69 research outputs found
Fidelity for Multimode Thermal Squeezed States
In the theory of quantum transmission of information the concept of fidelity
plays a fundamental role. An important class of channels, which can be
experimentally realized in quantum optics, is that of Gaussian quantum
channels. In this work we present a general formula for fidelity in the case of
two arbitrary Gaussian states. From this formula one can get a previous result
(H. Scutaru, J. Phys. A: Mat. Gen {\bf 31}, 3659 (1998)), for the case of a
single mode; or, one can apply it to obtain a closed compact expression for
multimode thermal states.Comment: 5 pages, RevTex, submitted to Phys. Rev.
Upper bounds on the relative energy difference of pure and mixed Gaussian states with a fixed fidelity
Exact and approximate formulas for the upper bound of the relative energy
difference of two Gaussian states with the fixed fidelity between them are
derived. The reciprocal formulas for the upper bound of the fidelity for the
fixed value of the relative energy difference are obtained as well. The bounds
appear higher for pure states than for mixed ones, and their maximal values
correspond to squeezed vacuum states. In particular, to guarantee the relative
energy difference less than 10%, for quite arbitrary Gaussian states, the
fidelity between them must exceed the level 0.998866.Comment: 9 pages, accepted for publication in Journal of Physics
Transition probabilities between quasifree states
We obtain a general formula for the transition probabilities between any
state of the algebra of the canonical commutation relations (CCR-algebra) and a
squeezed quasifree state. Applications of this formula are made for the case of
multimode thermal squeezed states of quantum optics using a general canonical
decomposition of the correlation matrix valid for any quasifree state. In the
particular case of a one mode CCR-algebra we show that the transition
probability between two quasifree squeezed states is a decreasing function of
the geodesic distance between the points of the upper half plane representing
these states. In the special case of the purification map it is shown that the
transition probability between the state of the enlarged system and the product
state of real and fictitious subsystems can be a measure for the entanglement.Comment: 13 pages, REVTeX, no figure
Fidelity for displaced squeezed states and the oscillator semigroup
The fidelity for two displaced squeezed thermal states is computed using the
fact that the corresponding density operators belong to the oscillator
semigroup.Comment: 3 pages, REVTEX, no figures, submitted to Journal of Physics A, May
5, 199
Bures distance between two displaced thermal states
The Bures distance between two displaced thermal states and the corresponding
geometric quantities (statistical metric, volume element, scalar curvature) are
computed. Under nonunitary (dissipative) dynamics, the statistical distance
shows the same general features previously reported in the literature by
Braunstein and Milburn for two--state systems. The scalar curvature turns out
to have new interesting properties when compared to the curvature associated
with squeezed thermal states.Comment: 3 pages, RevTeX, no figure
Two-Qubit Separability Probabilities and Beta Functions
Due to recent important work of Zyczkowski and Sommers (quant-ph/0302197 and
quant-ph/0304041), exact formulas are available (both in terms of the
Hilbert-Schmidt and Bures metrics) for the (n^2-1)-dimensional and
(n(n-1)/2-1)-dimensional volumes of the complex and real n x n density
matrices. However, no comparable formulas are available for the volumes (and,
hence, probabilities) of various separable subsets of them. We seek to clarify
this situation for the Hilbert-Schmidt metric for the simplest possible case of
n=4, that is, the two-qubit systems. Making use of the density matrix (rho)
parameterization of Bloore (J. Phys. A 9, 2059 [1976]), we are able to reduce
each of the real and complex volume problems to the calculation of a
one-dimensional integral, the single relevant variable being a certain ratio of
diagonal entries, nu = (rho_{11} rho_{44})/{rho_{22} rho_{33})$. The associated
integrand in each case is the product of a known (highly oscillatory near nu=1)
jacobian and a certain unknown univariate function, which our extensive
numerical (quasi-Monte Carlo) computations indicate is very closely
proportional to an (incomplete) beta function B_{nu}(a,b), with a=1/2,
b=sqrt{3}in the real case, and a=2 sqrt{6}/5, b =3/sqrt{2} in the complex case.
Assuming the full applicability of these specific incomplete beta functions, we
undertake separable volume calculations.Comment: 17 pages, 4 figures, paper is substantially rewritten and
reorganized, with the quasi-Monte Carlo integration sample size being greatly
increase
Proof of an entropy conjecture for Bloch coherent spin states and its generalizations
Wehrl used Glauber coherent states to define a map from quantum density
matrices to classical phase space densities and conjectured that for Glauber
coherent states the mininimum classical entropy would occur for density
matrices equal to projectors onto coherent states. This was proved by Lieb in
1978 who also extended the conjecture to Bloch SU(2) spin-coherent states for
every angular momentum . This conjecture is proved here. We also recall our
1991 extension of the Wehrl map to a quantum channel from to , with corresponding to the Wehrl map to classical densities.
For each and we show that the minimal output entropy for
these channels occurs for a coherent state. We also show that coherent
states both Glauber and Bloch minimize any concave functional, not just
entropy.Comment: Version 2 only minor change
Instruments and channels in quantum information theory
While a positive operator valued measure gives the probabilities in a quantum
measurement, an instrument gives both the probabilities and the a posteriori
states. By interpreting the instrument as a quantum channel and by using the
typical inequalities for the quantum and classical relative entropies, many
bounds on the classical information extracted in a quantum measurement, of the
type of Holevo's bound, are obtained in a unified manner.Comment: 12 pages, revtex
On Bures fidelity of displaced squeezed thermal states
Fidelity plays a key role in quantum information and communication theory.
Fidelity can be interpreted as the probability that a decoded message possesses
the same information content as the message prior to coding and transmission.
In this paper, we give a formula of Bures fidelity for displaced squeezed
thermal states directly by the displacement and squeezing parameters and
birefly discuss how the results can apply to quantum information theory.Comment: 10 pages with RevTex require
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