4,915 research outputs found
Non-Equilibrium Quantum Electrodynamics
We employ the influence functional technique to trace out the photonic
contribution from full quantum electrodynamics. The reduced density matrix
propagator for the spinor field is then constructed. We discuss the role of
time-dependent renormalization in the propagator and focus on the possibility
of obtaining dynamically induced superselection rules. Finally, we derive the
master equation for the case of the field being in an one-particle state in a
non-relativistic regime and discuss whether EM vacuumm fluctuations are
sufficient to produce decoherence in the position basis.Comment: 28 pages, 2 figures. Substantially revised, one important mistake
corrected; discussion on decoherence upgraded, section 4 essentially
rewritte
Moving Atom-Field Interactions: Quantum Motional Decoherence and Relaxation
The reduced dynamics of an atomic qubit coupled both to its own quantized
center of mass motion through the spatial mode functions of the electromagnetic
field, as well as the vacuum modes, is calculated in the influence functional
formalism. The formalism chosen can describe the entangled non-Markovian
evolution of the system with a full account of the coherent back-action of the
environment on the qubit. We find a slight increase in the decoherence due to
the quantized center of mass motion and give a condition on the mass and qubit
resonant frequency for which the effect is important. In optically resonant
alkali-metal atom systems, we find the effect to be negligibly small. The
framework presented here can nevertheless be used for general considerations of
the coherent evolution of qubits in moving atoms in an electromagnetic field.Comment: 9 pages, 1 figure, minor change
Classical Vs Quantum Probability in Sequential Measurements
We demonstrate in this paper that the probabilities for sequential
measurements have features very different from those of single-time
measurements. First, they cannot be modelled by a classical stochastic process.
Second, they are contextual, namely they depend strongly on the specific
measurement scheme through which they are determined. We construct
Positive-Operator-Valued measures (POVM) that provide such probabilities. For
observables with continuous spectrum, the constructed POVMs depend strongly on
the resolution of the measurement device, a conclusion that persists even if we
consider a quantum mechanical measurement device or the presence of an
environment. We then examine the same issues in alternative interpretations of
quantum theory. We first show that multi-time probabilities cannot be naturally
defined in terms of a frequency operator. We next prove that local hidden
variable theories cannot reproduce the predictions of quantum theory for
sequential measurements, even when the degrees of freedom of the measuring
apparatus are taken into account. Bohmian mechanics, however, does not fall in
this category. We finally examine an alternative proposal that sequential
measurements can be modelled by a process that does not satisfy the Kolmogorov
axioms of probability. This removes contextuality without introducing
non-locality, but implies that the empirical probabilities cannot be always
defined (the event frequencies do not converge). We argue that the predictions
of this hypothesis are not ruled out by existing experimental results
(examining in particular the "which way" experiments); they are, however,
distinguishable in principle.Comment: 56 pages, latex; revised and restructured. Version to appear in
Found. Phy
Bayesian Probabilities and the Histories Algebra
We attempt a justification of a generalisation of the consistent histories
programme using a notion of probability that is valid for all complete sets of
history propositions. This consists of introducing Cox's axioms of probability
theory and showing that our candidate notion of probability obeys them. We also
give a generalisation of Bayes' theorem and comment upon how Bayesianism should
be useful for the quantum gravity/cosmology programmes.Comment: 10 pages, accepted by Int. J. Theo. Phys. Feb 200
Decoherence and classical predictability of phase space histories
We consider the decoherence of phase space histories in a class of quantum
Brownian motion models, consisting of a particle moving in a potential
in interaction with a heat bath at temperature and dissipation gamma, in
the Markovian regime. The evolution of the density operator for this open
system is thus described by a non-unitary master equation. The phase space
histories of the system are described by a class of quasiprojectors.
