L. Ciotti, H. Zhao, T. de Zeeuw
We study mass models that correspond to MOND (triaxial) potentials for which
the Hamilton-Jacobi equation separates in ellipsoidal coordinates. The problem
is first discussed in the simpler case of deep-MOND systems, and then
generalized to the full MOND regime. We prove that the Kuzmin property for
Newtonian gravity still holds, i.e., that the density distribution of separable
potentials is fully determined once the density profile along the minor axis is
assigned. At variance with the Newtonian case, the fact that a positive density
along the minor axis leads to a positive density everywhere remains unproven.
We also prove that (i) all regular separable models in MOND have a vanishing
density at the origin, so that they would correspond to centrally dark-matter
dominated systems in Newtonian gravity; (ii) triaxial separable potentials
regular at large radii and associated with finite total mass leads to density
distributions that at large radii are not spherical and decline as ln(r)/r^5;
(iii) when the triaxial potentials admit a genuine Frobenius expansion with
exponent 0View original: http://arxiv.org/abs/1202.1723
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