QUANTPHYS.bib
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@COMMENT{{ concatenation of journals_ref.bib withpyblio.bib optimization.bib mypapers.bib other.bib refvulg.bib these_ref.bib philo.bib ../math/journals_ref.bib ../math/citeseer.bib ../math/books.bib }}
@COMMENT{{ date: Thu Nov 2 00:20:16 CET 2006 }}
@MISC{chaio2002heisenberg,
AUTHOR = {R. Y. Chiao, P. G. Kwiat},
TITLE = {Heisenberg's Introduction of the `Collapse of the
Wavepacket' into Quantum Mechanics},
YEAR = {2001},
NOTE = {Comments: 13 pages, 3 figures. Chiao's Heisenberg
Centennial Symposium lecture given in Bamberg,
Germany, in Sept. 2001},
ROPSECTIONS = {QUANTPHYS},
URL = {http://fr.arxiv.org/abs/quant-ph/0201036},
PS = {/sci_docs/physics/papers/arxiv/chaio2002heisenberg.ps.gz},
ABSTRACT = {Heisenberg in 1929 introduced the "collapse of the
wavepacket" into quantum theory. We review here an
experiment at Berkeley which demonstrated several
aspects of this idea. In this experiment, a pair of
daughter photons was produced in an entangled state,
in which the sum of their two energies was equal to
the sharp energy of their parent photon, in the
nonlinear optical process of spontaneous parametric
down-conversion. The wavepacket of one daughter
photon collapsed upon a measurement-at-a-distance of
the other daughter's energy, in such a way that the
total energy of the two-photon system was
conserved. Heisenberg's energy-time uncertainty
principle was also demonstrated to hold in this
experiment.}
}
@MISC{delaMadrid2002pedestrian,
AUTHOR = {R. de la Madrid, M. Gadella},
TITLE = {A Pedestrian Introduction to Gamow Vectors},
YEAR = {2002},
URL = {http://fr.arxiv.org/abs/quant-ph/0201091},
PS = {/sci_docs/physics/papers/arxiv/delaMadrid2002pedestrian.ps.gz},
ROPSECTIONS = {SMATRIX QUANTPHYS},
ABSTRACT = { The Gamow vector description of resonances is
compared with the S-matrix and the Green function
descriptions using the example of the square barrier
and similar potentials. By imposing different
boundary conditions on the time independent
Schrodinger equation, we get either eigenvectors
corresponding to real eigenvalues (Dirac kets) and
the real ``physical'' spectrum or we get
eigenvectors corresponding to complex eigenvalues
(Gamow vectors) and the resonance spectrum. We will
show that the poles of the S-matrix are the same as
the poles of the Green function and as the complex
eigenvalues of the Schrodinger equation subject to a
purely outgoing boundary condition. We also obtain
the basis vector expansion generated by the Gamow
vectors. The time asymmetry built into the purely
outgoing boundary condition will be revealed. It
will be also shown that the probability to detect
the decay within a shell around the origin of the
decaying state follows the exponential law if the
Gamow vector (resonance) contribution to this
probability is the only contribution that is taken
into account. }
}
@ARTICLE{1464-4266-4-3-201,
AUTHOR = {T C Weinacht and P H Bucksbaum},
TITLE = {Using feedback for coherent control of quantum
systems},
JOURNAL = {Journal of Optics B: Quantum and Semiclassical
Optics},
VOLUME = {4},
NUMBER = {3},
PAGES = {R35-R52},
YEAR = {2002},
ROPSECTIONS = {PHYSX SURVEY QUANTPHYS},
PDF = {/sci_docs/physics/papers/JOpticsB/Weinacht2002using.pdf},
ABSTRACT = {A longstanding goal in chemical physics has been the
control of atoms and molecules using coherent light
fields. This paper provides a brief overview of the
field and discusses experiments that use a
programmable pulse shaper to control the quantum
state of electronic wavepackets in Rydberg atoms and
electronic and nuclear dynamics in molecular
liquids. The shape of Rydberg wavepackets was
controlled by using tailored ultrafast pulses to
excite a beam of caesium atoms. The quantum state of
these atoms was measured using holographic
techniques borrowed from optics. The experiments
with molecular liquids involved the construction of
an automated learning machine. A genetic algorithm
directed the choice of shaped pulses which
interacted with the molecular system inside a
learning control loop. Analysis of successful pulse
