It is shown that with every Lax operator, which is a pseudodifferential operator of nonzero leading order, is associated a KP hierarchy. For each such operator, we construct the second Gelfand–Dikii bracket associated with the Lax equation and show that it defines a Hamiltonian structure. When the leading order is positive the corresponding compatible first Hamiltonian structure, which turns out, in general, to be different from the naive first Gelfand–Dikii bracket is derived. The corresponding Hamiltonian structures for the constrained Lax operator, where the next to leading‐order term vanishes or has a constant coefficient, is discussed.
REFERENCES
1.
2.
3.
4.
A. C. Newell, Solitonsin Mathematical Physics (SIAM, Philadelphia, 1985).
5.
L. D. Faddeev and L. A. Takhtajan, Hamiltonian Methods in the Theory of Solitons (Springer-Verlag, New York, 1987).
6.
A. Das, Integrable Models (World Scientific, Singapore, 1989).
7.
8.
9.
10.
I.M. Gelfand and L. A. Dikii, Preprint No. 136, Inst. Appl. Math. Acad. Sci. USSR, 1978.
11.
12.
13.
14.
15.
16.
17.
See, for example, P. DiFrancesco, C. Itzykson, and J. B. Zuber, NSF-ITP-90-193, SPhT/90–149, PUPT-1211 (1990).
18.
19.
20.
J. M.
Figueroa-O’Farrill
, J.
Mas
, and E.
Ramos
, Phys. Lett. B
266
, 298
(1991
).21.
F. Yu and Y. S. Wu, Utah preprint (1991).
This content is only available via PDF.
© 1992 American Institute of Physics.
1992
American Institute of Physics
You do not currently have access to this content.