1,011 research outputs found
Accurate "superluminal" transmission via entanglement, superoscillations and quasi-Dirac distributions
We analyse a system in which, due to entanglement between the spin and
spatial degrees of freedom, the reduced transmitted state has the shape of the
freely propagating pulse translated in the complex co-ordinate plane. In the
case an apparently "superluminal" advancement of the pulse the delay amplitude
distribution is found to be a peculiar approximation to the Dirac
delta-function, and the transmission coefficient exhibits a well-defined
super-oscillatory window. Analogies with potential tunnelling and the Wheeler's
delayed choice experiment are highlighted
Hartman effect and spin precession in graphene
Spin precession has been used to measure the transmission time \tau over a
distance L in a graphene sheet. Since conduction electrons in graphene have an
energy-independent velocity v, one would expect \tau > L/v. Here we calculate
that \tau < L/v at the Dirac point (= charge neutrality point) in a clean
graphene sheet, and we interpret this result as a manifestation of the Hartman
effect (apparent superluminality) known from optics.Comment: 6 pages, 4 figures; v2: added a section on the case of
perpendicularly aligned magnetizations; v3: added a figur
The Larmor clock and anomalous spin dephasing in silicon
Drift-diffusion theory - which fully describes charge transport in
semiconductors - is also universally used to model transport of spin-polarized
electrons in the presence of longitudinal electric fields. By transforming spin
transit time into spin orientation with precession (a technique called the
"Larmor clock") in current-sensing vertical-transport intrinsic Si devices, we
show that spin diffusion (and concomitant spin dephasing) can be greatly
enhanced with respect to charge diffusion, in direct contrast to predictions of
spin Coulomb-drag diffusion suppression.Comment: minor edits and updated ref
On causality, apparent 'superluminality' and reshaping in barrier penetration
We consider tunnelling of a non-relativistic particle across a potential
barrier. It is shown that the barrier acts as an effective beam splitter which
builds up the transmitted pulse from the copies of the initial envelope shifted
in the coordinate space backwards relative to the free propagation. Although
along each pathway causality is explicitly obeyed, in special cases reshaping
can result an overall reduction of the initial envelope, accompanied by an
arbitrary coordinate shift. In the case of a high barrier the delay amplitude
distribution (DAD) mimics a Dirac -function, the transmission amplitude
is superoscillatory for finite momenta and tunnelling leads to an accurate
advancement of the (reduced) initial envelope by the barrier width. In the case
of a wide barrier, initial envelope is accurately translated into the complex
coordinate plane. The complex shift, given by the first moment of the DAD,
accounts for both the displacement of the maximum of the transmitted
probability density and the increase in its velocity. It is argued that
analysing apparent 'superluminality' in terms of spacial displacements helps
avoid contradiction associated with time parameters such as the phase time
The Faraday Quantum Clock and Non-local Photon Pair Correlations
We study the use of the Faraday effect as a quantum clock for measuring
traversal times of evanescent photons through magneto-refractive structures.
The Faraday effect acts both as a phase-shifter and as a filter for circular
polarizations. Only measurements based on the Faraday phase-shift properties
are relevant to the traversal time measurements. The Faraday polarization
filtering may cause the loss of non-local (Einstein-Podolsky-Rosen) two-photon
correlations, but this loss can be avoided without sacrificing the clock
accuracy. We show that a mechanism of destructive interference between
consecutive paths is responsible for superluminal traversal times measured by
the clock.Comment: 6 figure
Compact and Loosely Bound Structures in Light Nuclei
A role of different components in the wave function of the weakly bound light
nuclei states was studied within the framework of the cluster model, taking
into account of orbitals "polarization". It was shown that a limited number of
structures associated with the different modes of nucleon motion can be of
great importance for such systems. Examples of simple and quite flexible trial
wave functions are given for the nuclei Be, He. Expressions for the
microscopic wave functions of these nuclei were found and used for the
calculation of basic nuclear characteristics, using well known central-exchange
nucleon-nucleon potentials.Comment: 19 pages, 3 ps figure
Towards the Gravity Dual of Quarkonium in the Strongly Coupled QCD Plasma
We build a "bottom-up" holographic model of charmonium by matching the
essential spectral data. We argue that this data must include not only the
masses but also the decay constants of the J/psi and psi' mesons. Relative to
the "soft-wall" models for light mesons, such a matching requires two new
features in the holographic potential: an overall upward shift as well as a
narrow "dip" near the holographic boundary. We calculate the spectral function
as well as the position of the complex singularities (quasinormal frequencies)
of the retarded correlator of the charm current at finite temperatures. We
further extend this analysis by showing that the residues associated with these
singularities are given by the boundary derivative of the appropriately
normalized quasinormal mode. We find that the "melting" of the J/psi spectral
peak occurs at a temperature of about 540 MeV, or 2.8 T_c, in good agreement
with lattice results.Comment: 13 pages, 9 figure
Linewidths in bound state resonances for helium scattering from Si(111)-(1x1)H
Helium-3 spin-echo measurements of resonant scattering from the Si(111)â(1 Ă 1)H surface, in the energy range 4â14 meV, are presented. The measurements have high energy resolution yet they reveal bound state resonance features with uniformly broad linewidths. We show that exact quantum mechanical calculations of the elastic scattering, using the existing potential for the helium/Si(111)â(1 Ă 1)H interaction, cannot reproduce the linewidths seen in the experiment. Further calculations rule out inelastic and other mechanisms that might give rise to losses from the elastic scattering channels. We show that corrugation in the attractive part of the atomâsurface potential is the most likely origin of the experimental lineshapes
\bar{p}p low energy parameters from annihilation cross section data
The recent experimental data obtained by the OBELIX group on total
annihilation cross section are analysed; the low energy spin averaged
parameters of the scattering amplitude (the imaginary parts of the
S-wave scattering length and P-wave scattering volume) are extracted from the
data. Their values are found to be equal to . The
results are in very good agreement with existing atomic data.Comment: latex.tar.gz file, 8 pages, 1 figur
- âŠ