180 research outputs found
CP-odd effective gluonic Lagrangian in Kobayashi-Maskawa model
Schwinger operator method is applied for studying CP-odd pure gluonic
effective Lagrangian in the Standard Model at three-loop level. The induced
-term vanishes by the same reasons as EDMs of quark and W-boson to
two-loop approximation. A simple way is found to demonstrate these
cancellations. All other terms of the effective Lagrangian acquire
non-vanishing contributions. The effective operator of dimension six, Weinberg
operator, is calculated explicitly. The corresponding contribution to the EDM
of neutron is much smaller than that comes from large distances.Comment: Latex, 12 pages, BUDKERINP 94-2
Electric dipole moment of neutron in the Kobayashi-Maskawa model with four generations of quarks
We show that the existence of a possible fourth heavy generation of quarks
gives rise to a significant enhancement to the neutron electric dipole moment
in comparison with the Standard Model prediction. The smaller degree of
suppression in this case is linked to the presence of the operators of
dimension 6 which enter into the effective Lagrangian with coefficients
proportional to the square of the top quark mass. Numerically, the enhancement
is mainly associated with chromoelectric dipole moment of the s quark which
appears at three loop level, of the order \al_s\al_w^2m_sm_t^2/m^4_w from the
CP-odd combination of mixing angles between second, third and fourth
generations. Its value is calculated explicitly in the limit of large masses of
the fourth generation of quarks. The corresponding contribution to the electric
dipole moment of the neutron is in the most
optimistic scenarios about the values of the Kobayashi-Maskawa matrix elements.
The additive renormalization of -term in this model is estimated as
.Comment: 14 pages, LaTex, 5 figures (available upon the request
Probing CP Violation with the Deuteron Electric Dipole Moment
We present an analysis of the electric dipole moment (EDM) of the deuteron as
induced by CP-violating operators of dimension 4, 5 and 6 including theta QCD,
the EDMs and color EDMs of quarks, four-quark interactions and the Weinberg
operator. We demonstrate that the precision goal of the EDM Collaboration's
proposal to search for the deuteron EDM, (1-3)\times 10^{-27} e cm, will
provide an improvement in sensitivity to these sources of one-two orders of
magnitude relative to the existing bounds. We consider in detail the level to
which CP-odd phases can be probed within the MSSM.Comment: 5 pages, 4 figures; precision estimates clarified, to appear in Phys.
Rev.
Radiative corrections to theta term in the left-right supersymmetric models
We calculate the radiative correction to the theta term in the generic
left-right supersymmetric model due to the Kobayashi-Maskawa source of
CP-violation. We found that the value of is very sensitive to
the relations between vacuum expectation values of bidoublet scalars and . The
minimal value of in the model is found to be of order
for , in agreement with the
experimental constraint without an axion mechanism or fine tuning. In other
regions of the parameter space, the radiatively induced gives
unacceptably large contributions to the electric dipole moment of the neutron.Comment: 6 pages, latex, no figure
Can Measurements of Electric Dipole Moments Determine the Seesaw Parameters?
In the context of the supersymmetrized seesaw mechanism embedded in the
Minimal Supersymmetric Standard Model (MSSM), complex neutrino Yukawa couplings
can induce Electric Dipole Moments (EDMs) for the charged leptons, providing an
additional route to seesaw parameters. However, the complex neutrino Yukawa
matrix is not the only possible source of CP violation. Even in the framework
of Constrained MSSM (CMSSM), there are additional sources, usually attributed
to the phases of the trilinear soft supersymmetry breaking couplings and the
mu-term, which contribute not only to the electron EDM but also to the EDMs of
neutron and heavy nuclei. In this work, by combining bounds on various EDMs, we
analyze how the sources of CP violation can be discriminated by the present and
planned EDM experiments.Comment: 26 pages, 9 figures; added reference
Neutron-Electron EDM Correlations in Supersymmetry and Prospects for EDM Searches
Motivated by recent progress in experimental techniques of electric dipole
moment (EDM) measurements, we study correlations between the neutron and
electron EDMs in common supersymmetric models. These include minimal
supergravity (mSUGRA) with small CP phases, mSUGRA with a heavy SUSY spectrum,
the decoupling scenario and split SUSY. In most cases, the electron and neutron
EDMs are found to be observable in the next round of EDM experiments. They
exhibit certain correlation patterns. For example, if d_n ~ 10^{-27} e cm is
found, d_e is predicted to lie in the range 10^{-28}-10^{-29} e cm.Comment: 16 pages,12 figures. To appear in JHEP. A note on stability of the
correlations added in Conclusions; refs. and footnotes adde
Hadronic EDMs, the Weinberg Operator, and Light Gluinos
We re-examine questions concerning the contribution of the three-gluon
Weinberg operator to the electric dipole moment of the neutron, and provide
several QCD sum rule-based arguments that the result is smaller than - but
nevertheless consistent with - estimates which invoke naive dimensional
analysis. We also point out a regime of the MSSM parameter space with light
gluinos for which this operator provides the dominant contribution to the
neutron electric dipole moment due to enhancement via the dimension five color
electric dipole moment of the gluino.Comment: 6 pages, RevTeX, 3 figures; v2: references added; v3: typos
corrected, to appear in Phys. Rev.
Enhancement factor for the electron electric dipole moment in francium and gold atoms
If electrons had an electric dipole moment (EDM) they would induce EDMs of
atoms. The ratio of the atomic EDM to the electron EDM for a particular atom is
called the enhancement factor, R. We calculate the enhancement factor for the
francium and gold atoms, with the results 910 plus/minus 5% for Fr and 260
plus/minus 15% for Au. The large values of these enhancement factors make these
atoms attractive for electron EDM measurements, and hence the search for
time-reversal invariance violation.Comment: 6 pages, no figures, uses RevTex, reference adde
Higgs sector and R-parity breaking couplings in models with broken U(1)_B-L gauge symmetry
Four different supersymmetric models based on SU(2)_L X U(1)_R X U(1)_B-L and
SU(2)_L X SU(2)_R X U(1)_B-L gauge symmetry groups are studied. U(1)_B-L
symmetry is broken spontaneously by a vacuum expectation value (VEV) of a
sneutrino field. The right-handed gauge bosons may obtain their mass solely by
sneutrino VEV. The physical charged lepton and neutrino are mixtures of
gauginos, higgsinos and lepton interaction eigenstates. Explicit formulae for
masses and mixings in the physical lepton fields are found. The spontaneous
symmetry breaking mechanism fixes the trilinear R-parity breaking couplings.
Only some special R-parity breaking trilinear couplings are allowed. There is a
potentially large trilinear lepton number breaking coupling - which is unique
to left-right models - that is proportional to the SU(2)_R gauge coupling g_R.
The couplings are parametrized by few mixing angles, making the spontaneous
R-parity breaking a natural ``unification framework'' for R-parity breaking
couplings in SUSYLR models.Comment: 19 pages, no figures, uses REVTeX. To be published in PR
CP Violation in a Multi-Higgs Doublet Model
We study CP violation in a multi-Higgs doublet model based on a horizontal symmetry. We consider two mechanisms for CP violation in this
model: a) CP violation due to complex Yukawa couplings; and b) CP violation due
to scalar-pseudoscalar mixings. We find that the predictions for
, CP violation in B decays and the electric dipole moments
of neutron and electron are different between these two mechanisms. These
predictions are also dramatically different from the minimal Standard Model
predictions.Comment: 17 pages + one figure, Revtex. Talk presented by Deshpande at the
Conference WHEPP-3, December 199
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