Articles
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07/14/1999--
07/14/1999
Phenomenology of V_ub from Ratios of Inclusive B Decay Rates
We explore the theoretical feasibility of extracting V_ub from two ratios
built from B meson inclusive partial decays,
R_1 = Gamma(b-> u cbar s)/3Gamma(b -> c l nu), and
R_2 = [Gamma(b -> c X) - Gamma(b -> cbar X)]/Gamma(b -> c ubar d).
We discuss contributions to these quantities from perturbative and
nonperturbative physics, and show that they can be computed with overall
uncertainties at the level of 10%.
02/08/1999--
03/05/1998
A molecular-dynamics study of ductile and brittle fracture in model non-crystalline solids
Molecular-dynamics simulations of fracture in metallic glass-like systems are
observed to undergo embrittlement due to a small change in interatomic
potential. This change in fracture toughness, however, is not accompanied by a
corresponding change in flow stress. Theories of brittle fracture proposed by
Freund and Hutchinson indicate that strain rate sensitivity is the controling
physical parameter in these cases. A recent theory of viscoplasticity in this
class of solids by Falk and Langer further suggests that the change in strain
rate sensitivity corresponds to a change in the susceptibility of local shear
transformation zones to applied shear stresses. A simple model of these zones
is develped in order to quantify the dependence of this sensitivity on the
interparticle potential.
10/02/2017--
10/02/2017
Global Brain Dynamics During Social Exclusion Predict Subsequent Behavioral Conformity
Individuals react differently to social experiences; for example, people who
are more sensitive to negative social experiences, such as being excluded, may
be more likely to adapt their behavior to fit in with others. We examined
whether functional brain connectivity during social exclusion in the fMRI
scanner can be used to predict subsequent conformity to peer norms. Adolescent
males (N = 57) completed a two-part study on teen driving risk: a social
exclusion task (Cyberball) during an fMRI session and a subsequent driving
simulator session in which they drove alone and in the presence of a peer who
expressed risk-averse or risk-accepting driving norms. We computed the
difference in functional connectivity between social exclusion and social
inclusion from each node in the brain to nodes in two brain networks, one
previously associated with mentalizing (medial prefrontal cortex,
temporoparietal junction, precuneus, temporal poles) and another with social
pain (anterior cingulate cortex, anterior insula). Using cross-validated
machine learning, this measure of global network connectivity during exclusion
predicts the extent of conformity to peer pressure during driving in the
subsequent experimental session. These findings extend our understanding of how
global neural dynamics guide social behavior, revealing functional network
activity that captures individual differences.
10/20/1994--
10/18/1994
Possible Puzzles in Nonleptonic B Decays
I discuss the recent controversy over the semileptonic branching ratio of the
$B$ meson, pointing out that it is only the combination of this quantity with
the reported charm multiplicity in $B$ decays which is in serious conflict with
theoretical calculations. I consider possible solutions to the problem.
(Invited talk presented at the Eighteenth Johns Hopkins Workshop on Current
Problems in Particle Theory, Florence, Italy, August 31--September 2, 1994.)
06/30/1998--
06/30/1998
Final State Interactions in Hadronic B Decays
I discuss the effect of final state interactions on the determination of the
CKM angle \gamma from B -> K + pi decays. Using a simple Regge-based model for
rescattering processes, I argue that such effects could be substantial enough
to make it problematic to obtain reliable limits on \gamma in this way.
Fortunately, an analysis of B -> K + K decays may provide model-independent
bounds on rescattering contributions.
11/10/1999--
03/29/1999
Measuring V_ub in Inclusive B Decays to Charm
We propose a novel method of measuring the CKM matrix element V_ub, via
inclusive B decays to "wrong sign" charm. This process is mediated by the quark
level decay b -> u cbar s'. When normalized to the inclusive semileptonic decay
rate, the theoretical expression is very well behaved, with small uncertainties
from unknown quark masses and no leading renormalon ambiguity. We compute the
decay rate for this process, including the leading perturbative and
nonperturbative corrections.
08/08/2013--
02/18/2013
Identical classical particles: half fermions and half bosons
We study the problem of particle indistinguishability for the three cases
known in nature: identical classical particles, identical bosons and identical
fermions. By exploiting the fact that different types of particles are
associated with Hilbert space vectors with different symmetries, we establish
some relations between the expectation value of several different operators, as
the particle number one and the interparticle correlation one, evaluated for
states of a pair of identical (a) classical particles, (b) bosons and (c)
fermions. We find that the quantum behavior of a pair of identical classical
particles has exactly half fermionic and half bosonic characteristics.
04/27/2023--
02/28/2023
Energy transfer between gravitational waves and quantum matter
We study the interaction between gravitational waves and quantum matter such
as Bose-Einstein condensates, super-fluid Helium, or ultra-cold solids,
explicitly taking into account the changes of the trapping potential induced by
the gravitational wave. As a possible observable, we consider the change of
energy due to the gravitational wave, for which we derive rigorous bounds in
terms of kinetic energy and particle number. Finally, we discuss implications
for possible experimental tests.
02/04/1994--
02/04/1994
Corrections to Bino Annihilation II: One-Loop Contribution to $\widetilde B \widetilde B \to Z^*$
We calculate the one-loop contribution to the bino annihilation rate due to
the process $\widetilde B \widetilde B \to Z^*$, which vanishes at tree level.
05/20/1994--
05/20/1994
Another Source of Baryons in $B$ Meson Decays
It is usually assumed that the production of baryons in $B$ meson decays is
induced primarily by the quark level process $b\to c\bar ud$, where the charm
quark hadronizes into a charmed baryon. With this assumption, the $\Lambda_c$
momentum spectrum would indicate that the transition $B\to\Lambda_c X$ is
dominated by multi-body $B$ decays. However, a closer examination of the
momentum spectrum reveals that the mass $m_X$ against which the $\Lambda_c$ is
recoiling almost always satisfies $m_X\agt m_{\Xi_c}$. This fact leads us to
examine the hypothesis that the production of charmed baryons in $B$ decays is
in fact dominated by the underlying transition $b\to c\bar cs$, and is seen
primarily in modes with two charmed baryons in the final state. We propose a
number of tests of this hypothesis. If this mechanism is indeed important in
baryon production, then there are interesting consequences and applications,
including potentially important implications for the ``charm deficit'' in $B$
decays.
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