The Ultimate Heisenberg group - American History Information Guide and Reference

In mathematics, the Heisenberg group, named after Werner Heisenberg, is a group of 3×3 upper triangular matrices of the form

$\begin{pmatrix} 1 & a & c\\ 0 & 1 & b\\ 0 & 0 & 1\\ \end{pmatrix}.$

Elements a,b,c can be taken from some (arbitrary) commutative ring.

Contents

1 Examples

2 General Heisenberg group

3 The connection with the Weyl algebra

4 Weyl's view of quantum mechanics

Examples

(i) If a,b,c are real numbers (in the ring R) then we get the continuous Heisenberg group. It is a nilpotent Lie group.

(ii) If a,b,c are integers (in the ring Z) then we get the discrete Heisenberg group H₃. It is a non-abelian nilpotent group. It has two generators

$x=\begin{pmatrix} 1 & 1 & 0\\ 0 & 1 & 0\\ 0 & 0 & 1\\ \end{pmatrix},\ \ y=\begin{pmatrix} 1 & 0 & 0\\ 0 & 1 & 1\\ 0 & 0 & 1\\ \end{pmatrix}$

and relations

$z^{}_{}=xyx^{-1}y^{-1},\ xz=zx,\ yz=zy$ ,

where

$z=\begin{pmatrix} 1 & 0 & 1\\ 0 & 1 & 0\\ 0 & 0 & 1\\ \end{pmatrix}$

is the generator of the center of H₃. By Bass' theorem, it has a polynomial growth rate of order 4.

(iii) If one takes a,b,c in Z/p Z, then we get the Heisenberg group modulo p. It is a group of order p³ with two generators, x, y and relations

$z^{}_{}=xyx^{-1}y^{-1},\ x^p=y^p=z^p=1,\ xz=zx,\ yz=zy$ .

General Heisenberg group

There are more general Heisenberg groups H_n. We begin by discussing the Real Heisenberg group of dimension 2n+1, for any integer n ≥ 1. As a group of matrices, H_n (or H_n(R) to indicate this is the Heisenberg group over the ring R) is defined as the group of square matrices of size n+2 with entries in R:

$\begin{bmatrix} 1 & a & c \\ 0 & 1_n & b \\ 0 & 0 & 1 \end{bmatrix}$

where a is a row vector of length n, b is a column vector of length n and 1_n is the identity matrix of size n. This is indeed a group, as is shown by the multiplication:

$\begin{bmatrix} 1 & a & c \\ 0 & 1_n & b \\ 0 & 0 & 1 \end{bmatrix} \times \begin{bmatrix}1 & a' & c' \\ 0 & 1_n & b' \\ 0 & 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & a+ a' & c+c' +a b' \\ 0 & 1_n & b+b' \\ 0 & 0 & 1 \end{bmatrix}$

and

$\begin{bmatrix} 1 & a & c \\ 0 & 1_n & b \\ 0 & 0 & 1 \end{bmatrix} \times \begin{bmatrix}1 & -a & -c +a b\\ 0 & 1_n & -b \\ 0 & 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & 0 & 0 \\ 0 & 1_n & 0 \\ 0 & 0 & 1 \end{bmatrix}.$

The Heisenberg group is a connected, simply connected Lie group whose Lie algebra consists of matrices

$\begin{bmatrix} 0 & a & c \\ 0 & 0_n & b \\ 0 & 0 & 0 \end{bmatrix},$

where a is a row vector of length n, b is a column vector of length n and 0_n is the zero matrix of size n. The exponential map is given by the following expression

$\exp \begin{bmatrix} 0 & a & c \\ 0 & 0_n & b \\ 0 & 0 & 0 \end{bmatrix} = \sum_{k=0}^\infty \frac{1}{k!}\begin{bmatrix} 0 & a & c \\ 0 & 0_n & b \\ 0 & 0 & 0 \end{bmatrix}^k = \begin{bmatrix} 1 & a & c + {1\over 2}a b\\ 0 & 1_n & b \\ 0 & 0 & 1 \end{bmatrix}.$

