2000
DOI: 10.1142/9789812813435
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Theory of Critical Phenomena in Finite-Size Systems - Scaling and Quantum Effects

Abstract: Library of Congress Cataloging-in-PublicationAll rights reserved. This book, or parts thereof, may not be reproduced in any form or by any means, electronic or mechanical, including photocopying, recording or any information storage and retrieval system now known or to be invented, without written permission from the Publisher.For photocopying of material in this volume, please pay a copying fee through the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, USA. In this case permission to… Show more

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Cited by 146 publications
(378 citation statements)
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“…(1.7) implies a leading nonuniversal (cutoff dependent) non-scaling term ∼ L −2 in the behavior of the Casimir force, because the scaling function X sr (x) ∼ exp(−x) when x ≫ 1 [7,41,42,43,45]. Therefore Eqs.…”
Section: B Finite Size Scalingmentioning
confidence: 99%
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“…(1.7) implies a leading nonuniversal (cutoff dependent) non-scaling term ∼ L −2 in the behavior of the Casimir force, because the scaling function X sr (x) ∼ exp(−x) when x ≫ 1 [7,41,42,43,45]. Therefore Eqs.…”
Section: B Finite Size Scalingmentioning
confidence: 99%
“…Finite-size scaling asserts that near the bulk critical temperature T c the influence of a finite sample size L on critical phenomena is governed by universal finite-size scaling functions which depend on the ratio L/ξ, so that the rounding of the thermodynamic singularities sets in for L/ξ ≃ O(1) [7,41,42,43,44,45].…”
Section: B Finite Size Scalingmentioning
confidence: 99%
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