364 research outputs found
Revealing Randall-Sundrum Hidden Valleys
We study 5D gauge symmetries in the Randall-Sundrum geometry that are hidden
from the standard model through either small 5D gauge coupling, or through
vanishing quantum numbers for the standard model fields. Geometric warping of
5D gravity creates a TeV scale bridge from the standard model to the hidden
sector gauge fields. We apply these concepts to a revival of the electroweak
axion model, in which the dynamics of Peccei-Quinn symmetry breaking occur at
the TeV scale.Comment: 29 pages, 3 figures, 3 table
A viable axion from gauged flavor symmetries
We consider a string inspired non-supersymmetric extension of the standard
model with gauged anomalous U(1) flavor symmetries. Consistency requires the
Green-Schwarz mechanism to cancel mixed anomalies. The additional required
scalars provide Stuckelberg masses for the particles associated to the
gauged flavor symmetry, so they decouple at low energies. Our models also
include a complex scalar field to generate Froggatt-Nielsen mass terms
for light particles giving a partial solution to the fermion mass problem. A
residual approximate (anomalous) global symmetry survives at low energies. The
associated pseudo-Goldstone mode is the phase of the scalar field, and
it becomes the dominant contribution to the physical axion. An effective field
theory analysis that includes neutrino masses gives a prediction for the axion
decay constant. We find a simple modeI where the axion decay constant is in the
center of the allowed window.Comment: 4 pages, 1 figure. v2: Couplings of axions to matter revised, other
minor revision
Constraining the Axion Portal with B -> K l+ l-
We investigate the bounds on axionlike states from flavor-changing neutral
current b->s decays, assuming the axion couples to the standard model through
mixing with the Higgs sector. Such GeV-scale axions have received renewed
attention in connection with observed cosmic ray excesses. We find that
existing B->K l+ l- data impose stringent bounds on the axion decay constant in
the multi-TeV range, relevant for constraining the "axion portal" model of dark
matter. Such bounds also constrain light Higgs scenarios in the next-to-minimal
supersymmetric standard model. These bounds can be improved by dedicated
searches in B-factory data and at LHCb.Comment: 7 pages, 4 figures; v2: to match version to appear in PR
Baryon Asymmetry, Dark Matter and Quantum Chromodynamics
We propose a novel scenario to explain the observed cosmological asymmetry
between matter and antimatter, based on nonperturbative QCD physics. This
scenario relies on a mechanism of separation of quarks and antiquarks in two
coexisting phases at the end of the cosmological QCD phase transition: ordinary
hadrons (and antihadrons), along with massive lumps (and antilumps) of novel
color superconducting phase. The latter would serve as the cosmological cold
dark matter. In certain conditions the separation of charge is C and CP
asymmetric and can leave a net excess of hadrons over antihadrons in the
conventional phase, even if the visible universe is globally baryon symmetric
. In this case an equal, but negative, overall baryon charge must be
hidden in the lumps of novel phase. Due to the small volume occupied by these
dense lumps/antilumps of color superconducting phase and the specific features
of their interaction with "normal" matter in hadronic phase, this scenario does
not contradict the current phenomenological constrains on presence of
antimatter in the visible universe. Moreover, in this scenario the observed
cosmological ratio within an order of magnitude
finds a natural explanation, as both contributions to originated from
the same physics during the QCD phase transition. The baryon to entropy ratio
would also be a natural outcome, fixed by the
temperature T_f \simlt T_{QCD} at which the separation of phases is
completed.Comment: New paragraph added in subsection II.D; version to appear in Physical
Review
Open string axions and the flavor problem
We consider extensions of the standard model inspired by intersecting D-brane
constructions, in order to address flavor mass textures. We include additional
anomalous gauge symmetries, and scalar fields to break them and to generate
Froggatt-Nielsen mass terms. Green-Schwarz axions are included to cancel mixed
anomalies rendering the models consistent. At low energies, a residual
anomalous global symmetry remains, and its associated pseudo-Goldstone mode
becomes the physical axion, which can be interpreted as an axion arising from
open string modes. General considerations show that such axions are very common
in D-brane models and can be completely incompatible with current bounds.
Astrophysical constraints are placed on the axion both by including neutrino
masses in the Froggatt-Nielsen scheme and considering QCD instanton
contributions to the axion mass. We find simple models where the axion decay
constant is in the allowed range, but only one such minimal model with this
property is free from excessive fine tunings elsewhere. We also note that
generically addressing flavor textures for the CKM matrix leads to
deconstructed extra dimensions.Comment: 30 pages, 2 figures. v2: references added. v3:typos fixe
Slow nucleation rates in Chain Inflation with QCD Axions or Monodromy
The previous proposal (by two of us) of chain inflation with the QCD axion is
shown to fail. The proposal involved a series of fast tunneling events, yet
here it is shown that tunneling is too slow. We calculate the bubble nucleation
rates for phase transitions in the thick wall limit, approximating the barrier
by a triangle. A similar problem arises in realization of chain inflation in
the string landscape that uses series of minima along the monodromy staircase
around the conifold point. The basic problem is that the minima of the
potential are too far apart to allow rapid enough tunneling in these two
models. We entertain the possibility of overcoming this problem by modifying
the gravity sector to a Brans-Dicke theory. However, one would need extremely
small values for the Brans-Dicke parameter. Many successful alternatives exist,
including other "axions" (with mass scales not set by QCD) or potentials with
comparable heights and widths that do not suffer from the problem of slow
tunneling and provide successful candidates for chain inflation.Comment: 6 pages, 1 figur
Anomalous Axion Interactions and Topological Currents in Dense Matter
Recently an effective Lagrangian for the interactions of photons,
Nambu-Goldstone bosons and superfluid phonons in dense quark matter has been
derived using anomaly matching arguments. In this paper we illuminate the
nature of certain anomalous terms in this Lagrangian by an explicit microscopic
calculation. We also generalize the corresponding construction to introduce the
axion field. We derive an anomalous axion effective Lagrangian describing the
interactions of axions with photons and superfluid phonons in the dense matter
background. This effective Lagrangian, among other things, implies that an
axion current will be induced in the presence of magnetic field. We speculate
that this current may be responsible for the explanation of neutron star kicks.Comment: 10 page
Inflation from a Supersymmetric Axion Model
We show that a supersymmetric axion model naturally induces a hybrid
inflation with the waterfall field identified as a Peccei-Quinn scalar. The
Peccei-Quinn scale is predicted to be around 10^{15}GeV for reproducing the
large-scale density perturbation of the Universe. After the built-in late-time
entropy-production process, the axion becomes a dark matter candidate. Several
cosmological implications are discussed.Comment: 5 pages; to appear in PR
Odd Decays from Even Anomalies: Gauge Mediation Signatures Without SUSY
We analyze the theory and phenomenology of anomalous global chiral symmetries
in the presence of an extra dimension. We propose a simple extension of the
Standard Model in 5D whose signatures closely resemble those of supersymmetry
with gauge mediation, and we suggest a novel scalar dark matter candidate.Comment: 26 pages, 1 figure; v2: references added; discussion of direct
collider constraints added; v3: corrected dark matter calculation in chapter
4.2 and replaced figure 1
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