4,649 research outputs found
Interpretations and Implications of the Top Quark Rapidity Asymmetries and
Forward-backward asymmetries and are observed in the
top quark rapidity distribution and in the rapidity distribution of charged
leptons from top quark decay at the Tevatron proton-antiproton collider,
and a charge asymmetry is seen in proton-proton collisions at the Large
Hadron Collider (LHC). In this paper, we update our previous studies of the
Tevatron asymmetries using the most recent data. We provide expectations for
at the LHC based first on model independent extrapolations from the
Tevatron, and second based on new physics models that can explain the Tevatron
asymmetries. We examine the relationship of the two asymmetries and
. We show their connection through the spin correlation
between the charged lepton and the top quark with different polarization
states. We show that the ratio of the two asymmetries provides independent
insight into new physics models that are invoked to fit the top quark
asymmetry. We emphasize the value of the measurement of both asymmetries, and
we conclude that a model which produces more right-handed than left-handed top
quarks is favored by the present Tevatron data.Comment: Some figures changed. A typo in appendix fixed. Published in Physical
Review
Repeat-Until-Success Quantum Computing
We demonstrate the possibility to perform distributed quantum computing using
only single photon sources (atom-cavity-like systems), linear optics and photon
detectors. The qubits are encoded in stable ground states of the sources. To
implement a universal two-qubit gate, two photons should be generated
simultaneously and pass through a linear optics network, where a measurement is
performed on them. Gate operations can be repeated until a success is heralded
without destroying the qubits at any stage of the operation. In contrast to
other schemes, this does not require explicit qubit-qubit interactions, a
priori entangled ancillas nor the feeding of photons into photon sources.Comment: 5 pages, 2 figures, v3: substantially revised, v4: typos correcte
Top Quark Polarization As A Probe of Models with Extra Gauge Bosons
New heavy gauge bosons exist in many models of new physics beyond the
standard model of particle physics. Discovery of these W^\prime and Z^\prime
resonances and the establishment of their spins, couplings, and other quantum
numbers would shed light on the gauge structure of the new physics. The
measurement of the polarization of the SM fermions from the gauge boson decays
would decipher the handedness of the coupling of the new states, an important
relic of the primordial new physics symmetry. Since the top quark decays
promptly, its decay preserves spin information. We show how decays of new gauge
bosons into third generation fermions (W^\prime \to tb, Z^\prime\to t\bar{t})
can be used to determine the handedness of the couplings of the new states and
to discriminate among various new physics models
Sizes of Minimum Connected Dominating Sets of a Class of Wireless Sensor Networks
We consider an important performance measure of wireless sensor networks, namely, the least number of nodes, N, required to facilitate routing between any pair of nodes, allowing other nodes to remain in sleep mode in order to conserve energy. We derive the expected value and the distribution of N for single dimensional dense networks
Approach to accurately measuring the speed of optical precursors
Precursors can serve as a bound on the speed of information with dispersive
medium. We propose a method to identify the speed of optical precursors using
polarization-based interference in a solid-state device, which can bound the
accuracy of the precursors' speed to less than with conventional
experimental conditions. Our proposal may have important implications for
optical communications and fast information processing.Comment: 4 pages, 4 figure
Top Quark Forward-Backward Asymmetry and Same-Sign Top Quark Pairs
The top quark forward-backward asymmetry measured at the Tevatron collider
shows a large deviation from standard model expectations. Among possible
interpretations, a non-universal model is of particular interest as
it naturally predicts a top quark in the forward region of large rapidity. To
reproduce the size of the asymmetry, the couplings of the to
standard model quarks must be large, inevitably leading to copious production
of same-sign top quark pairs at the energies of the Large Hadron Collider
(LHC). We explore the discovery potential for and production in
early LHC experiments at 7-8 TeV and conclude that if {\it no} signal is
observed with 1 fb of integrated luminosity, then a non-universal
alone cannot explain the Tevatron forward-backward asymmetry.Comment: Tevatron limit from same-sign tt search adde
The Top Quark Production Asymmetries and
A large forward-backward asymmetry is seen in both the top quark rapidity
distribution and in the rapidity distribution of charged leptons
from top quarks produced at the Tevatron. We study the kinematic
and dynamic aspects of the relationship of the two observables arising from the
spin correlation between the charged lepton and the top quark with different
polarization states. We emphasize the value of both measurements, and we
conclude that a new physics model which produces more right-handed than
left-handed top quarks is favored by the present data.Comment: accepted for publication in Physical Review Letter
More on volume dependence of spectral weight function
Spectral weight functions are easily obtained from two-point correlation
functions and they might be used to distinguish single-particle from
multi-particle states in a finite-volume lattice calculation, a problem crucial
for many lattice QCD simulations. In previous studies, it is shown that the
spectral weight function for a broad resonance shares the typical volume
dependence of a two-particle scattering state i.e. proportional to in a
large cubic box of size while the narrow resonance case requires further
investigation. In this paper, a generalized formula is found for the spectral
weight function which incorporates both narrow and broad resonance cases.
Within L\"uscher's formalism, it is shown that the volume dependence of the
spectral weight function exhibits a single-particle behavior for a extremely
narrow resonance and a two-particle behavior for a broad resonance. The
corresponding formulas for both and channels are derived. The
potential application of these formulas in the extraction of resonance
parameters are also discussed
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