shapes that were found by using the genetic
algorithm yield insight into the systems being
controlled. }
}
@ARTICLE{kamefuchi,
AUTHOR = {S. Kamefuchi},
TITLE = {Some Considerations on Quantum Mechanics-Matter Wave
and Probability Wave},
JOURNAL = {Foundations of Physics},
YEAR = {1998},
VOLUME = {28},
NUMBER = {1},
PAGES = {31--43},
PUBLISHER = {Kluwer/Plenum},
URL = {http://leporello.catchword.com/vl=5116453/cl=15/nw=1/rpsv/catchword/plenum/00159018/v28n1/s2/p31},
PDF = {/sci_docs/physics/papers/FoundPhys/kamefuchi1998considerations.pdf},
ROPSECTIONS = {QUANTPHYS},
ABSTRACT = {It is argued that the distinction between matter
wave and probability wave is made clear when the
problem is considered from the field-theory
viewpoint . Interference can take place for each of
these waves , and the similarity as well as
dissimilarity between the two cases is discussed .}
}
@ARTICLE{braginsky1998galileo,
AUTHOR = { V. B. Braginsky},
TITLE = {From Galileo's Pendulum to a Quantum One (A Short
Review)},
JOURNAL = {Foundations of Physics },
YEAR = {1998},
VOLUME = {28},
NUMBER = {1},
PAGES = {125--130},
URL = {http://leporello.catchword.com/vl=5116453/cl=15/nw=1/rpsv/catchword/plenum/00159018/v28n1/s7/p125},
PDF = {/sci_docs/physics/papers/FoundPhys/braginsky1998galileo.pdf},
ROPSECTIONS = {QUANTPHYS SURVEY}
}
@ARTICLE{kimball1998states,
AUTHOR = {J. C. Kimball},
TITLE = {States on the Sierpinski Triangle},
JOURNAL = {Foundations of Physics },
YEAR = {1998},
VOLUME = {28},
NUMBER = {1},
PAGES = {87--105},
URL = {http://leporello.catchword.com/vl=5116453/cl=15/nw=1/rpsv/catchword/plenum/00159018/v28n1/s5/p87},
PDF = {/sci_docs/physics/papers/FoundPhys/kimball1998states.pdf},
ROPSECTIONS = {LOCALIZATION QUANTPHYS RG},
ABSTRACT = {States on a Sierpinski triangle are described using
a formally exact and general Hamiltonian
renormalization . The spectra of new (as well as
previously examined) models are characterized
. Numerical studies based on the renormalization
suggest that the only models which exhibit
absolutely continuous specta are effectively
one-dimensional in the limit of large distances . }
}
@ARTICLE{0034-4885-61-2-002,
AUTHOR = {Andrew Steane},
TITLE = {Quantum computing},
JOURNAL = {Reports on Progress in Physics},
VOLUME = {61},
NUMBER = {2},
PAGES = {117-173},
YEAR = {1998},
NOTE = {quant-ph/9708022},
URL = {http://xxx.lanl.gov/abs/quant-ph/9708022},
PDF = {/sci_docs/physics/papers/RepProgPhys/steane1997quantum.pdf},
ROPSECTIONS = {QUANTPHYS SURVEY},
ABSTRACT = {The subject of quantum computing brings together
ideas from classical information theory, computer
science, and quantum physics. This review aims to
summarize not just quantum computing, but the whole
subject of quantum information theory. Information
can be identified as the most general thing which
must propagate from a cause to an effect. It
therefore has a fundamentally important role in the
science of physics. However, the mathematical
treatment of information, especially information
processing, is quite recent, dating from the
mid-20th century. This has meant that the full
significance of information as a basic concept in
physics is only now being discovered. This is
especially true in quantum mechanics. The theory of
quantum information and computing puts this
significance on a firm footing, and has led to some
profound and exciting new insights into the natural
world. Among these are the use of quantum states to
permit the secure transmission of classical
information (quantum cryptography), the use of
quantum entanglement to permit reliable transmission
of quantum states (teleportation), the possibility
of preserving quantum coherence in the presence of
irreversible noise processes (quantum error
correction), and the use of controlled quantum
evolution for efficient computation (quantum
computation). The common theme of all these insights
is the use of quantum entanglement as a
computational resource. It turns out that
information theory and quantum mechanics fit
together very well. In order to explain their
relationship, this review begins with an
