5,575 research outputs found
Quantum error correction for continuously detected errors
We show that quantum feedback control can be used as a quantum error
correction process for errors induced by weak continuous measurement. In
particular, when the error model is restricted to one, perfectly measured,
error channel per physical qubit, quantum feedback can act to perfectly protect
a stabilizer codespace. Using the stabilizer formalism we derive an explicit
scheme, involving feedback and an additional constant Hamiltonian, to protect
an ()-qubit logical state encoded in physical qubits. This works for
both Poisson (jump) and white-noise (diffusion) measurement processes. In
addition, universal quantum computation is possible in this scheme. As an
example, we show that detected-spontaneous emission error correction with a
driving Hamiltonian can greatly reduce the amount of redundancy required to
protect a state from that which has been previously postulated [e.g., Alber
\emph{et al.}, Phys. Rev. Lett. 86, 4402 (2001)].Comment: 11 pages, 1 figure; minor correction
Selective linear or quadratic optomechanical coupling via measurement
The ability to engineer both linear and non-linear coupling with a mechanical
resonator is an important goal for the preparation and investigation of
macroscopic mechanical quantum behavior. In this work, a measurement based
scheme is presented where linear or square mechanical displacement coupling can
be achieved using the optomechanical interaction linearly proportional to the
mechanical position. The resulting square displacement measurement strength is
compared to that attainable in the dispersive case using the direct interaction
to the mechanical displacement squared. An experimental protocol and parameter
set are discussed for the generation and observation of non-Gaussian states of
motion of the mechanical element.Comment: 7 pages, 2 figures, (accepted in Physical Review X
Modal dynamics for positive operator measures
The modal interpretation of quantum mechanics allows one to keep the standard
classical definition of realism intact. That is, variables have a definite
status for all time and a measurement only tells us which value it had.
However, at present modal dynamics are only applicable to situations that are
described in the orthodox theory by projective measures. In this paper we
extend modal dynamics to include positive operator measures (POMs). That is,
for example, rather than using a complete set of orthogonal projectors, we can
use an overcomplete set of nonorthogonal projectors. We derive the conditions
under which Bell's stochastic modal dynamics for projective measures reduce to
deterministic dynamics, showing (incidentally) that Brown and Hiley's
generalization of Bohmian mechanics [quant-ph/0005026, (2000)] cannot be thus
derived. We then show how {\em deterministic} dynamics for positive operators
can also be derived. As a simple case, we consider a Harmonic oscillator, and
the overcomplete set of coherent state projectors (i.e. the Husimi POM). We
show that the modal dynamics for this POM in the classical limit correspond to
the classical dynamics, even for the nonclassical number state . This
is in contrast to the Bohmian dynamics, which for energy eigenstates, the
dynamics are always non-classical.Comment: 14 page
Nontrivial quantum effects in biology: A skeptical physicists' view
Invited contribution to "Quantum Aspects of Life", D. Abbott Ed. (World
Scientific, Singapore, 2007).Comment: 15 pages, minor typographical errors correcte
- …