Regularization of Toda lattices by Hamiltonian reduction

Nov, 1995
43 pages
Published in:
  • J.Geom.Phys. 21 (1997) 97-135
e-Print:
Report number:
  • INS-1123

Citations per year

199620022008201420183102
Abstract:
The Toda lattice defined by the Hamiltonian H=12i=1 npi 2+i=1 n1νie qiqi+1H={1\over 2} \sum_{i=1}~n p_i~2 + \sum_{i=1}~{n-1} \nu_i e~{q_i-q_{i+1}} with νi{±1}\nu_i\in \{ \pm 1\}, which exhibits singular (blowing up) solutions if some of the νi=1\nu_i=-1, can be viewed as the reduced system following from a symmetry reduction of a subsystem of the free particle moving on the group G=SL(n,\Real ). The subsystem is T GeT~*G_e, where Ge=N+ANG_e=N_+ A N_- consists of the determinant one matrices with positive principal minors, and the reduction is based on the maximal nilpotent group N+×NN_+ \times N_-. Using the Bruhat decomposition we show that the full reduced system obtained from T GT~*G, which is perfectly regular, contains 2 n12~{n-1} Toda lattices. More precisely, if nn is odd the reduced system contains all the possible Toda lattices having different signs for the νi\nu_i. If nn is even, there exist two non-isomorphic reduced systems with different constituent Toda lattices. The Toda lattices occupy non-intersecting open submanifolds in the reduced phase space, wherein they are regularized by being glued together. We find a model of the reduced phase space as a hypersurface in {\Real}~{2n-1}. If νi=1\nu_i=1 for all ii, we prove for n=2,3,4n=2,3,4 that the Toda phase space associated to T GeT~*G_e is a connected component of this hypersurface. The generalization of the construction for the other simple Lie groups is also presented.