10,945 research outputs found
Is the Top Quark Really Heavier than the Boson?
Scalar induced top decays may drastically suppress
and still hide the top below . The collider experiments should
enlarge the scope and study the plane. Specific model
signatures such as (multiple high -jets) and
, (with $B(t\to b\tau\nu) \
\raisebox{-.5ex}{\rlap{}} \raisebox{.4ex}{}\ 1/3t^\primeb^\prime$ quark,
while top quark and toponium physics could still turn up at LEP-II.Comment: 11 pages (RevTex), 3 figures (not included), NTUTH-93-0
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.
Highlights from Five Years at the B Factories
The highlights and conflicts at the B Factories are briefly reviewed.
violation was established in 2001 in and related modes,
which has now become a precision measurement of CP violation in - mixing. However, the situation for the and charmless
modes, which probe also CP violation in the {\it decay} amplitude, are
not quite settled yet. They could be hinting at presence of both strong (CP
conserving) and new physics (CP violating) phases. We critically assess the
developments and discuss some related discrepancies and highlights, such as
observation of direct CP violation, and make a projection towards the next few
years.Comment: 16 pages, 5 figures, to appear as Brief Review in Mod. Phys. Lett.
Real-time lattice boltzmann shallow waters method for breaking wave simulations
We present a new approach for the simulation of surfacebased fluids based in a hybrid formulation of Lattice Boltzmann Method for Shallow Waters and particle systems. The modified LBM can handle arbitrary underlying terrain conditions and arbitrary fluid depth. It also introduces a novel method for tracking dry-wet regions and moving boundaries. Dynamic rigid bodies are also included in our simulations using a two-way coupling. Certain features of the simulation that the LBM can not handle because of its heightfield nature, as breaking waves, are detected and automatically turned into splash particles. Here we use a ballistic particle system, but our hybrid method can handle more complex systems as SPH. Both the LBM and particle systems are implemented in CUDA, although dynamic rigid bodies are simulated in CPU. We show the effectiveness of our method with various examples which achieve real-time on consumer-level hardware.Peer ReviewedPostprint (author's final draft
Window on Higgs Boson: Fourth Generation Decays Revisited
Direct and indirect searches of the Higgs boson suggest that 113 GeV
170 GeV is likely. With the LEP era over and the
Tevatron Run II search via arduous, we revisit a case where
or jets could arise via strong pair
production. In contrast to 10 years ago, the tight electroweak constraint on
-- (hence --) splitting reduces FCNC
, rates, making naturally competitive.
Such a "cocktail solution" is precisely the mix that could evade the CDF search
for , and the may well be lurking below the top. In
light of the Higgs program, this two-in-one strategy should be pursued.Comment: 4 pages, RevTex, 4 eps figures, One more figure, version to be
published in Phys. Rev.
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
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