arXiv subjects

Hiroshi Mizukawa

Publications and source records attributed to Hiroshi Mizukawa.

10 recordsLinked to original sources

arXiv2016

Interactions between Ehrenfest's urns arising from group actions

Ehrenfest's diffusion model is a well-known classical physical model consisting of two urns and n balls. A group theoretical interpretation of the model by using the Gelfand pair (Z/2Zwr S_{n},S_{n}) is provided by Diaconis-Shahshahani. This interpretation remains valid for an r-urns generalization, in which case, the corresponding Gelfand pair is (S_{r}wr S_{n},S_{r-1}wr S_{n}). In these models, there are no restrictions for ball movements, i.e., each balls can freely move to any urn. This paper introduces interactions between urns arising from actions of finite groups. The degree of freedom of ball movements is restricted by finite groups actions. Furthermore, for some cases, the existence of the cut-off phenomenons is shown.

math.PR↗

arXiv2015

Glaisher combinatorics of regular partitions

Extending the notion of $r$-(class) regular partitions, we define $(r_{1},...,r_{m})$-class regular partitions. A partition identity is presented and described by making use of the Glaisher correspondence.

math.CO↗

arXiv2013

Schur function identities arising from the basic representation of $A^{(2)}_{2}$

A Lie theoretic interpretation is given for some formulas of Schur functions and Schur $Q$-functions. Two realizations of the basic representation of the Lie algebra $A^{(2)}_2$ are considered; one is on the fermionic Fock space and the other is on the bosonic polynomial space. Via the boson-fermion correspondence, simple relations of the vacuum expectation values of fermions turn out to be algebraic relations of Schur functions.

math.RT↗

arXiv2011

Orthogonality Relations for Multivariate Krawtchouk Polynomials

The orthogonality relations of multivariate Krawtchouk polynomials are discussed. In case of two variables, the necessary and sufficient conditions of orthogonality is given by Grünbaum and Rahman in [SIGMA 6 (2010), 090, 12 pages, arXiv:1007.4327]. In this study, a simple proof of the necessary and sufficient condition of orthogonality is given for a general case.

math.CO↗

arXiv2010

Wreath Product Generalizations of the Triple $(S_{2n},H_{n},ϕ)$ and Their Spherical Functions

The symmetric group $S_{2n}$ and the hyperoctaheadral group $H_{n}$ is a Gelfand triple for an arbitrary linear representation $ϕ$ of $H_{n}$. Their $ϕ$-spherical functions can be caught as transition matrix between suitable symmetric functions and the power sums. We generalize this triplet in the term of wreath product. It is shown that our triplet are always to be a Gelfand triple. Furthermore we study the relation between their spherical functions and multi-partition version of the ring of symmetric functions.

math.RT↗

arXiv2010

Finite Gelfand Pair Approaches for Ehrenfest Diffusion Model

A classical diffusion model of Ehrenfest which consists of $2$-urns and $n$-balls is realized by a finite Gelfand pair $(H_{n},S_{n})$, where $H_{n}$ is the hyperoctahedral group and $S_{n}$ is the symmetric group. This fact can be generalized to multi-urn version by using Gelfand pairs of complex reflection groups.

math.CO↗

arXiv2008

Compound basis arising from the basic $A^{(1)}_{1}$-module

A new basis for the polynomial ring of infinitely many variables is constructed which consists of products of Schur functions and Q-functions. The transition matrix from the natural Schur function basis is investigated.

math.RT↗

arXiv2007

Compound basis for the space of symmetric functions

The aim of this note is to introduce a compound basis for the space of symmetric functions. Our basis consists of products of Schur functions and $Q$-functions. The basis elements are indexed by the partitions. It is well known that the Schur functions form an orthonormal basis for our space. A natural question arises. How are these two bases connected? In this note we present some numerical results of the transition matrix for these bases. In particular we will see that the determinant of the transition matrix is a power of 2. This is not a surprising fact. However the explicit formula involves an interesting combinatorial feature. Our compound basis comes from the twisted homogeneous realization of the basic representation of the affine Lie algebras. This note is not written in a standard style of mathematical articles. It is more like a draft of a talk. In particular proofs are not given here. Details and proofs will be published elsewhere.

math.RT↗

arXiv2007

Mixed expansion formula for the rectangular Schur functions and the affine Lie algebra A_1^(1)

Formulas are obtained that express the Schur S-functions indexed by Young diagrams of rectangular shape as linear combinations of "mixed" products of Schur's S- and Q-functions. The proof is achieved by using representations of the affine Lie algebra of type A_1^{(1)}. A realization of the basic representation that is of ``D_2^{(2)}''-type plays the central role.

math.RT↗

arXiv2002

Rectangular Schur functions and the basic representation of affine Lie algebras

An expression is given for the plethysm $p_{2}\circ S_{\square}$, where $p_{2}$ is the power sum of degree two and $S_{\square}$ is the Schur function indexed by a rectangular partition. The formula can be well understood from the viewpoint of the basic representation of the affine Lie algebra of type $A_{2}^{(2)}$.

math.CO↗