introduction to classical information theory and
computer science, including Shannon's theorem, error
correcting codes, Turing machines and computational
complexity. The principles of quantum mechanics are
then outlined, and the Einstein, Podolsky and Rosen
(EPR) experiment described. The EPR-Bell
correlations, and quantum entanglement in general,
form the essential new ingredient which
distinguishes quantum from classical information
theory and, arguably, quantum from classical
physics. Basic quantum information ideas are next
outlined, including qubits and data compression,
quantum gates, the `no cloning' property and
teleportation. Quantum cryptography is briefly
sketched. The universal quantum computer (QC) is
described, based on the Church-Turing principle and
a network model of computation. Algorithms for such
a computer are discussed, especially those for
finding the period of a function, and searching a
random list. Such algorithms prove that a QC of
sufficiently precise construction is not only
fundamentally different from any computer which can
only manipulate classical information, but can
compute a small class of functions with greater
efficiency. This implies that some important
computational tasks are impossible for any device
apart from a QC. To build a universal QC is well
beyond the abilities of current technology. However,
the principles of quantum information physics can be
tested on smaller devices. The current experimental
situation is reviewed, with emphasis on the linear
ion trap, high-Q optical cavities, and nuclear
magnetic resonance methods. These allow coherent
control in a Hilbert space of eight dimensions
(three qubits) and should be extendable up to a
thousand or more dimensions (10 qubits). Among other
things, these systems will allow the feasibility of
quantum computing to be assessed. In fact such
experiments are so difficult that it seemed likely
until recently that a practically useful QC
(requiring, say, 1000 qubits) was actually ruled out
by considerations of experimental imprecision and
the unavoidable coupling between any system and its
environment. However, a further fundamental part of
quantum information physics provides a solution to
this impasse. This is quantum error correction
(QEC). An introduction to QEC is provided. The
evolution of the QC is restricted to a carefully
chosen subspace of its Hilbert space. Errors are
almost certain to cause a departure from this
subspace. QEC provides a means to detect and undo
such departures without upsetting the quantum
computation. This achieves the apparently
impossible, since the computation preserves quantum
coherence even though during its course all the
qubits in the computer will have relaxed
spontaneously many times. The review concludes with
an outline of the main features of quantum
information physics and avenues for future
research.}
}
@ARTICLE{doncheski2002quantum,
AUTHOR = {M. A. Doncheski and R. W. Robinett},
TITLE = {Quantum Mechanical Analysis of the Equilateral
Triangle Billiard: Periodic Orbit Theory and Wave
Packet Revivals},
JOURNAL = { Annals of Physics},
YEAR = {2002},
VOLUME = {299},
NUMBER = {2},
PAGES = {208--227},
MONTH = {August},
ROPSECTIONS = {QUANTPHYS MULTISCATT},
PDF = {/sci_docs/physics/papers/AnnPhys/doncheski2002quantum.pdf},
ABSTRACT = {Using the fact that the energy eigenstates of the
equilateral triangle infinite well (or billiard) are
available in closed form, we examine the connections
between the energy eigenvalue spectrum and the
classical closed paths in this geometry, using both
periodic orbit theory and the short-term
semi-classical behavior of wave packets. We also
discuss wave packet revivals and show that there are
exact revivals, for all wave packets, at times given
by (Eq) where a and µ are the length of one side and
the mass of the point particle, respectively. We
find additional cases of exact revivals with shorter
revival times for zero-momentum wave packets
initially located at special symmetry points inside
the billiard. Finally, we discuss simple variations
on the equilateral (60°-60°-60°) triangle, such as