Generalizing earlier results of Hagedorn and Omn\`es, we show that a phase
space projector onto a phase space cell is approximately evolved under
the master equation into another phase space projector onto the classical
dissipative evolution of , and with a certain amount of degradation due
to the noise produced by the environment. We thus show that histories of phase
space samplings approximately decohere, and that the probabilities for these
histories are peaked about classical dissipative evolution, with a width of
peaking depending on the size of the noise.Comment: 34 pages, LATEX, revised version to avoid LATEX error
Gravitational backreaction in cosmological spacetimes
We develop a new formalism for the treatment of gravitational backreaction in
the cosmological setting. The approach is inspired by projective techniques in
non-equilibrium statistical mechanics. We employ group-averaging with respect
to the action of the isotropy group of homogeneous and isotropic spacetimes
(rather than spatial averaging), in order to define effective FRW variables for
a generic spacetime. Using the Hamiltonian formalism for gravitating perfect
fluids, we obtain a set of equations for the evolution of the effective
variables; these equations incorporate the effects of backreaction by the
inhomogeneities. Specializing to dust-filled spacetimes, we find regimes that
lead to a closed set of backreaction equations, which we solve for small
inhomogeneities. We then study the case of large inhomogeneities in relation to
the proposal that backreaction can lead to accelerated expansion. In
particular, we identify regions of the gravitational state space that
correspond to effective cosmic acceleration. Necessary conditions are (i) a
strong expansion of the congruences corresponding to comoving observers, and
(ii) a large negative value of a dissipation variable that appears in the
effective equations (i.e, an effective "anti-dissipation").Comment: 36 pages, latex. Extended discussion on results and on relation to
Lemaitre-Tolman-Bondi models. Version to appear in PR
Quantum recoil effects in finite-time disentanglement of two distinguishable atoms
Starting from the requirement of distinguishability of two atoms by their
positions, it is shown that photon recoil has a strong influence on finite-time
disentanglement and in some cases prevents its appearance. At near-field inter
atomic distances well localized atoms, with maximally one atom being initially
excited, may suffer disentanglement at a single finite time or even at a series
of equidistant finite times, depending on their mean inter atomic distance and
their initial electronic preparation.Comment: 13 pages, 1 figure, submitted to Physical Review on august 2
Quantum optical versus quantum Brownian motion master-equation in terms of covariance and equilibrium properties
Structures of quantum Fokker-Planck equations are characterized with respect
to the properties of complete positivity, covariance under symmetry
transformations and satisfaction of equipartition, referring to recent
mathematical work on structures of unbounded generators of covariant quantum
dynamical semigroups. In particular the quantum optical master-equation and the
quantum Brownian motion master-equation are shown to be associated to
and symmetry respectively. Considering the motion
of a Brownian particle, where the expression of the quantum Fokker-Planck
equation is not completely fixed by the aforementioned requirements, a recently
introduced microphysical kinetic model is briefly recalled, where a quantum
generalization of the linear Boltzmann equation in the small energy and
momentum transfer limit straightforwardly leads to quantum Brownian motion.Comment: 11 pages, latex, no figures, slight changes and a few references
added, to appear in J. Math. Phy
Moving Atom-Field Interaction: Correction to Casimir-Polder Effect from Coherent Back-action
The Casimir-Polder force is an attractive force between a polarizable atom
and a conducting or dielectric boundary. Its original computation was in terms
of the Lamb shift of the atomic ground state in an electromagnetic field (EMF)
modified by boundary conditions along the wall and assuming a stationary atom.
We calculate the corrections to this force due to a moving atom, demanding
maximal preservation of entanglement generated by the moving atom-conducting
wall system. We do this by using non-perturbative path integral techniques
which allow for coherent back-action and thus can treat non-Markovian
processes. We recompute the atom-wall force for a conducting boundary by
allowing the bare atom-EMF ground state to evolve (or self-dress) into the
interacting ground state. We find a clear distinction between the cases of
stationary and adiabatic motions. Our result for the retardation correction for
adiabatic motion is up to twice as much as that computed for stationary atoms.
We give physical interpretations of both the stationary and adiabatic atom-wall
forces in terms of alteration of the virtual photon cloud surrounding the atom
by the wall and the Doppler effect.Comment: 16 pages, 2 figures, clarified discussions; to appear in Phys. Rev.
- …