2,655 research outputs found
Controlling the dynamics of a coupled atom-cavity system by pure dephasing : basics and potential applications in nanophotonics
The influence of pure dephasing on the dynamics of the coupling between a
two-level atom and a cavity mode is systematically addressed. We have derived
an effective atom-cavity coupling rate that is shown to be a key parameter in
the physics of the problem, allowing to generalize the known expression for the
Purcell factor to the case of broad emitters, and to define strategies to
optimize the performances of broad emitters-based single photon sources.
Moreover, pure dephasing is shown to be able to restore lasing in presence of
detuning, a further demonstration that decoherence can be seen as a fundamental
resource in solid-state cavity quantum electrodynamics, offering appealing
perspectives in the context of advanced nano-photonic devices.Comment: 10 pages, 7 figure
Infrared problem for the Nelson model on static space-times
We consider the Nelson model with variable coefficients and investigate the
problem of existence of a ground state and the removal of the ultraviolet
cutoff. Nelson models with variable coefficients arise when one replaces in the
usual Nelson model the flat Minkowski metric by a static metric, allowing also
the boson mass to depend on position. A physical example is obtained by
quantizing the Klein-Gordon equation on a static space-time coupled with a
non-relativistic particle. We investigate the existence of a ground state of
the Hamiltonian in the presence of the infrared problem, i.e. assuming that the
boson mass tends to 0 at infinity
Hadamard states from null infinity
Free field theories on a four dimensional, globally hyperbolic spacetime,
whose dynamics is ruled by a Green hyperbolic partial differential operator,
can be quantized following the algebraic approach. It consists of a two-step
procedure: In the first part one identifies the observables of the underlying
physical system collecting them in a *-algebra which encodes their relational
and structural properties. In the second step one must identify a quantum
state, that is a positive, normalized linear functional on the *-algebra out of
which one recovers the interpretation proper of quantum mechanical theories via
the so-called Gelfand-Naimark-Segal theorem. In between the plethora of
possible states, only few of them are considered physically acceptable and they
are all characterized by the so-called Hadamard condition, a constraint on the
singular structure of the associated two-point function. Goal of this paper is
to outline a construction scheme for these states which can be applied whenever
the underlying background possesses a null (conformal) boundary. We discuss in
particular the examples of a real, massless conformally coupled scalar field
and of linearized gravity on a globally hyperbolic and asymptotically flat
spacetime.Comment: 23 pages, submitted to the Proceedings of the conference "Quantum
Mathematical Physics", held in Regensburg from the 29th of September to the
02nd of October 201
Upper critical field of CeCoIn5
We present a detailed analysis of the upper critical field for CeCoIn5 under
high pressure. We show that, consistently with other measurements, this system
shows a decoupling between maximum of the superconducting transition
temperature Tc and maximum pairing strength. This puts forward CeCoIn5 as an
important paradigm for this class of unconventional, strongly correlated
superconductors.Comment: 15 pages, 5 figures, author version, published in New J. Phy
Pauli-Fierz model with Kato-class potentials and exponential decays
Generalized Pauli-Fierz Hamiltonian with Kato-class potential \KPF in
nonrelativistic quantum electrodynamics is defined and studied by a path
measure. \KPF is defined as the self-adjoint generator of a strongly
continuous one-parameter symmetric semigroup and it is shown that its bound
states spatially exponentially decay pointwise and the ground state is unique.Comment: We deleted Lemma 3.1 in vol.
Universal optimal broadband photon cloning and entanglement creation in one dimensional atoms
We study an initially inverted three-level atom in the lambda configuration
embedded in a waveguide, interacting with a propagating single-photon pulse.
Depending on the temporal shape of the pulse, the system behaves either as an
optimal universal cloning machine, or as a highly efficient deterministic
source of maximally entangled photon pairs. This quantum transistor operates
over a wide range of frequencies, and can be implemented with today's
solid-state technologies.Comment: 5 pages, 3 figure
Approach to ground state and time-independent photon bound for massless spin-boson models
It is widely believed that an atom interacting with the electromagnetic field
(with total initial energy well-below the ionization threshold) relaxes to its
ground state while its excess energy is emitted as radiation. Hence, for large
times, the state of the atom+field system should consist of the atom in its
ground state, and a few free photons that travel off to spatial infinity.
Mathematically, this picture is captured by the notion of asymptotic
completeness. Despite some recent progress on the spectral theory of such
systems, a proof of relaxation to the ground state and asymptotic completeness
was/is still missing, except in some special cases (massive photons, small
perturbations of harmonic potentials). In this paper, we partially fill this
gap by proving relaxation to an invariant state in the case where the atom is
modelled by a finite-level system. If the coupling to the field is sufficiently
infrared-regular so that the coupled system admits a ground state, then this
invariant state necessarily corresponds to the ground state. Assuming slightly
more infrared regularity, we show that the number of emitted photons remains
bounded in time. We hope that these results bring a proof of asymptotic
completeness within reach.Comment: 45 pages, published in Annales Henri Poincare. This archived version
differs from the journal version because we corrected an inconsequential
mistake in Section 3.5.1: to do this, a new paragraph was added after Lemma
3.
Correlated Photon Emission from a Single II-VI Quantum Dot
We report correlation and cross-correlation measurements of photons emitted
under continuous wave excitation by a single II-VI quantum dot (QD) grown by
molecular-beam epitaxy. A standard technique of microphotoluminescence combined
with an ultrafast photon correlation set-up allowed us to see an antibunching
effect on photons emitted by excitons recombining in a single CdTe/ZnTe QD, as
well as cross-correlation within the biexciton ()-exciton ()
radiative cascade from the same dot. Fast microchannel plate photomultipliers
and a time-correlated single photon module gave us an overall temporal
resolution of 140 ps better than the typical exciton lifetime in II-VI QDs of
about 250ps.Comment: 4 pages, 3 figures, to appear in Appl. Phys. Let
Probing top-Higgs non-standard interactions at the LHC
Effective interactions involving both the top quark and the Higgs field are
among the least constrained of all possible (gauge invariant) dimension-six
operators in the Standard Model. Such a handful of operators, in particular the
top quark chromomagnetic dipole moment, might encapsulate signs of the new
physics responsible for electroweak symmetry breaking. In this work, we compute
the contributions of these operators to inclusive Higgs and t tbar h
production. We argue that: i) rather strong constraints on the overall size of
these operators can already be obtained from the current limits/evidence on
Higgs production at the LHC; ii) t tbar h production will provide further key
information that is complementary to t tbar measurements, and the possibility
of discriminating among different contributions by performing accurate
measurements of total and differential rates.Comment: 8 pages, 9 figures. v2: Logarithmic contribution of the top quark
chromomagnetic operator to Higgs production by gluon fusion correcte
Optimal irreversible stimulated emission
We studied the dynamics of an initially inverted atom in a semi-infinite
waveguide, in the presence of a single propagating photon. We show that atomic
relaxation is enhanced by a factor of 2, leading to maximal bunching in the
output field. This optimal irreversible stimulated emission is a novel
phenomenon that can be observed with state-of-the-art solid-state atoms and
waveguides. When the atom interacts with two one-dimensional electromagnetic
environments, the preferential emission in the stimulated field can be
exploited to efficiently amplify a classical or a quantum state.Comment: 9 pages, 6 figure
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