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The '''Toda lattice''', introduced by {{harvs|txt|first=Morikazu |last=Toda|authorlink=Morikazu Toda|year=1967}}, is a simple model for a one-dimensional crystal
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in [[solid state physics]]. It is given by a chain of particles with nearest neighbor interaction
described by the equations of motion
:<math> \begin{align}
\frac{d}{dt} p(n,t) &= e^{-(q(n,t) - q(n-1,t))} - e^{-(q(n+1,t) - q(n,t))}, \\
\frac{d}{dt} q(n,t) &= p(n,t),
\end{align} </math>
where <math>q(n,t)</math> is the displacement of the <math>n</math>-th particle from its equilibrium position,
and <math>p(n,t)</math> is its momentum (mass <math>m=1</math>).
 
The Toda lattice is a prototypical example of a [[completely integrable system]] with [[soliton]] solutions. To see this one uses [[Hermann Flaschka|Flaschka]]'s variables
:<math> a(n,t) = \frac{1}{2} {\rm e}^{-(q(n+1,t) - q(n,t))/2}, \qquad b(n,t) = -\frac{1}{2} p(n,t) </math>
such that the Toda lattice reads
:<math> \begin{align}
\dot{a}(n,t) &= a(n,t) \Big(b(n+1,t)-b(n,t)\Big), \\
\dot{b}(n,t) &= 2 \Big(a(n,t)^2-a(n-1,t)^2\Big).
\end{align}</math>
Then one can verify that the Toda lattice is equivalent to the Lax equation
:<math>\frac{d}{dt} L(t) = [P(t), L(t)]</math>
where [''L'',&nbsp;''P''] =&nbsp;''LP''&nbsp;-&nbsp;''PL'' is the [[commutator]] of two [[operator (mathematics)|operator]]s. The operators ''L'' and ''P'', the [[Lax pair]], are [[linear operators]] in the [[Hilbert space]] of square summable sequences <math>\ell^2(\mathbb{Z})</math> given by
:<math> \begin{align}
L(t) f(n) &= a(n,t) f(n+1) + a(n-1,t) f(n-1) + b(n,t) f(n), \\
P(t) f(n) &= a(n,t) f(n+1) - a(n-1,t) f(n-1).
\end{align}</math>
The matrix <math>L(t)</math> has the property that its eigenvalues are invariant in time. These eigenvalues constitute independent integrals of motion, therefore the Toda lattice is completely integrable.
In particular, the Toda lattice can be solved by virtue of the [[inverse scattering transform]] for the [[Jacobi operator]] ''L''. The main result implies that arbitrary (sufficiently fast) decaying initial conditions asymptotically for large ''t'' split into a sum of solitons and a decaying [[Dispersion (water waves)|dispersive]] part.
 
==References==
 
*{{citation|id={{MR|2493113}}|last=Krüger|first=Helge|last2=Teschl|first2= Gerald
|title=Long-time asymptotics of the Toda lattice for decaying initial data revisited
|journal=Rev. Math. Phys.|volume= 21 |year=2009|issue= 1|pages=  61-109|doi=10.1142/S0129055X0900358X}}
*{{citation|id={{MR|1711536}}|title=Jacobi Operators and Completely Integrable Nonlinear Lattices
|first=Gerald|last=Teschl|authorlink=Gerald Teschl|publisher=Amer. Math. Soc.|location=Providence|year=2000|url=http://www.mat.univie.ac.at/~gerald/ftp/book-jac/|isbn=0-8218-1940-2}}
*{{citation|id={{MR|1879178}}|last=Teschl|first= Gerald
|title=Almost everything you always wanted to know about the Toda equation
|journal=Jahresbericht der Deutschen Mathematiker-Vereinigung |volume= 103 |year=2001|issue= 4|pages= 149–162|url=http://www.mat.univie.ac.at/~gerald/ftp/articles/Toda.html}}
*Integrable Hamiltonians with Exponential Potential, Eugene Gutkin, Physica 16D (1985)  398-404.
*{{citation|first=Morikazu|last= Toda|title=Vibration of a chain with a non-linear interaction|journal= J. Phys. Soc. Japan |volume= 22 |year=1967|pages= 431–436|doi=10.1143/JPSJ.22.431}}
*{{citation|id={{MR|0971987}}|title=Theory of Nonlinear Lattices
|first=Morikazu|last= Toda|edition=2|publisher=Springer|location=Berlin|year=1989|isbn=978-0-387-10224-5|doi=10.1007/978-3-642-83219-2}}
 
==External links==
* E. W. Weisstein, [http://scienceworld.wolfram.com/physics/TodaLattice.html Toda Lattice] at ScienceWorld
* G. Teschl, [http://www.mat.univie.ac.at/~gerald/ftp/book-jac/toda.html The Toda Lattice]
 
[[Category:Exactly solvable models]]
[[Category:Solitons]]

Latest revision as of 20:18, 20 September 2014

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