3,238 research outputs found
Alternative scheme for two-qubit conditional phase gate by adiabatic passage under dissipation
We check a recent proposal [H. Goto and K. Ichimura Phys. Rev. A 70, 012305
(2004)] for controlled phase gate through adiabatic passage under the influence
of spontaneous emission and the cavity decay. We show a modification of above
proposal could be used to generate the necessary conditional phase gates in the
two-qubit Grover search. Conditioned on no photon leakage either from the
atomic excited state or from the cavity mode during the gating period, we
numerically analyze the success probability and the fidelity of the two-qubit
conditional phase gate by adiabatic passage. The comparison made between our
proposed gating scheme and a previous one shows that Goto and Ichimura's scheme
is an alternative and feasible way in the optical cavity regime for two-qubit
gates and could be generalised in principle to multi-qubit gates.Comment: to appear in J. Phys.
Qubit measurement using a quantum point contact with a quantum Langevin equation approach
We employ a quantum Langevin equation approach to establish non-Markovian
dynamical equations, on a fully microscopic basis, to investigate the
measurement of the state of a coupled quantum dot qubit by a nearby quantum
point contact. The ensuing Bloch equations allow us to examine qubit relaxation
and decoherence induced by measurement, and also the noise spectrum of meter
output current with the help of a quantum regression theorem, at arbitrary
bias-voltage and temperature. Our analyses provide a clear resolution of a
recent debate concerning the occurrence of a quantum oscillation peak in the
noise spectrum.Comment: 5 pages, 3 figures, submitted, published version in Phys. Rev.
Slow polaritons with orbital angular momentum in atomic gases
Polariton formalism is applied for studying the propagation of a probe field
of light in a cloud of cold atoms influenced by two control laser beams of
larger intensity. The laser beams couple resonantly three hyperfine atomic
ground states to a common excited state thus forming a tripod configuration of
the atomic energy levels involved. The first control beam can have an optical
vortex with the intensity of the beam going to zero at the vortex core. The
second control beam without a vortex ensures the loseless (adiabatic)
propagation of the probe beam at a vortex core of the first control laser. We
investigate the storage of the probe pulse into atomic coherences by switching
off the control beams, as well as its subsequent retrieval by switching the
control beams on. The optical vortex is transferred from the control to the
probe fields during the storage or retrieval of the probe field. We analyze
conditions for the vortex to be transferred efficiently to the regenerated
probe beam and discuss possibilities of experimental implementation of the
proposed scheme using atoms like rubidium or sodium.Comment: 4 figure
Entanglement of formation for a class of -dimensional systems
Currently the entanglement of formation can be calculated analytically for
mixed states in a -dimensional Hilbert space. For states in higher
dimensional Hilbert space a closed formula for quantifying entanglement does
not exist. In this regard only entanglement bounds has been found for
estimating it. In this work, we find an analytical expression for evaluating
the entanglement of formation for bipartite ()-dimensional mixed
states.Comment: 5 pages, 4 figures. Submitted for publicatio
Influence of Pure Dephasing on Emission Spectra from Single Photon Sources
We investigate the light-matter interaction of a quantum dot with the
electromagnetic field in a lossy microcavity and calculate emission spectra for
non-zero detuning and dephasing. It is found that dephasing shifts the
intensity of the emission peaks for non-zero detuning. We investigate the
characteristics of this intensity shifting effect and offer it as an
explanation for the non-vanishing emission peaks at the cavity frequency found
in recent experimental work.Comment: Published version, minor change
The second law, Maxwell's daemon and work derivable from quantum heat engines
With a class of quantum heat engines which consists of two-energy-eigenstate
systems undergoing, respectively, quantum adiabatic processes and energy
exchanges with heat baths at different stages of a cycle, we are able to
clarify some important aspects of the second law of thermodynamics. The quantum
heat engines also offer a practical way, as an alternative to Szilard's engine,
to physically realise Maxwell's daemon. While respecting the second law on the
average, they are also capable of extracting more work from the heat baths than
is otherwise possible in thermal equilibrium
Optical selection rules and phase-dependent adiabatic state control in a superconducting quantum circuit
We analyze the optical selection rules of the microwave-assisted transitions
in a flux qubit superconducting quantum circuit (SQC). We show that the
parities of the states relevant to the superconducting phase in the SQC are
well-defined when the external magnetic flux , then the
selection rules are same as the ones for the electric-dipole transitions in
usual atoms. When , the symmetry of the potential of
the artificial "atom'' is broken, a so-called -type "cyclic"
three-level atom is formed, where one- and two-photon processes can coexist. We
study how the population of these three states can be selectively transferred
by adiabatically controlling the electromagnetic field pulses. Different from
-type atoms, the adiabatic population transfer in our three-level
-atom can be controlled not only by the amplitudes but also by the
phases of the pulses
Nonequilibrium thermal entanglement in three-qubit model
Making use of the master equation and effective Hamiltonian approach, we
investigate the steady state entanglement in a three-qubit model. Both
symmetric and nonsymmetric qubit-qubit couplings are considered. The system
(the three qubits) is coupled to two bosonic baths at different temperatures.
We calculate the steady state by the effective Hamiltonian approach and discuss
the dependence of the steady state entanglement on the temperatures and
couplings. The results show that for symmetric qubit-qubit couplings, the
entanglements between the nearest neighbor are equal, independent of the
temperatures of the two baths. The maximum of the entanglement arrives at
. For nonsymmetric qubit-qubit couplings, however, the situation is
totally different. The baths at different temperatures would benefit the
entanglement and the entanglements between the nearest neighbors are no longer
equal. By examining the probability distribution of each eigenstate in the
steady state, we present an explanation for these observations. These results
suggest that the steady entanglement can be controlled by the temperature of
the two baths.Comment: Comments are welcom
Mach-Zehnder Interferometry at the Heisenberg Limit with coherent and squeezed-vacuum light
We show that the phase sensitivity of a Mach-Zehnder
interferometer fed by a coherent state in one input port and squeezed-vacuum in
the other one is i) independent from the true value of the phase shift and ii)
can reach the Heisenberg limit , where is the
average number of particles of the input states. We also show that the
Cramer-Rao lower bound, , can be saturated for arbitrary values of the squeezing parameter
and the amplitude of the coherent mode by a Bayesian phase
inference protocol.Comment: 4 pages, 4 figure
Phase detection at the quantum limit with multi-photon Mach-Zehnder interferometry
We study a Mach-Zehnder interferometer fed by a coherent state in one input
port and vacuum in the other. We explore a Bayesian phase estimation strategy
to demonstrate that it is possible to achieve the standard quantum limit
independently from the true value of the phase shift and specific assumptions
on the noise of the interferometer. We have been able to implement the protocol
using parallel operation of two photon-number-resolving detectors and
multiphoton coincidence logic electronics at the output ports of a
weakly-illuminated Mach-Zehnder interferometer. This protocol is unbiased and
saturates the Cramer-Rao phase uncertainty bound and, therefore, is an optimal
phase estimation strategy.Comment: 4 pages, 5 figures replaced fig. 1 to correct graphics bu
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