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Two-integral distribution functions for axisymmetric stellar systems with separable densities  [PDF]
Zhenglu Jiang,Leonid Ossipkov
Physics , 2008, DOI: 10.1111/j.1365-2966.2007.12514.x
Abstract: We show different expressions of distribution functions (DFs) which depend only on the two classical integrals of the energy and the magnitude of the angular momentum with respect to the axis of symmetry for stellar systems with known axisymmetric densities. The density of the system is required to be a product of functions separable in the potential and the radial coordinate, where the functions of the radial coordinate are powers of a sum of a square of the radial coordinate and its unit scale. The even part of the two-integral DF corresponding to this type of density is in turn a sum or an infinite series of products of functions of the energy and of the magnitude of the angular momentum about the axis of symmetry. A similar expression of its odd part can be also obtained under the assumption of the rotation laws. It can be further shown that these expressions are in fact equivalent to those obtained by using Hunter and Qian's contour integral formulae for the system. This method is generally computationally preferable to the contour integral method. Two examples are given to obtain the even and odd parts of their two-integral DFs. One is for the prolate Jaffe model and the other for the prolate Plummer model. It can be also found that the Hunter-Qian contour integral formulae of the two-integral even DF for axisymmetric systems can be recovered by use of the Laplace-Mellin integral transformation originally developed by Dejonghe.
Separable triaxial potential-density pairs in MOND  [PDF]
L. Ciotti,H. Zhao,T. de Zeeuw
Physics , 2012, DOI: 10.1111/j.1365-2966.2012.20716.x
Abstract: 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 0
The Casimir Energy in a Separable Potential  [PDF]
R. L. Jaffe,L. R. Williamson
Physics , 1999, DOI: 10.1006/aphy.2000.6041
Abstract: The Casimir energy is the first-order-in-\hbar correction to the energy of a time-independent field configuration in a quantum field theory. We study the Casimir energy in a toy model, where the classical field is replaced by a separable potential. In this model the exact answer is trivial to compute, making it a good place to examine subtleties of the problem. We construct two traditional representations of the Casimir energy, one from the Greens function, the other from the phase shifts, and apply them to this case. We show that the two representations are correct and equivalent in this model. We study the convergence of the Born approximation to the Casimir energy and relate our findings to computational issues that arise in more realistic models.
Chirally motivated separable potential model for $ηN$ amplitudes  [PDF]
A. Cieply,J. Smejkal
Physics , 2013, DOI: 10.1016/j.nuclphysa.2013.10.003
Abstract: We analyze the $\eta N$ interaction using a coupled channel separable potential model that implements the chiral symmetry. The model predicts an $\eta N$ stattering length $\Re a_{\eta N} \approx 0.7$ fm and in-medium subthreshold attraction most likely sufficient to generate $\eta$-nuclear bound states. The energy dependence of the $\eta N$ amplitude and pole content of the model are discussed. An idea of the same origin of the baryon resonances $N^{\star}(1535)$ and $N^{\star}(1650)$ is presented.
Inverse Scattering Problem for the Schr?dinger Operator with a Separable Potential  [PDF]
Yu. P. Chuburin
Mathematics , 2005,
Abstract: We prove that the inverse scattering problem for the Schr\"odinger operator with the separable potential can be reduced to the solving of a certain singular integral equation. We establish the uniqueness of the potential corresponding to given scattering amplitude in the class of separable potentials.
Exactly separable version of the Bohr Hamiltonian with the Davidson potential  [PDF]
Dennis Bonatsos,E. A. McCutchan,N. Minkov,R. F. Casten,P. Yotov,D. Lenis,D. Petrellis,I. Yigitoglu
Physics , 2008, DOI: 10.1103/PhysRevC.76.064312
Abstract: An exactly separable version of the Bohr Hamiltonian is developed using a potential of the form u(beta)+u(gamma)/beta^2, with the Davidson potential u(beta)= beta^2 + beta_0^4/beta^2 (where beta_0 is the position of the minimum) and a stiff harmonic oscillator for u(gamma) centered at gamma=0. In the resulting solution, called exactly separable Davidson (ES-D), the ground state band, gamma band and 0_2^+ band are all treated on an equal footing. The bandheads, energy spacings within bands, and a number of interband and intraband B(E2) transition rates are well reproduced for almost all well-deformed rare earth and actinide nuclei using two parameters (beta_0, gamma stiffness). Insights regarding the recently found correlation between gamma stiffness and the gamma-bandhead energy, as well as the long standing problem of producing a level scheme with Interacting Boson Approximation SU(3) degeneracies from the Bohr Hamiltonian, are also obtained.
The separable analogue of Kerr in Newtonian gravity  [PDF]
K. Glampedakis,T. A. Apostolatos
Physics , 2013, DOI: 10.1088/0264-9381/30/5/055006
Abstract: General Relativity's Kerr metric is famous for its many symmetries which are responsible for the separability of the Hamilton-Jacobi equation governing the geodesic motion and of the Teukolsky equation for wave dynamics. We show that there is a unique stationary and axisymmetric Newtonian gravitational potential that has exactly the same dual property of separable point-particle and wave motion equations. This `Kerr metric analogue' of Newtonian gravity is none other than Euler's 18th century problem of two-fixed gravitating centers.
Potential-density pairs for axisymmetric galaxies: the influence of scalar fields  [PDF]
M. A. Rodriguez-Meza,Jorge L. Cervantes-Cota,M. I. Pedraza,J. F. Tlapanco,E. M. De la Calleja
Physics , 2005, DOI: 10.1007/s10714-005-0067-2
Abstract: We present a formulation for potential-density pairs to describe axisymmetric galaxies in the Newtonian limit of scalar-tensor theories of gravity. The scalar field is described by a modified Helmholtz equation with a source that is coupled to the standard Poisson equation of Newtonian gravity. The net gravitational force is given by two contributions: the standard Newtonian potential plus a term stemming from massive scalar fields. General solutions have been found for axisymmetric systems and the multipole expansion of the Yukawa potential is given. In particular, we have computed potential-density pairs of galactic disks for an exponential profile and their rotation curves.
Solutions of Three-Dimensional Separable Non-Central Potential

Ozlem Yesiltas,

中国物理快报 , 2008,
Abstract: We show that a wide class of non-central potentials can be analysed via the improved picture of the Nikiforov--Uvarov method Physica Scripta 75(2007)686]. It has been shown that using the alternative approach, polynomialsolutions of three-dimensional separable non-central potential can be obtained.
The 2H Electric Dipole Moment in a Separable Potential Approach  [cached]
Gibson B.F.,Afnan I.R.
EPJ Web of Conferences , 2010, DOI: 10.1051/epjconf/20100304016
Abstract: Measurement of the electric dipole moment (EDM) of 2H or of 3He may well come prior to the coveted measurement of the neutron EDM. Exact model calculations for the deuteron are feasible, and we explore here the model dependence of such deuteron EDM calculations. We investigate in a separable potential approach the relationship of the full model calculation to the plane wave approximation, correct an error in an early potential model result, and examine the tensor force aspects of the model results as well as the e ect of the short range repulsion found in the realistic, contemporary potential model calculations of Liu and Timmermans. We conclude that, because one-pion exchange dominates the EDM calculation, separable potential model calculations should provide an adequate picture of the 2H EDM until better than 10% measurements are achieved.
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