{"title":"Malte Henkel","description":null,"products":[{"product_id":"non-equilibrium-phase-transitions-book-malte-henkel-9789401783729","title":"Non-Equilibrium Phase Transitions","description":"The importance of knowledge consists not only in its direct practical utility but also in the fact the it promotes a widely contemplative habit of mind; on this ground, utility is to be found in much of the knowledge that is nowadays labelled 'useless'.  Bertrand Russel, In Praise of Idleness, London (1935) Why are scientists in so many cases so deeply interested in their work ? Is it merely because it is useful ? It is only necessary to talk to such scientists to discover that the utilitarian possibilities of their work are generally of secondary interest to them. Something else is primary.  David Bohm, On creativity, Abingdon (1996) In this volume, the dynamical critical behaviour of many-body systems far from equilibrium is discussed. Therefore, the intrinsic properties of the - namics itself, rather than those of the stationary state, are in the focus of 1 interest. Characteristically, far-from-equilibrium systems often display - namical scaling, even if the stationary state is very far from being critical. A 1 As an example of a non-equilibrium phase transition, with striking practical c- sequences, consider the allotropic change of metallic ?-tin to brittle ?-tin. At o equilibrium, the gray ?-Sn becomes more stable than the silvery ?-Sn at 13. 2 C. Kinetically, the transition between these two solid forms of tin is rather slow at higher temperatures. It starts from small islands of ?-Sn, the growth of which proceeds through an auto-catalytic reaction.","brand":"WoB","offers":[{"title":"GB \/ NEW \/ INGRAM","offer_id":52147178438929,"sku":"NLS9789401783729","price":0.0,"currency_code":"GBP","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0784\/4072\/6801\/files\/9789401783729.jpg?v=1757599684"},{"product_id":"non-equilibrium-phase-transitions-book-malte-henkel-9789400796607","title":"Non-Equilibrium Phase Transitions","description":"This book describes two main classes of non-equilibrium phase-transitions: static and dynamics of transitions into an absorbing state, and dynamical scaling in far-from-equilibrium relaxation behavior and ageing.","brand":"WoB","offers":[{"title":"- \/ - \/ INTERNAL","offer_id":52336841130257,"sku":null,"price":0.0,"currency_code":"GBP","in_stock":true},{"title":"GB \/ NEW \/ INGRAM","offer_id":52336841556241,"sku":"NLS9789400796607","price":0.0,"currency_code":"GBP","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0784\/4072\/6801\/files\/9789400796607.jpg?v=1758164694"},{"product_id":"non-equilibrium-phase-transitions-book-malte-henkel-9789048128686","title":"Non-Equilibrium Phase Transitions","description":"The importance of knowledge consists not only in its direct practical utility but also in the fact the it promotes a widely contemplative habit of mind; on this ground, utility is to be found in much of the knowledge that is nowadays labelled 'useless'.  Bertrand Russel, In Praise of Idleness, London (1935) Why are scientists in so many cases so deeply interested in their work ? Is it merely because it is useful ? It is only necessary to talk to such scientists to discover that the utilitarian possibilities of their work are generally of secondary interest to them. Something else is primary.  David Bohm, On creativity, Abingdon (1996) In this volume, the dynamical critical behaviour of many-body systems far from equilibrium is discussed. Therefore, the intrinsic properties of the - namics itself, rather than those of the stationary state, are in the focus of 1 interest. Characteristically, far-from-equilibrium systems often display - namical scaling, even if the stationary state is very far from being critical. A 1 As an example of a non-equilibrium phase transition, with striking practical c- sequences, consider the allotropic change of metallic ?-tin to brittle ?-tin. At o equilibrium, the gray ?-Sn becomes more stable than the silvery ?-Sn at 13. 2 C. Kinetically, the transition between these two solid forms of tin is rather slow at higher temperatures. It starts from small islands of ?