Archivo de la categoría: Math-Ph

HEM 2016: Inverse problems for Jacobi operators IV: Interior mass-spring perturbations of semi-infinite systems

hechoenmexico

Inverse problems for Jacobi operators IV: Interior mass-spring perturbations of semi-infinite systems

This work gives results on the interplay of the spectra of two Jacobi operators corresponding to an infinite mass-spring system and a modification of it obtained by changing one mass and one spring of the system. It is shown that the system can be recovered from these two spectra. Necessary and sufficient conditions for two sequences to be the spectra of the mass-spring system and the perturbed one are provided.

Comments: 37 pages 2 figures
Subjects: Mathematical Physics (math-ph)
MSC classes: 34K29, 47A75, 47B36, 70F17
Cite as: arXiv:1604.00099 [math-ph]
(or arXiv:1604.00099v1 [math-ph] for this version)

HEM 2016: SUSY partners of the truncated oscillator, Painlevé transcendents and Bäcklund transformations

hechoenmexico

SUSY partners of the truncated oscillator, Painlevé transcendents and Bäcklund transformations

In this work the supersymmetric technique is applied to the truncated oscillator to generate Hamiltonians ruled by second and third-order polynomial Heisenberg algebras, which are connected to the Painlev\’e IV and Painlev\’e V equations respectively. The aforementioned connection is exploited to produce particular solutions to both non-linear differential equations and the B\”acklund transformations relating them.

Comments: This article is a natural continuation of arXiv:1310.5628
Subjects: Mathematical Physics (math-ph); Quantum Physics (quant-ph)
Cite as: arXiv:1603.05173 [math-ph]
(or arXiv:1603.05173v1 [math-ph] for this version)

HEM 2016: Conformal Laplace superintegrable systems in 2D: polynomial invariant subspaces

hechoenmexico

Conformal Laplace superintegrable systems in 2D: polynomial invariant subspaces

2nd-order conformal superintegrable systems in n dimensions are Laplace equations on a manifold with an added scalar potential and 2n1 independent 2nd order conformal symmetry operators. They encode all the information about Helmholtz (eigenvalue) superintegrable systems in an efficient manner: there is a 1-1 correspondence between Laplace superintegrable systems and Stackel equivalence classes of Helmholtz superintegrable systems. In this paper we focus on superintegrable systems in two dimensions, n=2, where there are 44 Helmholtz systems, corresponding to 12 Laplace systems. For each Laplace equation we determine the possible 2-variate polynomial subspaces that are invariant under the action of the Laplace operator, thus leading to families of polynomial eigenfunctions. We also study the behavior of the polynomial invariant subspaces under a Stackel transform. The principal new results are the details of the polynomial variables and the conditions on parameters of the potential corresponding to polynomial solutions. The hidden gl_3-algebraic structure is exhibited for the exact and quasi-exact systems. For physically meaningful solutions, the orthogonality properties and normalizability of the polynomials are presented as well. Finally, for all Helmholtz superintegrable solvable systems we give a unified construction of 1D and 2D quasi-exactly solvable potentials possessing polynomial solutions, and a construction of new 2D PT-symmetric potentials is established.

Comments: 28 pages
Subjects: Mathematical Physics (math-ph)
MSC classes: 81Rxx, 33Cxx, 33C45
Cite as: arXiv:1602.03149 [math-ph]
(or arXiv:1602.03149v1 [math-ph] for this version)

HEM 2016:Observable currents in lattice field theories

hechoenmexico

Observable currents in lattice field theories

Observable currents are spacetime local objects that induce physical observables when integrated on an auxiliary codimension one surface. Since the resulting observables are independent of local deformations of the integration surface, the currents themselves carry most of the information about the induced physical observables. I study observable currents in a multisymplectic framework for Lagrangian field theory over discrete spacetime. A weak version of observable currents preserves many of their properties, while inducing a family of observables capable of separating points in the space of physically distinct solutions. A Poisson bracket gives the space of observable currents the structure of a Lie algebra. Peierls bracket for bulk observables gives an algebra homomorphism mapping equivalence classes of bulk observables to weak observable currents. The study covers scalar fields, nonlinear sigma models and gauge theories (including gauge theory formulations of general relativity) on the lattice. Even when this paper is entirely classical, this study is relevant for quantum field theory because a quantization of the framework leads to a spin foam model formulation of lattice field theory.

Comments: 29 pages, 1 figure
Subjects: Mathematical Physics (math-ph)
MSC classes: 53D42
Cite as: arXiv:1602.02304 [math-ph]
(or arXiv:1602.02304v1 [math-ph] for this version)

HEM 2016:New conditionally exactly solvable potentials of exponential type

hechoenmexico

New conditionally exactly solvable potentials of exponential type

Based on a method that produces the solutions to the Schrodinger equations of partner potentials, we give two conditionally exactly solvable partner potentials of exponential type defined on the half line. These potentials are multiplicative shape invariant and each of their linearly independent solution includes a sum of two hypergeometric functions. Furthermore we calculate the scattering amplitudes and study some of their properties.

Comments: 16 pages, 5 figures
Subjects: Mathematical Physics (math-ph); Quantum Physics (quant-ph)
Cite as: arXiv:1602.00405 [math-ph]
(or arXiv:1602.00405v1 [math-ph] for this version)

HEM 2016: Weakly bound states in heterogeneous waveguides: a calculation to fourth order

hechoenmexico

Weakly bound states in heterogeneous waveguides: a calculation to fourth order

We have extended a previous calculation of the energy of a weakly heterogeneous waveguide to fourth order in the density perturbation, deriving its general expression. For particular configurations where the second and third orders both vanish, we discover that the fourth order contribution lowers in general the energy of the state, below the threshold of the continuum. In these cases the waveguide possesses a localized state. We have applied our general formula to a solvable model with vanishing second and third orders reproducing the exact expression for the fourth order.

Comments: 16 pages, one table, two figures
Subjects: Mathematical Physics (math-ph)
Cite as: arXiv:1601.02470 [math-ph]
(or arXiv:1601.02470v1 [math-ph] for this version)

HEM 2016: Factorization of the transition matrix for the general Jacobi system

hechoenmexico

Factorization of the transition matrix for the general Jacobi system

The Jacobi system on a full-line lattice is considered when it contains additional weight factors. A factorization formula is derived expressing the scattering from such a generalized Jacobi system in terms of the scattering from its fragments. This is done by writing the transition matrix for the generalized Jacobi system as an ordered matrix product of the transition matrices corresponding to its fragments. The resulting factorization formula resembles the factorization formula for the Schr\”odinger equation on the full line.

Comments: 18 pages
Subjects: Mathematical Physics (math-ph)
MSC classes: 39A70, 47A40, 47A68, 47B36, 47B39
Cite as: arXiv:1601.04673 [math-ph]
(or arXiv:1601.04673v1 [math-ph] for this version)