the half equilateral (30°-60°-90°) triangle and
other "foldings," which have related energy spectra
and revival structures.}
}
@ARTICLE{omnes1992consistent,
AUTHOR = {Roland Omn{\`e}s},
TITLE = {Consistent interpretations of quantum mechanics},
JOURNAL = {Rev. Mod. Phys.},
YEAR = {1992},
VOLUME = {64},
NUMBER = {2},
PAGES = {339--382},
MONTH = {April},
ROPSECTIONS = {QUANTPHYS},
URL = {http://link.aps.org/abstract/RMP/v64/p339},
PDF = {/sci_docs/physics/papers/RMP/omnes1992consistent.pdf},
ABSTRACT = {Within the last decade, significant progress has
been made towards a consistent and complete
reformulation of the Copenhagen interpretation (an
interpretation consisting in a formulation of the
experimental aspects of physics in terms of the
basic formalism; it is consistent if free from
internal contradiction and complete if it provides
precise predictions for all experiments). The main
steps involved decoherence (the transition from
linear superpositions of macroscopic states to a
mixing), Griffiths histories describing the
evolution of quantum properties, a convenient
logical structure for dealing with histories, and
also some progress in semiclassical physics, which
was made possible by new methods. The main outcome
is a theory of phenomena, viz., the classically
meaningful properties of a macroscopic system. It
shows in particular how and when determinism is
valid. This theory can be used to give a deductive
form to measurement theory, which now covers some
cases that were initially devised as counterexamples
against the Copenhagen interpretation. These
theories are described, together with their
applications to some key experiments and some of
their consequences concerning epistemology.}
}
@ARTICLE{oppenheim2002temporal,
AUTHOR = {J Oppenheim and B Reznik and W G Unruh},
TITLE = {Temporal ordering in quantum mechanics},
JOURNAL = {Journal of Physics A: Mathematical and General},
VOLUME = {35},
NUMBER = {35},
PAGES = {7641-7652},
YEAR = {2002},
ROPSECTIONS = {TIME QUANTPHYS},
PDF = {/sci_docs/physics/papers/JPhysA/oppenheim2002temporal.pdf},
ABSTRACT = {We examine the measurability of the temporal
ordering of two events, as well as event
coincidences. In classical mechanics, a measurement
of the order-of-arrival of two particles is shown to
be equivalent to a measurement involving only one
particle (in higher dimensions). In quantum
mechanics, we find that diffraction effects
introduce a minimum inaccuracy to which the temporal
order-of-arrival can be determined
unambiguously. The minimum inaccuracy of the
measurement is given by deltat = hbar/bar E where
bar E is the total kinetic energy of the two
particles. Similar restrictions apply to the case of
coincidence measurements. We show that these
limitations are much weaker than limitations on
measuring the time-of-arrival of a particle to a
fixed location.}
}
@ARTICLE{valdenebro2002assumptions,
AUTHOR = {Angel G Valdenebro},
TITLE = {Assumptions underlying Bell's inequalities},
JOURNAL = {European Journal of Physics},
VOLUME = {23},
NUMBER = {5},
PAGES = {569-577},
YEAR = {2002},
ROPSECTIONS = {QUANTPHYS},
PDF = {/sci_docs/physics/papers/NewJPhys/valdenebro2002assumptions.pdf},
ABSTRACT = {There are several versions of Bell's inequalities
(BI), proved in different contexts, using different
sets of assumptions. The discussions of their
experimental violation often disregard some required
assumptions and loosely use formulations of
others. The issue, to judge from recent
publications, continues to cause
misunderstandings. We present a very simple but
general proof of BI, identifying explicitly the
complete set of assumptions required. }
}
@ARTICLE{sica1999bell-I,
AUTHOR = {Louis Sica},
TITLE = {Bell's inequalities I: An explanation for their
experimental violation },
JOURNAL = {Optics Communications},
YEAR = {1999},
VOLUME = {170},
NUMBER = {1-3},
PAGES = {55-60},
MONTH = {October},
ROPSECTIONS = {QUANTPHYS},
PDF = {/sci_docs/physics/papers/OptComm/sica1999bell-II.pdf},
ABSTRACT = {Derivations of two Bell's inequalities are given in
a form appropriate to the interpretation of
