Librería: Anybook.com, Lincoln, Reino Unido
EUR 34,33
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Añadir al carritoCondición: Good. Volume 1880. This is an ex-library book and may have the usual library/used-book markings inside.This book has soft covers. In good all round condition. Please note the Image in this listing is a stock photo and may not match the covers of the actual item,650grams, ISBN:9783540309918.
Librería: Romtrade Corp., STERLING HEIGHTS, MI, Estados Unidos de America
EUR 57,35
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Añadir al carritoCondición: New. This is a Brand-new US Edition. This Item may be shipped from US or any other country as we have multiple locations worldwide.
Librería: Basi6 International, Irving, TX, Estados Unidos de America
EUR 57,35
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Añadir al carritoCondición: Brand New. New. US edition. Expediting shipping for all USA and Europe orders excluding PO Box. Excellent Customer Service.
Librería: Ria Christie Collections, Uxbridge, Reino Unido
EUR 72,60
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Añadir al carritoCondición: New. In.
Librería: BennettBooksLtd, Los Angeles, CA, Estados Unidos de America
EUR 102,21
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Añadir al carritopaperback. Condición: New. In shrink wrap. Looks like an interesting title!
Idioma: Inglés
Publicado por Springer, Springer Vieweg, 2006
ISBN 10: 3540309918 ISBN 13: 9783540309918
Librería: AHA-BUCH GmbH, Einbeck, Alemania
EUR 69,54
Cantidad disponible: 2 disponibles
Añadir al carritoTaschenbuch. Condición: Neu. Druck auf Anfrage Neuware - Printed after ordering - This is the rst in a series of three volumes dedicated to the lecture notes of the Summer School 'Open Quantum Systems' which took place at the Institut Fourier in Grenoble from June 16th to July 4th 2003. The contributions presented in these volumes are revised and expanded versions of the notes provided to the students during the School. Closed vs. Open Systems By de nition, the time evolution of a closed physical systemS is deterministic. It is usually described by a differential equation x = X(x ) on the manifold M of t t possible con gurations of the system. If the initial con guration x M is known 0 then the solution of the corresponding initial value problem yields the con guration x at any future time t. This applies to classical as well as to quantum systems. In the t classical case M is the phase space of the system and x describes the positions and t velocities of the various components (or degrees of freedom) ofS at time t. Inthe quantum case, according to the orthodoxinterpretation of quantum mechanics, M is a Hilbert space and x a unit vector - the wave function - describing the quantum t state of the system at time t. In both cases the knowledge of the state x allows t to predict the result of any measurement made onS at time t.