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191.
J. Song Y. Xia H. S. Song B. Liu 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,50(1):91-96
We propose a scheme to generate a maximally four-dimensional
entangled state of two six-level atoms in two remote cavities. By
choosing suitable intensities and detunings of fields, atomic spontaneous radiation and photon leakage out of cavity and fibre
are efficiently suppressed. Thus, the intended state can be generated with high fidelity in the presence of decoherence. We
extend the scheme to generate an N-atom four-dimensional entangled
state. 相似文献
192.
Robert H. Swendsen 《Journal of statistical physics》2004,117(5-6):1063-1070
In a recent paper, Nagle criticized the new definition of entropy that I had proposed in an earlier work. In the examples for which Nagle claims my definition fails, he took a formula that I had derived for one set of experiments and used it to represent my definition for other experiments. However, the formulas obtained from my definition depend on the specific experimental observables. If my definition is correctly applied to Nagles experiments, no contradictions remain. 相似文献
193.
E. Santos 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,42(3):501-509
A family of local models containing two angles as hidden variables is
defined for experiments measuring polarization correlation of optical
photons. Searching for the best model of the family, that is giving
predictions most close to quantum mechanics, allows deriving Bell-type
inequalities which may be tested with relatively low detection efficiency. 相似文献
194.
S. K.?GhosalEmail author Saroj?Nepal Debarchana?Das 《Foundations of Physics Letters》2005,18(7):603-619
No Heading The canonical twin paradox is explained by making a correct use of the principle of equivalence. The role of the principle
of equivalence is to provide a physical agent i.e gravity which can supply the required extra aging to the rocket-bound sibling
during its acceleration phase through a gravitational time-offset effect. We follow an approach where a novel variation on
the twin paradox is used to connect gravity with the desynchronization in the clocks of two spatially distant, identically
accelerated observers. It is shown that this approach removes certain drawbacks of an earlier effort which claims to exploit
the equivalence principle in explaining the differential aging in the paradox.
* Author to whom all correspondences should be made. 相似文献
195.
M. Mirzaee M. Rezaei M. A. Jafarizadeh 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,60(2):193-201
In this study the intimate connection is established between the
Banach space wavelet reconstruction method on homogeneous spaces
with both singular and nonsingular vacuum vectors, and some of the
well known quantum tomographies, such as: Moyal-representation for a
spin, discrete phase space tomography, tomography of a free
particle, Homodyne tomography, phase space tomography and SU(1,1)
tomography. And both the atomic decomposition and the Banach frame
nature of these quantum tomographic examples are also revealed in
details. Finally the connection between the wavelet formalism on
Banach space and Q-function is discussed. 相似文献
196.
Hrvoje Nikolić 《Foundations of Physics Letters》2000,13(6):595-601
We study the role of acceleration in the twin paradox. From the coordinate transformation that relates an accelerated and an inertial observer we find that, from the point of view of the accelerated observer, the rate of the differential lapses of time depends not only on the relative velocity, but also on the product of the acceleration and the distance between the observers. However, this result does not have a direct operational interpretation because an observer at a certain position can measure only physical quantities that are defined at the same position. For local measurements, the asymmetry between the two observers can be attributed to the fact that noninertial coordinate systems, contrary to inertial coordinate systems, can be correctly interpreted only locally. 相似文献
197.
Andrei Khrennikov 《Journal of Russian Laser Research》2008,29(2):101-113
Our aim is to understand the role of implicit assumptions which has been used by Einstein, Podolsky, and Rosen (EPR) in their
famous article [Phys. Rev., 47, 777 (1935)] devoted to the so-called EPR paradox. We found that the projection postulate plays a crucial role in the EPR
argument. It seems that EPR made a mistake in this paper — the projection postulate was applied not in its original form (as
it has been formulated in von Neumann's book [Mathematical Foundations of Quantum mechanics, Princeton University Press (1955)] but in the form which was later formalized as Lüders' postulate [Ann. Phys., Lpz. 8, 322 (1951)]. Von Neumann's postulate was crucially modified by extending it to observables with degenerate spectra. This
modification is the real source of “quantum nonlocality.” The use of the original von Neumann postulate eliminates this problem
— instead of (an action at a distance)-nonlocality, we obtain a classical measurement nonlocality, which is related to the
synchronization of two measurements (produced on the two parts of a composite system). If one uses correctly von Neumann's
projection postulate, no “elements of reality” can be assigned to entangled systems.
Talk presented at the oral issue of J. Russ. Laser Res. dedicated to the memory of Professor Vladimir A. Isakov, Professor
Alexander S. Shumovsky, and Professor Andrei V. Vinogradov held in Moscow February 21–22, 2008. 相似文献
198.
P. Caban J. Rembieliński K. A. Smoliński Z. Walczak 《International Journal of Theoretical Physics》2003,42(5):1045-1052
Einstein—Podolsky—Rosen spin correlations in the framework of nonrelativistic quantum mechanics for moving observers are calculated. The measurements are performed in bounded regions of space (detectors), not necessarily simultaneously. The resulting correlation function depends not only on the directions of spin measurements but also on the relative velocity of the observers. 相似文献
199.
S. K. Ghosal Biplab Raychaudhuri Anjan Kumar Chowdhury Minakshi Sarker 《Foundations of Physics》2003,33(6):981-1001
There seems to exist a dilemma in the literature as to the correct relativistic formula for the Sagnac phase-shift. The paper addresses this issue in the light of a novel, kinematically equivalent linear Sagnac-type thought experiment, which provides a vantage point from which the effect of rotation in the usual Sagnac effect can be analyzed. The question is shown to be related to the so-called rotating disc problem known as the Ehrenfest paradox. The relativistic formula for the Sagnac phase-shift seems to depend on the way the paradox is resolved. Kinematic resolution of the Ehrenfest paradox proposed by some authors predicts the usually quoted formula for the Sagnac delay but the resolution itself is shown to be based upon some implicit assumptions regarding the behaviour of solid bodies under acceleration. In order to have a greater insight into the problem, a second version of the thought experiment involving linear motion of a special type of a non-rigid frame of reference is discussed. It is shown by analogy that the usually quoted special relativistic formula for the Sagnac delay follows, provided the material of the disc matches the special type. 相似文献
200.
Richard A. Mould 《Foundations of Physics》2003,33(4):591-612
If conscious observers are to be included in the quantum mechanical universe, we need to find the rules that engage observers with quantum mechanical systems. The author has proposed five rules that are discovered by insisting on empirical completeness; that is, by requiring the rules to draw empirical information from Schrödinger's solutions that is more complete than is currently possible with the (Born) probability interpretation. I discard Born's interpretation, introducing probability solely through probability current. These rules tell us something about brains. They require the existence of observer brain states that are neither conscious nor unconscious. I call them ready brain states because they are on stand-by, ready to become conscious the moment they are stochastically chosen. Two of the rules are selection rules involving ready brain states. The place of these rules in a wider theoretical context is discussed. 相似文献