experimental data for explicit determination of all
the correlations. They are arithmetic identities
independent of statistical reasoning and thus cannot
be violated by data that meets the conditions for
their validity. Two experimentally performable
procedures are described to meet these
conditions. Once such data are acquired, it follows
that the measured correlations cannot all equal a
negative cosine of angular differences. The relation
between this finding and the predictions of quantum
mechanics is discussed in a companion paper.}
}
@ARTICLE{sica1999bell-II,
AUTHOR = {Louis Sica},
TITLE = {Bell's inequalities II: Logical loophole in their
interpretation},
JOURNAL = {Optics Communications},
YEAR = {1999},
VOLUME = {170},
NUMBER = {1-3},
PAGES = {61-66},
MONTH = {October},
ROPSECTIONS = {QUANTPHYS},
PDF = {/sci_docs/physics/papers/OptComm/sica1999bell-II.pdf},
ABSTRACT = {Assumed data streams from a delayed choice gedanken
experiment must satisfy a Bell's identity
independently of locality assumptions. The violation
of Bell's inequality by assumed correlations of
identical form among these data streams implies that
they cannot all result from statistically equivalent
variables of a homogeneous process. This is
consistent with both the requirements of arithmetic
and distinctions between commuting and noncommuting
observables in quantum mechanics. Neglect of these
distinctions implies a logical loophole in the
conventional interpretation of Bell's inequalities.}
}
@ARTICLE{bell1964EPR,
AUTHOR = {J. S. Bell},
TITLE = {On the Einstein-Podolsky-Rosen Paradox},
JOURNAL = {Physics},
YEAR = {1964},
VOLUME = {1},
PAGES = {195--200},
ROPSECTIONS = {QUANTPHYS}
}
@ARTICLE{hall2002schrodinger,
AUTHOR = {Michael J W Hall and Marcel Reginatto},
TITLE = {Schr\"{o}dinger equation from an exact uncertainty
principle},
JOURNAL = {Journal of Physics A: Mathematical and General},
VOLUME = {35},
NUMBER = {14},
PAGES = {3289-3303},
YEAR = {2002},
ROPSECTIONS = {QUANTPHYS},
PDF = {/sci_docs/physics/papers/JPhysA/hall2002schrodinger.pdf},
ABSTRACT = {An exact uncertainty principle, formulated as the
assumption that a classical ensemble is subject to
random momentum fluctuations of a strength which is
determined by and scales inversely with uncertainty
in position, leads from the classical equations of
motion to the Schr\"{o}dinger equation. }
}
@INCOLLECTION{clauser2002early,
AUTHOR = {John F. Clauser},
TITLE = {Early history of Bell's theorem},
BOOKTITLE = {Quantum [un]speakable. From Bell to Quantum
Information.},
OPTCROSSREF = {},
PAGES = {61--98},
PUBLISHER = {Springer-Verlag},
YEAR = {2002},
EDITOR = {R. A. Bertlmann and A. Zeilinger},
ROPSECTIONS = {QUANTPHYS},
OPTVOLUME = {},
OPTNUMBER = {},
OPTSERIES = {},
OPTTYPE = {},
OPTCHAPTER = {},
OPTADDRESS = {},
OPTEDITION = {},
OPTMONTH = {},
OPTNOTE = {},
OPTANNOTE = {}
}
@ARTICLE{jirari2002renormalisation,
AUTHOR = {H. Jiraria and H. Kr\"{o}ger X. Q. Luo and G. Melkonyan and K. J. M. Moriarty},
TITLE = {Renormalisation in quantum mechanics },
JOURNAL = {Physics Letters A},
YEAR = {2002},
OPTKEY = {},
VOLUME = {303},
NUMBER = {5--6},
PAGES = {299--306},
MONTH = {October},
OPTNOTE = {},
OPTANNOTE = {},
PDF = {/sci_docs/physics/papers/PhysLettA/jirari2002renormalisation.pdf},
ROPSECTIONS = {RG QUANTPHYS},
ABSTRACT = {We study a recently proposed quantum action depending on
temperature. At zero temperature the quantum action is obtained
analytically and reproduces the exact ground state energy and wave
function. This is demonstrated for a number of cases with parity
symmetric confining potentials. In the case of the hydrogen atom, it
also reproduces exactly energy and wave function of a subset of
excited state (those of lowest energy for given angular momentum l)
and the quantum action is consistent with O(4) symmetry. In the case
of a double-well potential, the quantum action generates the ground
state of double-hump shape. In all cases we observe a coincidence
(in position) of minima of the quantum potential with maxima of the
wave function. The semi-classical WKB formula for the ground state
