Abstract

IIt is shown that the celebrated Heun operator He=−(a0x3+a1x2+a2x)d2dx2+(b0x2+b1x+b2)ddx+c0xH_e=-(a_0 x^3 + a_1 x^2 + a_2 x) \frac{d^2}{dx^2} + (b_0 x^2 + b_1 x + b_2)\frac{d}{dx} + c_0 x is the Hamiltonian of the sl(2,R)sl(2,R)-quantum Euler-Arnold top of spin νν in a constant magnetic field. For a0≠0a_0 \neq 0 it is canonically-equivalent to BC1(A1)−BC_1(A_1)- Calogero-Moser-Sutherland quantum models, if a0=0a_0=0, ten known one-dimensional quasi-exactly-solvable problems are reproduced, and if, in addition, b0=c0=0b_0=c_0=0, then four well-known one-dimensional quantal exactly-solvable problems are reproduced. If spin νν of the top takes (half)-integer value the Hamiltonian possesses a finite-dimensional invariant subspace and a number of polynomial eigenfunctions occurs. Discrete systems on uniform and exponential lattices are introduced which are canonically-equivalent to one described by the Heun operator.

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