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 1 - 5 จาก 80
หน้า 17
... pure and exhaustive ( that is , complete , Pn = 1 ) , they represent a basis of the corresponding Hilbert space . By introducing an arbitrary " measurement scale " an , one may construct general observables A Σn ) an ( n , which permit ...
... pure and exhaustive ( that is , complete , Pn = 1 ) , they represent a basis of the corresponding Hilbert space . By introducing an arbitrary " measurement scale " an , one may construct general observables A Σn ) an ( n , which permit ...
หน้า 25
... pure states and x , respectively , of ob- server and environment : ( a ) + | b ) ) | 0 ) | xo ) . The global Schrödinger evolution 9 Bennett did not define physical entropy to include that of the microscopic en- semble a , b , since he ...
... pure states and x , respectively , of ob- server and environment : ( a ) + | b ) ) | 0 ) | xo ) . The global Schrödinger evolution 9 Bennett did not define physical entropy to include that of the microscopic en- semble a , b , since he ...
หน้า 31
... pure matter of taste whether Occam's razor is applied to the wave func- tion ( by adding appropriate but not directly detectable collapse - producing nonlinear terms to its dynamical law ) , or to the dynamical law ( by instead adding ...
... pure matter of taste whether Occam's razor is applied to the wave func- tion ( by adding appropriate but not directly detectable collapse - producing nonlinear terms to its dynamical law ) , or to the dynamical law ( by instead adding ...
หน้า 34
... ( pure ) quantum state instead of being postu- lated by means of quantization rules . According to Sect . 2.2 , the probability for a state In ) to be " found " in a state | a ) in an appropriate measurement is given by ( na ) | 2 . Its ...
... ( pure ) quantum state instead of being postu- lated by means of quantization rules . According to Sect . 2.2 , the probability for a state In ) to be " found " in a state | a ) in an appropriate measurement is given by ( na ) | 2 . Its ...
หน้า 35
... pure ( completely defined ) global state ( V ) , is defined by a partial trace , osystem ) system ( system psystem = ΣΦ : = m , m ' trenv { V ) ( V } = Σosystem ) Cmncm'n ( system , m , m ' n ' m ' ( 2.13 ) where tr = trsystem trenv ...
... pure ( completely defined ) global state ( V ) , is defined by a partial trace , osystem ) system ( system psystem = ΣΦ : = m , m ' trenv { V ) ( V } = Σosystem ) Cmncm'n ( system , m , m ' n ' m ' ( 2.13 ) where tr = trsystem trenv ...
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