wave function becomes exact after replacing the parameters of the
classical action by those of quantum action.}
}
@ARTICLE{bassi2000general,
AUTHOR = {Angelo Bassi and GianCarlo Ghirardi},
TITLE = {A general argument against the universal validity of the superposition principle },
JOURNAL = {Physics Letters A},
YEAR = {2000},
VOLUME = {275},
NUMBER = {5--6},
PAGES = {373--381},
MONTH = {October},
PDF = {/sci_docs/physics/papers/PhysLettA/bassi2000general.pdf},
ROPSECTIONS = {QUANTPHYS},
ABSTRACT = {We reconsider a well-known problem of quantum theory,
i.e. the so-called measurement (or macro-objectification) problem,
and we rederive the fact that it gives rise to serious problems of
interpretation. The novelty of our approach derives from the fact
that the relevant conclusion is obtained in a completely general
way, in particular, without resorting to any of the assumptions of
ideality which are usually done for the measurement process. The
generality and unescapability of our assumptions (we take into
account possible malfunctionings of the apparatus, its unavoidable
entanglement with the environmment, its high but not absolute
reliability, its fundamentally uncontrollable features) allow to
draw the conclusion that the very possibility of performing
measurements on a microsystem combined with the assumed general
validity of the linear nature of quantum evolution leads to a
fundamental contradiction. }
}
@ARTICLE{grangier2002contextual,
AUTHOR = {Philippe Grangier},
TITLE = {Contextual objectivity: a realistic interpretation of quantum mechanics},
JOURNAL = {European Journal of Physics},
VOLUME = {23},
NUMBER = {3},
PAGES = {331-337},
YEAR = {2002},
PDF = {/sci_docs/physics/papers/JPhysA/grangier2002contextual.pdf},
ROPSECTIONS = {QUANTPHYS},
ABSTRACT = {An attempt is made to formulate quantum mechanics (QM) in
physical rather than in mathematical terms. It is argued that the
appropriate conceptual framework for QM is `contextual objectivity',
which includes an objective definition of the quantum state. This
point of view sheds new light on topics such as the reduction
postulate and the quantum measurement process. }
}
@ARTICLE{zeh2003quantization,
AUTHOR = {H. D. Zeh},
TITLE = {There is no "first" quantization},
JOURNAL = {Physics Letters A},
YEAR = {2003},
VOLUME = {309},
NUMBER = {5--6},
PAGES = {329--334},
MONTH = {March},
ROPSECTIONS = {QFT QUANTPHYS},
PDF = {/sci_docs/physics/papers/PhysLettA/zeh2003quantization.pdf},
ABSTRACT = {The introduction of spinor and other massive fields by
"quantizing" particles (corpuscles) is conceptually misleading. Only
spatial fields must be postulated to form the fundamental objects to
be quantized (that is, to define a formal basis for all quantum
states), while apparent "particles" are a mere consequence of
decoherence. This conclusion is also supported by the nature of
gauge fields.}
}
@ARTICLE{agnese1997clues,
AUTHOR = {A. Agnese and R. Festa},
TITLE = {Clues to discretization on the cosmic scale},
JOURNAL = {Physics Letters A},
YEAR = {1997},
VOLUME = {227},
PAGES = {165},
ROPSECTIONS = {QUANTPHYS COSMOLOGY},
PDF = {/sci_docs/physics/papers/PhysLettA/agnese1997clues.pdf}
}
@ARTICLE{taylor1997teaching,
AUTHOR = {Edwin F. Taylor and Stamatis Vokos and John M. O Meara and Nora S. Thornber},
TITLE = {Teaching Feynman s sum-over-paths quantum theory},
JOURNAL = {Computers in Physics},
YEAR = {1998},
VOLUME = {12},
NUMBER = {2},
PAGES = {190--199},
ROPSECTIONS = {LECTURE QUANTPHYS},
PDF = {/sci_docs/physics/papers/computerInPhysics/taylor1997teaching.pdf},
ABSTRACT = {We outline an introduction to quantum mechanics based on the
sum-over-paths method originated by Richard P. Feynman. Students use
software with a graphics interface to model sums associated with
multiple paths for photons and electrons, leading to the concepts of
electron wavefunction, the propagator, bound states, and stationary
states. Material in the first portion of this outline has been tried
with an audience of high-school science teachers. These students were
enthusiastic about the treatment, and we feel that it has promise for
