764 research outputs found
Comments on the Holographic Picture of the Randall-Sundrum Model
We discuss some issues about the holographic interpretation of the compact
Randall-Sundrum model, which is conjectured to be dual to a 4d field theory
with non-linearly realized conformal symmetry. We make several checks of this
conjecture. In particular, we show that the radion couples conformally to a
background 4d metric. We also discuss the interpretation of the Goldberger-Wise
mechanism for stabilizing the radion. We consider situations where the
electroweak breaking stabilizes the radion and we discuss the issue of natural
conservation of flavor quantum numbers.Comment: misprints corrected, references adde
Soft Supersymmetry Breaking in Deformed Moduli Spaces, Conformal Theories, and N = 2 Yang-Mills Theory
We give a self-contained discussion of recent progress in computing the
non-perturbative effects of small non-holomorphic soft supersymmetry breaking,
including a simple new derivation of these results based on an anomaly-free
gauged U(1)_R background. We apply these results to N = 1 theories with
deformed moduli spaces and conformal fixed points. In an SU(2) theory with a
deformed moduli space, we completely determine the vacuum expectation values
and induced soft masses. We then consider the most general soft breaking of
supersymmetry in N = 2 SU(2) super-Yang-Mills theory. An N = 2 superfield
spurion analysis is used to give an elementary derivation of the relation
between the modulus and the prepotential in the effective theory. This analysis
also allows us to determine the non-perturbative effects of all soft terms
except a non-holomorphic scalar mass, away from the monopole points. We then
use an N = 1 spurion analysis to determine the effects of the most general soft
breaking, and also analyze the monopole points. We show that naive dimensional
analysis works perfectly. Also, a soft mass for the scalar in this theory
forces the theory into a free Coulomb phase.Comment: 37 pages, LaTeX2e, 4 eps figure
The Fate of the Radion in Models with Metastable Graviton
We clarify some general issues in models where gravity is localized at
intermediate distances. We introduce the radion mode, which is usually
neglected, and we point out that its role in the model is crucial. We show that
the brane bending effects discussed in the literature can be obtained in a
formalism where the physical origin is manifest. The model violates positivity
of energy due to a negative tension brane, which induces a negative kinetic
term for the radion. The very same effect that violates positivity is
responsible for the recovery of conventional Einstein gravity at intermediate
distances.Comment: Latex file, 13 page
Graviton loops and brane observables
We discuss how to consistently perform effective Lagrangian computations in
quantum gravity with branes in compact extra dimensions. A reparametrization
invariant and infrared finite result is obtained in a non trivial way. It is
crucial to properly account for brane fluctuations and to correctly identify
physical observables. Our results correct some confusing claims in the
literature. We discuss the implications of graviton loops on electroweak
precision observables and on the muon g-2 in models with large extra
dimensions. We model the leading effects, not controlled by effective field
theory, by introducing a hard momentum cut-off.Comment: 9 pages + 4 eps figures, JHEP style latex document. The paper is
composed by a theoretical part, followed (after page 21) by a
phenomenological part. v2: version published in JHEP, few typos corrected.
v3: few additional typos corrected in the Appendi
Central Charge Bounds in 4D Conformal Field Theory
We derive model-independent lower bounds on the stress tensor central charge
C_T in terms of the operator content of a 4-dimensional Conformal Field Theory.
More precisely, C_T is bounded from below by a universal function of the
dimensions of the lowest and second-lowest scalars present in the CFT. The
method uses the crossing symmetry constraint of the 4-point function, analyzed
by means of the conformal block decomposition.Comment: 16 pages, 6 figure
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
Gaugino Mass without Singlets
In models with dynamical supersymmetry breaking in the hidden sector, the
gaugino masses in the observable sector have been believed to be extremely
suppressed (below 1 keV), unless there is a gauge singlet in the hidden sector
with specific couplings to the observable sector gauge multiplets. We point out
that there is a pure supergravity contribution to gaugino masses at the quantum
level arising from the superconformal anomaly. Our results are valid to all
orders in perturbation theory and are related to the `exact' beta functions for
soft terms. There is also an anomaly contribution to the A terms proportional
to the beta function of the corresponding Yukawa coupling. The gaugino masses
are proportional to the corresponding gauge beta functions, and so do not
satisfy the usual GUT relations.Comment: 25 pages, references added, typos and grammar correcte
Supersymmetry-Breaking Loops from Analytic Continuation into Superspace
We extend to all orders in perturbation theory a method to calculate
supersymmetry-breaking effects by analytic continuation of the renormalization
group into superspace. A central observation is that the renormalized gauge
coupling can be extended to a real vector superfield, thereby including soft
breaking effects in the gauge sector. We explain the relation between this
vector superfield coupling and the "holomorphic" gauge coupling, which is a
chiral superfield running only at 1 loop. We consider these issues for a number
of regulators, including dimensional reduction. With this method, the
renormalization group equations for soft supersymmetry breaking terms are
directly related to supersymmetric beta functions and anomalous dimensions to
all orders in perturbation theory. However, the real power of the formalism
lies in computing finite soft breaking effects corresponding to high-loop
component calculations. We prove that the gaugino mass in gauge-mediated
supersymmetry breaking is ``screened'' from strong interactions in the
messenger sector. We present the complete next-to-leading calculation of
gaugino masses (2 loops) and sfermion masses (3 loops) in minimal gauge
mediation, and several other calculations of phenomenological relevance.Comment: 50 pages, 1 ps and 1 eps figure, LaTe
Classical and Quantum Consistency of the DGP Model
We study the Dvali-Gabadadze-Porrati model by the method of the boundary
effective action. The truncation of this action to the bending mode \pi
consistently describes physics in a wide range of regimes both at the classical
and at the quantum level. The Vainshtein effect, which restores agreement with
precise tests of general relativity, follows straightforwardly. We give a
simple and general proof of stability, i.e. absence of ghosts in the
fluctuations, valid for most of the relevant cases, like for instance the
spherical source in asymptotically flat space. However we confirm that around
certain interesting self-accelerating cosmological solutions there is a ghost.
We consider the issue of quantum corrections. Around flat space \pi becomes
strongly coupled below a macroscopic length of 1000 km, thus impairing the
predictivity of the model. Indeed the tower of higher dimensional operators
which is expected by a generic UV completion of the model limits predictivity
at even larger length scales. We outline a non-generic but consistent choice of
counterterms for which this disaster does not happen and for which the model
remains calculable and successful in all the astrophysical situations of
interest. By this choice, the extrinsic curvature K_{\mu\nu} acts roughly like
a dilaton field controlling the strength of the interaction and the cut-off
scale at each space-time point. At the surface of Earth the cutoff is \sim 1 cm
but it is unlikely that the associated quantum effects be observable in table
top experiments.Comment: 26 pages, 1 eps figur
Strong Conformal Dynamics at the LHC and on the Lattice
Conformal technicolor is a paradigm for new physics at LHC that may solve the
problems of strong electroweak symmetry breaking for quark masses and precision
electroweak data. We give explicit examples of conformal technicolor theories
based on a QCD-like sector. We suggest a practical method to test the conformal
dynamics of these theories on the lattice.Comment: v2: Generalized discussion of lattice measurement of hadron masses,
references added, minor clarifications v3: references added, minor change
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