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

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書(shū)目名稱Magnetic Excitations and Fluctuations II影響因子(影響力)




書(shū)目名稱Magnetic Excitations and Fluctuations II影響因子(影響力)學(xué)科排名




書(shū)目名稱Magnetic Excitations and Fluctuations II網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Magnetic Excitations and Fluctuations II網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Magnetic Excitations and Fluctuations II被引頻次




書(shū)目名稱Magnetic Excitations and Fluctuations II被引頻次學(xué)科排名




書(shū)目名稱Magnetic Excitations and Fluctuations II年度引用




書(shū)目名稱Magnetic Excitations and Fluctuations II年度引用學(xué)科排名




書(shū)目名稱Magnetic Excitations and Fluctuations II讀者反饋




書(shū)目名稱Magnetic Excitations and Fluctuations II讀者反饋學(xué)科排名

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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 (? = 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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規(guī)范要多

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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 = ?, 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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