Abstract:
We propose a quantization of the Kadomtsev–Petviashvili equation
on a cylinder equivalent to an infinite system of nonrelativistic
one-dimensional bosons with the masses $m=1,2,\dots$.
The Hamiltonian is Galilei-invariant and includes the split and
merge terms $\Psi^{\dagger}_{m_1}\Psi^{\dagger}_{m_2} \Psi_{m_1+m_2}$
and $\Psi^{\dagger}_{m_1+m_2}\Psi_{m_1}\Psi_{m_2}$ for all
combinations of particles with masses $m_1$, $m_2$, and $m_1+m_2$
for a special choice of coupling constants. We construct
the Bethe eigenfunctions for the model and verify the consistency
of the coordinate Bethe ansatz and hence the quantum integrability
of the model up to the mass $M=8$ sector.