3,920 research outputs found
Quark number susceptibilities, strangeness and dynamical confinement
We report first results on the strange quark number susceptibility, chi_s,
over a large range of temperatures, mainly in the plasma phase of QCD. Chi_s
jumps across the phase transition temperature, T_c, and grows rapidly with
temperature above but close to T_c. For all quark masses and susceptibilities
in the entire temperature range studied, we found significant departures from
ideal-gas values. We also observed a strong correlation between these
quantities and the susceptibility in the scalar/pseudo-scalar channel,
supporting ideas of ``dynamical confinement'' in the high temperature phase of
the QCD plasma.Comment: 4 pages, 4 figure
Ballistic-Ohmic quantum Hall plateau transition in graphene pn junction
Recent quantum Hall experiments conducted on disordered graphene pn junction
provide evidence that the junction resistance could be described by a simple
Ohmic sum of the n and p mediums' resistances. However in the ballistic limit,
theory predicts the existence of chirality-dependent quantum Hall plateaus in a
pn junction. We show that two distinctively separate processes are required for
this ballistic-Ohmic plateau transition, namely (i) hole/electron Landau states
equilibration and (ii) valley iso-spin dilution of the incident Landau edge
state. These conclusions are obtained by a simple scattering theory argument,
and confirmed numerically by performing ensembles of quantum magneto-transport
calculations on a 0.1um-wide disordered graphene pn junction within the
tight-binding model. The former process is achieved by pn interface roughness,
where a pn interface disorder with a root-mean-square roughness of 10nm was
found to suffice under typical experimental conditions. The latter process is
mediated by extrinsic edge roughness for an armchair edge ribbon and by
intrinsic localized intervalley scattering centers at the edge of the pn
interface for a zigzag ribbon. In light of these results, we also examine why
higher Ohmic type plateaus are less likely to be observable in experiments.Comment: 9 pages, 6 figure
Structure, bonding and magnetism in cobalt clusters
The structural, electronic and magnetic properties of Co clusters
(20) have been investigated using density functional theory within the
pseudopotential plane wave method. An unusual hexagonal growth pattern has been
observed in the intermediate size range, 20. The cobalt atoms are
ferromagnetically ordered and the calculated magnetic moments are found to be
higher than that of corresponding hcp bulk value, which are in good agreement
with the recent Stern-Gerlach experiments. The average coordination number is
found to dominate over the average bond length to determine the effective
hybridization and consequently the cluster magnetic moment.Comment: 12 pages and 9 figure
Does the QCD plasma contain propagating gluons?
Comparison of two appropriately chosen screening masses of colour singlet
operators in the pure glue QCD plasma indicates that at sufficiently high
temperature it contains a weakly-interacting massive quasi-particle with the
quantum numbers of the electric gluon. Still in the deconfined phase, but
closer to T_c, the same mass ratio is similar to that at zero temperature,
indicating that the propagating modes are more glueball-like, albeit with a
lower scale for the masses. We observe a continuity between these two regimes.Comment: 4 pages, 3 figure
Roles of a 67-kDa polypeptide in reversal of protein synthesis inhibition in heme-deficient reticulocyte lysate.
Heavy Quark Diffusion and Lattice Correlators
We study charmonia correlators at finite temperature. We analyze to what
extent heavy quarkonia correlators are sensitive to the effect of heavy quark
transport and whether it is possible to constrain the heavy quark diffusion
constant by lattice calculations. Preliminary lattice calculations of quarkonia
correlators performed on anisotropic lattices show that they are sensitive to
the effect of heavy quark transport, but much detailed calculations are
required to constrain the value of the heavy quark diffusion constant.Comment: Based on talks presented on Lattice 2005, Extreme QCD 2005 and Quark
Matter 2005, 5 pages, 4 Figure
Effect of nonlinearity on the dynamics of a particle in dc field-induced systems
Dynamics of a particle in a perfect chain with one nonlinear impurity and in
a perfect nonlinear chain under the action of dc field is studied numerically.
The nonlinearity appears due to the coupling of the electronic motion to
optical oscillators which are treated in adiabatic approximation.
We study for both the low and high values of field strength. Three different
range of nonlinearity is obtained where the dynamics is different. In low and
intermediate range of nonlinearity, it reduces the localization. In fact in the
intermediate range subdiffusive behavior in the perfect nonlinear chain is
obtained for a long time. In all the cases a critical value of nonlinear
strength exists where self-trapping transition takes place. This critical value
depends on the system and the field strength. Beyond the self-trapping
transition nonlinearity enhances the localization.Comment: 9 pages, Revtex, 6 ps figures include
"All-versus-nothing" proof of tripartite quantum steering and genuine entanglement certification in the two-sided device-independent scenario
We consider the task of certification of genuine entanglement of tripartite
states. We first present an "all-versus-nothing" proof of tripartite
Einstein-Podolsky-Rosen (EPR) steering by demonstrating the non-existence of a
local hidden state (LHS) model in the tripartite network as a motivation to our
main result. A full logical contradiction of the predictions of the LHS model
with quantum mechanical outcome statistics for any three-qubit generalized
Greenberger-Horne-Zeilinger (GGHZ) states and pure W-class states is shown,
using which, one can distinguish between the GGHZ and W-class states in the
two-sided device-independent (2SDI) steering scenario. We next formulate a 2SDI
fine-grained steering inequality for the tripartite scenario. We show that the
maximum quantum violation of this FGI can be used to certify genuine
entanglement of three-qubit pure states.Comment: Analysis and results strengthened (sharp logical contradiction proofs
of W-class states added), comments are welcom
The continuum limit of quark number susceptibilities
We report the continuum limit of quark number susceptibilities in quenched
QCD. Deviations from ideal gas behaviour at temperature T increase as the
lattice spacing is decreased from T/4 to T/6, but a further decrease seems to
have very little effect. The measured susceptibilities are 20% lower than the
ideal gas values, and also 10% below the hard thermal loop (HTL) results. The
off-diagonal susceptibility is several orders of magnitude smaller than the HTL
results. We verify a strong correlation between the lowest screening mass and
the susceptibility. We also show that the quark number susceptibilities give a
reasonable account of the Wroblewski parameter, which measures the strangeness
yield in a heavy-ion collision.Comment: 8 pages, 5 figure
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