgs doublets as pseudo-Goldstone bosons of an approximate global symmetry.Comment: 18 pages, 2 figure
Non-supersymmetric extensions of the SM
We discuss the implications of having the Higgs particle arising as a composite pseudo-Goldstone boson, either from a new strong interacting sector at the TeV, or from the 5th-component of a gauge field in extra dimensional models
One-loop non-renormalization results in EFTs
In Effective Field Theories (EFTs) with higher-dimensional operators many
anomalous dimensions vanish at the one-loop level for no apparent reason. With
the use of supersymmetry, and a classification of the operators according to
their embedding in super-operators, we are able to show why many of these
anomalous dimensions are zero. The key observation is that one-loop
contributions from superpartners trivially vanish in many cases under
consideration, making supersymmetry a powerful tool even for non-supersymmetric
models. We show this in detail in a simple U(1) model with a scalar and
fermions, and explain how to extend this to SM EFTs and the QCD Chiral
Langrangian. This provides an understanding of why most "current-current"
operators do not renormalize "loop" operators at the one-loop level, and allows
to find the few exceptions to this ubiquitous rule.Comment: Corrections made in Sec. 3.2 and Fig.
The Strongly-Interacting Light Higgs
We develop a simple description of models where electroweak symmetry breaking
is triggered by a light composite Higgs, which emerges from a
strongly-interacting sector as a pseudo-Goldstone boson. Two parameters broadly
characterize these models: m_rho, the mass scale of the new resonances and
g_rho, their coupling. An effective low-energy Lagrangian approach proves to be
useful for LHC and ILC phenomenology below the scale m_rho. We identify two
classes of operators: those that are genuinely sensitive to the new strong
force and those that are sensitive to the spectrum of the resonances only.
Phenomenological prospects for the LHC and the ILC include the study of
high-energy longitudinal vector boson scattering, strong double-Higgs
production and anomalous Higgs couplings. We finally discuss the possibility
that the top quark could also be a composite object of the strong sector.Comment: 45 pages, 1 figure. v2: references adde
Renormalization of dimension-six operators relevant for the Higgs decays
The discovery of the Higgs boson has opened a new window to test the SM
through the measurements of its couplings. Of particular interest is the
measured Higgs coupling to photons which arises in the SM at the one-loop
level, and can then be significantly affected by new physics. We calculate the
one-loop renormalization of the dimension-six operators relevant for
, which can be potentially important since
it could, in principle, give log-enhanced contributions from operator mixing.
We find however that there is no mixing from any current-current operator that
could lead to this log-enhanced effect. We show how the right choice of
operator basis can make this calculation simple. We then conclude that
can only be affected by RG mixing from
operators whose Wilson coefficients are expected to be of one-loop size, among
them fermion dipole-moment operators which we have also included.Comment: 21 pages. Improved version with h -> gamma Z results added and
structure of anomalous-dimension matrix determined further. Conclusions
unchange
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