the education of physicists and other scientists, as well as for
distribution to a wider audience. }
}
@ARTICLE{1998A&A...335..281H,
AUTHOR = {{Hermann}, R. and {Schumacher}, G. and {Guyard}, R.},
TITLE = {{Scale relativity and quantization of the solar system. Orbit quantization of the planet's satellites}},
JOURNAL = {Astron. Astrophysics},
YEAR = 1998,
MONTH = JUL,
VOLUME = 335,
PAGES = {281-286},
ADSURL = {http://adsabs.harvard.edu/cgi-bin/nph-bib_query?bibcode=1998A%26A...335..281H&db_key=AST},
ADSNOTE = {Provided by the NASA Astrophysics Data System},
PDF = {/sci_docs/physics/papers/AstronAstrophys/hermann1998scale_relativity.pdf},
ROPSECTIONS = {QUANTPHYS}
}
@COMMENT{{ThisfilehasbeengeneratedbyPybliographer}}
@BOOK{cohen1973mecanique,
AUTHOR = {Claude Cohen-Tannoudji and Bernard Diu and Franck Lalo{\"e}},
ALTEDITOR = {},
TITLE = {M{\'e}canique quantique},
PUBLISHER = {Hermann},
YEAR = {1973},
VOLUME = {I et II},
ROPSECTIONS = {QUANTPHYS}
}
@MISC{accardi2000locality,
AUTHOR = {Luigi Accardi and Massimo Regoli},
TITLE = {Locality and Bell's inequality},
YEAR = {2000},
HOWPUBLISHED = { A talk given at Capri conference},
MONTH = {July},
NOTE = {quant-ph/0007005 -- 23 pages},
ROPSECTIONS = {QUANTPHYS},
PS = {/sci_docs/physics/papers/arxiv/accardi2000locality.ps.gz},
ABSTRACT = {We prove that the locality condition is irrelevant
to Bell in equality. We check that the real origin
of the Bell's inequality is the assumption of
applicability of classical (Kolmogorovian)
probability theory to quantum mechanics. We describe
the chameleon effect which allows to construct an
experiment realizing a local, realistic, classical,
deterministic and macroscopic violation of the Bell
inequalities. }
}
@MISC{adenier2000refutation,
AUTHOR = {Guillaume Adenier},
TITLE = {A Refutation of Bell's Theorem},
HOWPUBLISHED = {http://fr.arxiv.org/abs/quant-ph/0006014},
OPTMONTH = {June},
YEAR = {2000},
ROPSECTIONS = {QUANTPHYS},
ABSTRACT = {Bell's Theorem was developed on the basis of
considerations involving a linear combination of
spin correlation functions, each of which has a
distinct pair of arguments. The simultaneous
presence of these different pairs of arguments in
the same equation can be understood in two radically
different ways: either as `strongly objective,' that
is, all correlation functions pertain to the same
set of particle pairs, or as `weakly objective,'
that is, each correlation function pertains to a
different set of particle pairs. It is demonstrated
that once this meaning is determined, no discrepancy
appears between local realistic theories and quantum
mechanics: the discrepancy in Bell's Theorem is due
only to a meaningless comparison between a local
realistic inequality written within the strongly
objective interpretation (thus relevant to a single
set of particle pairs) and a quantum mechanical
prediction derived from a weakly objective
interpretation (thus relevant to several different
sets of particle pairs). }
}
@ARTICLE{cramer1986transactional,
AUTHOR = {John G. Cramer},
TITLE = {The transactional interpretation of quantum
mechanics},
JOURNAL = {Rev. Mod. Phys.},
YEAR = {1986},
VOLUME = {58},
PAGES = {647--688},
MONTH = {July},
ROPSECTIONS = {QUANTPHYS},
URLDOCUMENT = {/sci_docs/physics/papers/RMP/TI/}
}
@ARTICLE{youssef1993quantum,
AUTHOR = {S. Youssef},
TITLE = {Quantum Mechanics as Complex Probability Theory},
JOURNAL = {Mod.Phys.Lett. A},
YEAR = {1994},
VOLUME = {9},
PAGES = {2571-2586},
URL = {http://fr.arxiv.org/abs/hep-th/9307019},
PS = {/sci_docs/physics/papers/arxiv/youssef1993quantum.ps.gz},
ROPSECTIONS = {QUANTPHYS BAYES},
NOTE = {http://fr.arxiv.org/abs/hep-th/9307019},
ABSTRACT = {Realistic quantum mechanics based on complex
probability theory is shown to have a frequency
interpretation, to coexist with Bell's theorem, to
be linear, to include wavefunctions which are
expansions in eigenfunctions of Hermitian operators
and to describe both pure and mixed
systems. Illustrative examples are given. The
quantum version of Bayesian inference is
discussed. }
}
This file has been generated by
bibtex2html 1.46
. Bibliography collected by S. Correia.