Derive the Heisenberg Hamiltonian in the Dyson-Maleev representation of spins.
Neglect the terms containing more than two boson operators, and determine the
elementary excitations of the system. Under what circumstances
is this approximation justified?
(The Heisenberg Hamiltonian is
; the Dyson-Maleev representation expresses
the spin operator at site i as
,
and
, where
and
are boson creation
and annihilation operators, in units of
.)
Laszlo Mihaly
Thu Oct 31 13:23:11 EST 1996