Decoherence and the Appearance of a Classical World in Quantum TheoryErich Joos, H. Dieter Zeh, Claus Kiefer, Domenico J. W. Giulini, Joachim Kupsch, Ion-Olimpiu Stamatescu Springer Science & Business Media, 9 มี.ค. 2013 - 496 หน้า When we were preparing the first edition of this book, the concept of de coherence was known only to a minority of physicists. In the meantime, a wealth of contributions has appeared in the literature - important ones as well as serious misunderstandings. The phenomenon itself is now experimen tally clearly established and theoretically well understood in principle. New fields of application, discussed in the revised book, are chaos theory, informa tion theory, quantum computers, neuroscience, primordial cosmology, some aspects of black holes and strings, and others. While the first edition arose from regular discussions between the authors, thus leading to a clear" entanglement" of their otherwise quite different chap ters, the latter have thereafter evolved more or less independently. While this may broaden the book's scope as far as applications and methods are con cerned, it may also appear confusing to the reader wherever basic assumptions and intentions differ (as they do). For this reason we have rearranged the or der of the authors: they now appear in the same order as the chapters, such that those most closely related to the "early" and most ambitious concept of decoherence are listed first. The first three authors (Joos, Zeh, Kiefer) agree with one another that decoherence (in contradistinction to the Copen hagen interpretation) allows one to eliminate primary classical concepts, thus neither relying on an axiomatic concept of observables nor on a probability interpretation of the wave function in terms of classical concepts. |
จากด้านในหนังสือ
ผลการค้นหา 6 - 10 จาก 95
หน้า 21
... environment . A macroscopic measurement device is always asssumed to decohere into its macroscopic pointer states . However , environment - induced decoherence by itself does not yet solve the measure- ment problem , since the " pointer ...
... environment . A macroscopic measurement device is always asssumed to decohere into its macroscopic pointer states . However , environment - induced decoherence by itself does not yet solve the measure- ment problem , since the " pointer ...
หน้า 23
... environment , they cannot be described by an S - matrix at all . The unacceptable Born - von Neumann dynamical dualism was evidently the major motivation for an ignorance interpretation of the wave function . It attempts to explain the ...
... environment , they cannot be described by an S - matrix at all . The unacceptable Born - von Neumann dynamical dualism was evidently the major motivation for an ignorance interpretation of the wave function . It attempts to explain the ...
หน้า 25
... environment ( for example in the form of heat ) in order to reset the measurement or registration device ( second step of Fig . 2.1 ) . The reason is that two different states cannot deterministically evolve into the same final state ...
... environment ( for example in the form of heat ) in order to reset the measurement or registration device ( second step of Fig . 2.1 ) . The reason is that two different states cannot deterministically evolve into the same final state ...
หน้า 26
... environment a + b 0 0 ' measurement ' interaction Sensemble = So- kln2 Sphysical So- kln2 = | = 0 co + 0 a A O b B Sensemble = So - kln2 ( Sphysical So + kln2 ) = | = ? a A 0 or ( by reduction of resulting ensemble ) collapse reset ...
... environment a + b 0 0 ' measurement ' interaction Sensemble = So- kln2 Sphysical So- kln2 = | = 0 co + 0 a A O b B Sensemble = So - kln2 ( Sphysical So + kln2 ) = | = ? a A 0 or ( by reduction of resulting ensemble ) collapse reset ...
หน้า 27
... environment of ( 2.5 ) would be absolutely unrealistic for macroscopic pointer states n ) , this superposition remains nonetheless valid if is defined to include the " rest of the universe " , such as Pn ) = | On ) | Xn ) , with an envi ...
... environment of ( 2.5 ) would be absolutely unrealistic for macroscopic pointer states n ) , this superposition remains nonetheless valid if is defined to include the " rest of the universe " , such as Pn ) = | On ) | Xn ) , with an envi ...
เนื้อหา
1 | |
6 | |
41 | |
Decoherence in Quantum Field Theory | 181 |
Consistent Histories and Decoherence | 227 |
Giulini | 259 |
Open Quantum Systems | 316 |
Stochastic Collapse Models | 357 |
Related Concepts and Methods | 383 |
A1 Equation of Motion of a Mass Point | 394 |
Green Functions | 402 |
A4 Quantum Correlations | 415 |
A6 Galilean Symmetry | 425 |
A7 Stochastic Processes | 432 |
Stochastic Differential Equations | 439 |
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คำและวลีที่พบบ่อย
algebra approximation assumed atom Brownian motion Chap classical coherence collapse commute components corresponding coupling decay decohered decoherence defined degrees of freedom density matrix dependence derived described diagonal Diósi discussed dynamics eigenstates electromagnetic ensemble entanglement entropy environment equation of motion evolution example exponential field formal Gaussian Ghirardi given Hamiltonian Heisenberg picture hence Hilbert space initial interaction interference interpretation Kiefer leads linear macroscopic master equation models molecules momentum Neumann nonlocal observables oscillator parameter particle phase space photon Phys physical pointer position probability projection properties pure quantum mechanics quantum system quantum theory quantum Zeno effect reduced density matrix representation represented result rotation scattering Schrödinger equation Sect spacetime spatial statistical operator stochastic subspaces subsystem superposition principle superselection rules superselection sectors symmetry timescale tion transition unitary variables vector wave function wave packets Wigner function Zurek