Titlebook: Lectures on Integrable Systems; Jens Hoppe Book 1992 Springer-Verlag Berlin Heidelberg 1992 Dynamische Systeme.Hamiltonian.Hamiltonian mec

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书目名称Lectures on Integrable Systems影响因子(影响力)




书目名称Lectures on Integrable Systems影响因子(影响力)学科排名




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书目名称Lectures on Integrable Systems网络公开度学科排名




书目名称Lectures on Integrable Systems被引频次




书目名称Lectures on Integrable Systems被引频次学科排名




书目名称Lectures on Integrable Systems年度引用




书目名称Lectures on Integrable Systems年度引用学科排名




书目名称Lectures on Integrable Systems读者反馈




书目名称Lectures on Integrable Systems读者反馈学科排名

Flustered

Solution of a Quantum Mechanical ,-Body Problem,total momentum operator . commutes with (3.1) (due to the potential . depending only on the differences of the particle coordinates) the eigenfunctions ψ of (3.1) may be chosen to be also eigenfunctions of .; let us restrict ourselves to functions satisfying

RLS898

Lumbar-Spine

,Integrable Systems and gl(∞),echanics to (quantum) field theory having many different aspects, and in concrete models various physical interpretations, we will choose a purely . point of view — as in the context of integrable systems this turns out to be rather useful (yielding, e.g., a large class of possibilities which would

sigmoid-colon

Integrable Field Theories from Poisson Algebras,Poisson-bracket {,} on some space of functions from a (compact) manifold to the field ℂ (or IR), e.g. . — which is . of the type (10.1) — there exists an additional . assotiative multiplication, which is the one implied when writing . ., e.g., and which is the ordinary multiplication of functions. C

马赛克

Generalized Garnier Systems and Membranes,here exists another type of non-linear interaction, which is rather special: the class of quartic potentials. In the finite dimensional case, FWM [.] used the Lax-representation of the non-linear Schrödinger model to generalize the original work of Garnier [.]. In a compact notation (and dropping a

Intrepid

CBC471

Zero Curvature Conditions on ,,, Trigonometrical and Universal Enveloping Algebras,ties involved a finite number of . and . dependent fields . .(.) (. = 1 ... .), that made up .. The constant matrix . was chosen diagonal, and the construction of the constants of motion relied on the possibility to ‘diagonalize’ . by means of a similarity transformation ., which required the soluti

Hippocampus

Spectral Transform and Solitons,mportant role since then. Curiously, it uses the formulation (and abstract solution) of a problem known from quantum mechanics, namely that of solving . for given .(.), which is supposed to be a smooth real function and to go to zero (sufficiently fast) as . → ± ∞.

jaundiced