Noncommutative determinants, Cauchy-Binet formulae, and Capelli-type identities II. Grassmann and quantum oscillator algebra representation

preprint2013arXivOpen access

Abstract

We prove that, for XX, YY, AA and BB matrices with entries in a non-commutative ring such that [Xij,Ykℓ]=−AiℓBkj[X_{ij},Y_{k\ell}]=-A_{i\ell} B_{kj}, satisfying suitable commutation relations (in particular, XX is a Manin matrix), the following identity holds: coldetXcoldetY=<0∣coldet(aA+X(I−a†B)−1Y)∣0> \mathrm{coldet} X \mathrm{coldet} Y = < 0 | \mathrm{coldet} (a A + X (I-a^{\dagger} B)^{-1} Y) |0 > . Furthermore, if also YY is a Manin matrix, coldetXcoldetY=∫D(ψ,ψ†)exp⁡[∑k≥01k+1(ψ†Aψ)k(ψ†XBkYψ)] \mathrm{coldet} X \mathrm{coldet} Y =\int \mathcal{D}(ψ, ψ^{\dagger}) \exp [ \sum_{k \geq 0} \frac{1}{k+1} (ψ^{\dagger} A ψ)^{k} (ψ^{\dagger} X B^k Y ψ) ] . Notations: <0∣ < 0 |, ∣0>| 0 >, are respectively the bra and the ket of the ground state, a†a^{\dagger} and aa the creation and annihilation operators of a quantum harmonic oscillator, while ψi†ψ^{\dagger}_i and ψiψ_i are Grassmann variables in a Berezin integral. These results should be seen as a generalization of the classical Cauchy-Binet formula, in which AA and BB are null matrices, and of the non-commutative generalization, the Capelli identity, in which AA and BB are identity matrices and [Xij,Xkℓ]=[Yij,Ykℓ]=0[X_{ij},X_{k\ell}]=[Y_{ij},Y_{k\ell}]=0.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.