53 research outputs found
On the Equivalence of Different Lax Pairs for the Kac-van Moerbeke Hierarchy
We give a simple algebraic proof that the two different Lax pairs for the
Kac-van Moerbeke hierarchy, constructed from Jacobi respectively
super-symmetric Dirac-type difference operators, give rise to the same
hierarchy of evolution equations. As a byproduct we obtain some new recursions
for computing these equations.Comment: 8 page
Intersection local times of independent fractional Brownian motions as generalized white noise functionals
In this work we present expansions of intersection local times of fractional
Brownian motions in , for any dimension , with arbitrary Hurst
coefficients in . The expansions are in terms of Wick powers of white
noises (corresponding to multiple Wiener integrals), being well-defined in the
sense of generalized white noise functionals. As an application of our
approach, a sufficient condition on for the existence of intersection local
times in is derived, extending the results of D. Nualart and S.
Ortiz-Latorre in "Intersection Local Time for Two Independent Fractional
Brownian Motions" (J. Theoret. Probab.,20(4)(2007), 759-767) to different and
more general Hurst coefficients.Comment: 28 page
Point Interaction in two and three dimensional Riemannian Manifolds
We present a non-perturbative renormalization of the bound state problem of n
bosons interacting with finitely many Dirac delta interactions on two and three
dimensional Riemannian manifolds using the heat kernel. We formulate the
problem in terms of a new operator called the principal or characteristic
operator. In order to investigate the problem in more detail, we then restrict
the problem to one particle sector. The lower bound of the ground state energy
is found for general class of manifolds, e.g., for compact and Cartan-Hadamard
manifolds. The estimate of the bound state energies in the tunneling regime is
calculated by perturbation theory. Non-degeneracy and uniqueness of the ground
state is proven by Perron-Frobenius theorem. Moreover, the pointwise bounds on
the wave function is given and all these results are consistent with the one
given in standard quantum mechanics. Renormalization procedure does not lead to
any radical change in these cases. Finally, renormalization group equations are
derived and the beta-function is exactly calculated. This work is a natural
continuation of our previous work based on a novel approach to the
renormalization of point interactions, developed by S. G. Rajeev.Comment: 43 page
Gauge-Invariant Quasi-Free States on the Algebra of the Anyon Commutation Relations
Let and let , . For and from , we define a function to be equal to if , and to if . Let , () be operator-valued distributions such that is the adjoint of . We say that , satisfy the anyon commutation relations (ACR) if for and for . In particular, for , the ACR become the canonical commutation relations and for , the ACR become the canonical anticommutation relations. We define the ACR algebra as the algebra generated by operator-valued integrals of , . We construct a class of gauge-invariant quasi-free states on the ACR algebra. Each state from this class is completely determined by a positive self-adjoint operator on the real space which commutes with any operator of multiplication by a bounded function . In the case ), we discuss the corresponding particle density . For , using a renormalization, we rigorously define a vacuum state on the commutative algebra generated by operator-valued integrals of . This state is given by a negative binomial point process. A scaling limit of these states as gives the gamma random measure, depending on parameter
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