-Sn, the growth of which proceeds through an auto-catalytic reaction.","brand":"WoB","offers":[{"title":"GB \/ NEW \/ INGRAM","offer_id":52344152850705,"sku":"NLS9789048128686","price":0.0,"currency_code":"GBP","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0784\/4072\/6801\/files\/9789048128686.jpg?v=1758174371"},{"product_id":"conformal-invariance-and-critical-phenomena-book-malte-henkel-9783642084669","title":"Conformal Invariance and Critical Phenomena","description":"Critical phenomena arise in a wide variety of physical systems. Classi- cal examples are the liquid-vapour critical point or the paramagnetic- ferromagnetic transition. Further examples include multicomponent fluids and alloys, superfluids, superconductors, polymers and fully developed tur- bulence and may even extend to the quark-gluon plasma and the early uni- verse as a whole. Early theoretical investigators tried to reduce the problem to a very small number of degrees of freedom, such as the van der Waals equation and mean field approximations, culminating in Landau's general theory of critical phenomena. Nowadays, it is understood that the common ground for all these phenomena lies in the presence of strong fluctuations of infinitely many coupled variables. This was made explicit first through the exact solution of the two-dimensional Ising model by Onsager. Systematic subsequent developments have been leading to the scaling theories of critical phenomena and the renormalization group which allow a precise description of the close neighborhood of the critical point, often in good agreement with experiments. In contrast to the general understanding a century ago, the presence of fluctuations on all length scales at a critical point is emphasized today. This can be briefly summarized by saying that at a critical point a system is scale invariant. In addition, conformal invaTiance permits also a non-uniform, local rescal- ing, provided only that angles remain unchanged.","brand":"WoB","offers":[{"title":"GB \/ NEW \/ INGRAM","offer_id":52476407021841,"sku":"NLS9783642084669","price":0.0,"currency_code":"GBP","in_stock":true},{"title":"US \/ NEW \/ INGRAM","offer_id":52761802768657,"sku":"NIN9783642084669","price":0.0,"currency_code":"GBP","in_stock":false}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0784\/4072\/6801\/files\/9783642084669.jpg?v=1759844011"},{"product_id":"conformal-invariance-and-critical-phenomena-book-malte-henkel-9783540653219","title":"Conformal Invariance and Critical Phenomena","description":"Critical phenomena arise in a wide variety of physical systems. Classi- cal examples are the liquid-vapour critical point or the paramagnetic- ferromagnetic transition. Further examples include multicomponent fluids and alloys, superfluids, superconductors, polymers and fully developed tur- bulence and may even extend to the quark-gluon plasma and the early uni- verse as a whole. Early theoretical investigators tried to reduce the problem to a very small number of degrees of freedom, such as the van der Waals equation and mean field approximations, culminating in Landau's general theory of critical phenomena. Nowadays, it is understood that the common ground for all these phenomena lies in the presence of strong fluctuations of infinitely many coupled variables. This was made explicit first through the exact solution of the two-dimensional Ising model by Onsager. Systematic subsequent developments have been leading to the scaling theories of critical phenomena and the renormalization group which allow a precise description of the close neighborhood of the critical point, often in good agreement with experiments. In contrast to the general understanding a century ago, the presence of fluctuations on all length scales at a critical point is emphasized today. This can be briefly summarized by saying that at a critical point a system is scale invariant. 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Lecture 6 shows how familiar RG methods for equilibrium systems can be extended to systems far from equilibrium.","brand":"WoB","offers":[{"title":"- \/ - \/ INTERNAL","offer_id":52663120298257,"sku":null,"price":0.0,"currency_code":"GBP","in_stock":true},{"title":"GB \/ NEW \/ INGRAM","offer_id":52663121281297,"sku":"NLS9783540696834","price":0.0,"currency_code":"GBP","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0784\/4072\/6801\/files\/9783540696834.jpg?v=1762271190"},{"product_id":"conformal-invariance-an-introduction-to-loops-interfaces-and-stochastic-loewner-book-malte-henkel-9783642279331","title":"Conformal Invariance: an Introduction to Loops, Interfaces and Stochastic Loewner Evolution","description":"It then shows how to use conformal invariance to determine their properties.     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