14 research outputs found
Gluon Fusion: A Probe of Higgs Sector CP Violation
We demonstrate that CP violation in the Higgs sector, \eg\ of a multi-doublet
model, can be directly probed using gluon-gluon collisions at the SSC. %
requires phyzzx.tex macro packageComment: UCD-93-
Probing Top-Quark Couplings at Polarized NLC
The energy spectrum of the lepton(s) in e^+e^- --> tt-bar --> l^{+-}
...../l^+l^-..... at next linear colliders (NLC) is studied for arbitrary
longitudinal beam polarizations as a possible test of new physics in top-quark
couplings. The most general non-standard couplings for gamma-tt-bar, Ztt-bar
and Wtb vertices are considered. Expected precision of the
non-standard-parameter determination is estimated applying the
optimal-observable procedure.Comment: Final version, To appear in Phys. Rev.
CP-Violation in Bosonic Sector of SM with two Higgs Doublets
We investigate CP-violation effects in the bosonic sector of the Standard
Model (SM) with two Higgs doublets. First we calculate the mass eigenstates of
the physical neutral Higgses for small but nonzero CP-violation parameter
, and then a ``forward-backward'' asymmetry for the
decay that would be a signal of CP-violation. Although the
effects are in general small (), turns out to be a rather clean signal of
CP-violation, since neither the CP-conserving final state interactions nor the
direct production background events contribute to . The process is
a counterexample to the widespread belief that CP-violation processes must
involve fermions. The CKM-type CP-violation effects that could in principle
also contribute to are negligible. The nonzero
could possibly be detected at some later stage in future colliders such as LHC
or SSC.Comment: 11 pages (standard LaTeX), 3 figures (available from the author),
DO-TH 93-1
Direct CP Violation in Angular Distribution of Decays
We show that the study of certain observables in the angular distribution in
provide clear test for CP vioaltion beyond the Standard
Model. These observables vanish in SM, but in models beyond SM some of them can
be large enough to be measured at B factories.Comment: 7 pages, Revte
Prospects for Direct CP Violaton in Exclusive and Inclusive Charmless B decays
Within the Standard Model, CP rate asymmetries for could
reach 10%. With strong final state phases, they could go up to 20--30%, even
for mode which would have opposite sign. We can account for
, and rate data with new physics enhanced
color dipole coupling and destructive interference. Asymmetries could reach
40--60% for and modes and are all of the same sign. We are
unable to account for rate. Our inclusive study supports our
exclusive results.Comment: Minor changes, correct a small bug in Fig. 1(b). Version to appear in
Phys. Rev. Let
Final-State-Interaction Simulation of T-Violation in the Top-Quark Semileptonic Decay
The standard electroweak final-state interaction induces a false T-odd
correlation in the top-quark semileptonic decay. The correlation parameter is
calculated in the standard model and found to be considerably larger than those
that could be produced by genuine T-violation effects in a large class of
theoretical models.Comment: 14 pages, 1 diagram (not included
Enhanced Decay, Inclusive Production, and the Gluon Anomaly
The experimental hint of large is linked to the
penguins via the gluon anomaly. Using running in the
-- coupling, the standard penguin alone seems
insufficient, calling for the need of dipole at 10% level from new
physics, which could also resolve the and charm counting
problems. The intereference of standard and new physics contributions may
result in direct CP asymmetries at 10% level, which could be observed soon at B
Factories.Comment: 12 pages, revtex, 3 figs. (version to appear in Phys. Rev. Lett.
Optimal Spin Basis in Polarized Photon Linear Colliders
We analyze the spin correlations of the top quark pairs produced at Photon
Linear Colliders. We employ the circular polarized photon beams and general
spin basis for the top quark pair. We consider general spin bases to find a
strong spin correlation between produced top quark and anti-top quark. We show
the cross-section in these bases and discuss the characteristics of results.Comment: RevTeX, 16 pages, 6 figures, psfig.sty and here.sty are require
R-parity violation and uses of the rare decay sneutrino-->gamma+gamma in hadron and photon colliders
We consider implications of the loop process sneutrino -> gamma gamma in the
MSSM with R-parity violation for future experiments, where the sneutrino is
produced as the only supersymmetric particle. We present a scenario for the
R-parity violating couplings, where this clean decay, although rare with
Br(sneutrino -> gamma gamma) ~ 10^{-6}, may be useful for sneutrino detection
over a range of sneutrino masses at the LHC. Furthermore, the new
sneutrino-gamma-gamma effective coupling may induce detectable sneutrino
resonant production in gamma gamma collisions, over a considerably wide mass
range. We compare sneutrino -> gamma gamma, gg throughout the paper with the
analogous yet quantitatively very different, Higgs -> gamma gamma, gg decays
and comment on the loop processes sneutrino -> WW, ZZ.Comment: 19 pages using REVTEX, 3 figures embadded in the text using epsfi
Improving constraints on tan(beta)/m_H using B \to D tau \bar{nu}
We study the q^2 dependence of the exclusive decay mode B \to D tau \bar{nu}
in type II two Higgs doublet models and show that this mode may be used to put
stringent bounds on tan(beta)/m_H. There are currently rather large theoretical
uncertainties in the q^2 distribution, but these may be significantly reduced
by future measurements of the analogous distribution for B \to D(e,mu)\bar{nu}.
We estimate that this reduction in the theoretical uncertainties would
eventually (i.e., with sufficient data) allow one to push the upper bound on
tan(beta)/m_H down to about 0.06 GeV^{-1}. This would represent an improvement
on the current bound by about a factor of 7. We then apply the method of
optimized observables which allows us to estimate the reach of an experiment
with a given number of events. We thus find that an experiment with, for
example, 10^3 events could set a 2\sigma upper bound on tan(beta)/m_H of 0.07
GeV^{-1} or could differentiate at the 4.6\sigma level between a 2HDM with
tan(beta)/m_H = 0.1 GeV^{-1} and the SM.Comment: 19 pages, Late