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 11 - 15 จาก 95
หน้า 28
... environment a + b O 0 " measurement " interaction a A + O B Sensemble = So - kln2 Sensemble = Sphysical So - kln2 = 1 = 0 So - kln2 Sphysical So + kln2 = | = ? a A A " a + or ( by branching ) reset decoherence b B B " ( forget ) ...
... environment a + b O 0 " measurement " interaction a A + O B Sensemble = So - kln2 Sensemble = Sphysical So - kln2 = 1 = 0 So - kln2 Sphysical So + kln2 = | = ? a A A " a + or ( by branching ) reset decoherence b B B " ( forget ) ...
หน้า 29
... environments ) could well remain in a superposition of drastically different situations until he observes ( or communicates with ) them ! Environment - induced decoherence means that an avalanche of other causal chains unavoidably ...
... environments ) could well remain in a superposition of drastically different situations until he observes ( or communicates with ) them ! Environment - induced decoherence means that an avalanche of other causal chains unavoidably ...
หน้า 34
... environment , thus leading in turn to slightly different effective Hamiltonians for the gas . This will in general have strong ( " chaotic " ) effects in the microscopic states which form the original ensemble , and thus induce ...
... environment , thus leading in turn to slightly different effective Hamiltonians for the gas . This will in general have strong ( " chaotic " ) effects in the microscopic states which form the original ensemble , and thus induce ...
หน้า 35
... environment , say ) , | 4 ) = Σ Cmn | ¿ system environment m , n n " ( 2.10 ) does not factorize in any basis . The expectation values of all local observables , A = Asystem 11environment ( 2.11 ) are calculated by " tracing out " the ...
... environment , say ) , | 4 ) = Σ Cmn | ¿ system environment m , n n " ( 2.10 ) does not factorize in any basis . The expectation values of all local observables , A = Asystem 11environment ( 2.11 ) are calculated by " tracing out " the ...
หน้า 36
... environment ) , or the consequence of averaging over an ensemble of unknown ( but nonetheless entangled ) states ... environment , in order to write the total state as a single sum , ( Ψ ) = Σ VPK | System | environment ( 2.16 ) While ...
... environment ) , or the consequence of averaging over an ensemble of unknown ( but nonetheless entangled ) states ... environment , in order to write the total state as a single sum , ( Ψ ) = Σ VPK | System | environment ( 2.16 ) While ...
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 |
ฉบับอื่นๆ - ดูทั้งหมด
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