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Titlebook: Magnetic Excitations and Fluctuations II; Proceedings of an In Umberto Balucani,Stephen W. Lovesey,Valerio Tognet Conference proceedings 19

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书目名称Magnetic Excitations and Fluctuations II
副标题Proceedings of an In
编辑Umberto Balucani,Stephen W. Lovesey,Valerio Tognet
视频video
丛书名称Springer Proceedings in Physics
图书封面Titlebook: Magnetic Excitations and Fluctuations II; Proceedings of an In Umberto Balucani,Stephen W. Lovesey,Valerio Tognet Conference proceedings 19
出版日期Conference proceedings 19871st edition
关键词computer simulation; mathematical physics; mechanics; statistical mechanics
版次1
doihttps://doi.org/10.1007/978-3-642-73107-5
isbn_softcover978-3-642-73109-9
isbn_ebook978-3-642-73107-5Series ISSN 0930-8989 Series E-ISSN 1867-4941
issn_series 0930-8989
copyrightSpringer-Verlag Berlin Heidelberg 1987
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Statistical Mechanics of the Integrable Modelsling constant c < 0; the “repulsive” has c > 0; φ is complex. In (1.1) and (1.2) m is a mass (ħ = c = 1) and φ is real. These 4 integrable models are in one space and one time (1+1) dimensions. There are integrable models in 2+1 dimensions we cannot discuss here [1].
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Chaotic Dynamics of Spin Wave Instabilitiesin waves when pumped above the threshold for parametric excitation. However their extensive work fell short of connecting the spin wave turbulence phenomena with the modern ideas of chaotic dynamics of nonlinear dissipative systems.
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Lattice Equations, Hierarchies and Hamiltonian Structuresntegrable lattice equations are obtained in the form of Bianchi identities expressing the commutativity of BT’s. The integrable equations with one or more continuous variables and their direct linearizations are obtained applying suitable continuum limits to the lattice equation and the integral equation at the same time.
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On a Symmetric (2,+1)-State System Coupled to Its Environment: Tunneling Splitting and Quantum Coherhe level splitting between the two states that come from the bare states ∣±M>, provided the spin is set in a state ∣M> initially and if the transfer coupling is weak, AS « DS.. When S = ½, it is given exactly by. (2)where △ = A.S. This oscillation is one example of quantum coherence caused by quantum tunneling.
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Springer Proceedings in Physicshttp://image.papertrans.cn/m/image/621223.jpg
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