By choosing a basis e₁, ..., e_n of Rⁿ, and letting

$p_i = \begin{bmatrix} 0 & \operatorname{e}_i & 0 \\ 0 & 0_n & 0 \\ 0 & 0 & 0 \end{bmatrix}$

$q_j = \begin{bmatrix} 0 & 0 & 0 \\ 0 & 0_n & \operatorname{e}_j^{\mathrm{T}} \\ 0 & 0 & 0 \end{bmatrix}$

$z = \begin{bmatrix} 0 & 0 & 1\\ 0 & 0_n & 0 \\ 0 & 0 & 0 \end{bmatrix}$

the Lie algebra can also be characterized by the canonical commutation relations

$[p_i, q_j] = \delta_{ij}z \quad$

$[p_i, z] = 0 \quad$

$[q_j, z] = 0 \quad$

where p₁, .., p_n, q₁, .., q_n, z are generators. In particular, z is a central element of the Heisenberg Lie algebra.

This group occurs not only in quantum mechanics but in the theory of theta functions; it is also used in Fourier analysis. This group is also used in some formulations of the Stone-von Neumann theorem.

The above discussion (aside from statements referring to dimension and Lie group) applies if we replace R by any commutative ring A. The corresponding group is denoted H_n(A). Under the additional assumption that the prime 2 is invertible in the ring A the exponential map is also defined, since it reduces to a finite sum and has the form above (i.e. A could be a ring Z/pZ with an odd prime p or any field of characteristic 0).

The connection with the Weyl algebra

The Lie algebra $\mathfrak{h}_n$ of the Heisenberg group was described above as a Lie algebra of matrices. We now apply the Poincaré-Birkhoff-Witt theorem, to determine the universal enveloping algebra $\mathfrak{U}(\mathfrak{h}_n)$ . Among other properties, the universal enveloping algebra is an associative algebra into which $\mathfrak{h}_n$ injectively imbeds. By Poincaré-Birkhoff-Witt, it is the free vector space generated by the monomials

$z^j p_1^{k_1} p_2^{k_2} \cdots p_n^{k_n} q_1^{\ell_1} q_2^{\ell_2} \cdots q_n^{\ell_n}$

where the exponents are all non-negative. Thus $\mathfrak{U}(\mathfrak{h}_n)$ consists of real polynomials

$\sum_{\vec{k} \vec{\ell}} c_{j \ \vec{k} \ \vec{\ell}}\quad z^j p_1^{k_1} p_2^{k_2} \cdots p_n^{k_n} q_1^{\ell_1} q_2^{\ell_2} \cdots q_n^{\ell_n}$

with the commutation relations

$p_k p_\ell = p_\ell p_k, \quad q_k q_\ell = q_\ell q_k, \quad p_k q_\ell - q_\ell p_k = \delta_{k \ell} z, \quad z p_k - p_k z =0, \quad z q_k - q_k z =0$

$\mathfrak{U}(\mathfrak{h}_n)$ is closely related to the algebra of differential operators on Rⁿ with polynomial coefficients, since any such operator has a unique representation in the form:

$P = \sum_{\vec{k} \vec{\ell}} c_{\vec{k} \vec{\ell}}\quad \partial_{x_1}^{k_1} \partial_{x_2}^{k_2} \cdots \partial_{x_n}^{k_n} x_1^{\ell_1} x_2^{\ell_2} \cdots x_n^{\ell_n}$

This algebra is called the Weyl algebra. It follows from abstract nonsense that the Weyl algebra W_n is a quotient of $\mathfrak{U}(\mathfrak{h}_n)$ . However, this also easy to see directly from the above representations; viz, by the mapping

$z^j p_1^{k_1} p_2^{k_2} \cdots p_n^{k_n} q_1^{\ell_1} q_2^{\ell_2} \cdots q_n^{\ell_n} \rightarrow \partial_{x_1}^{k_1} \partial_{x_2}^{k_2} \cdots \partial_{x_n}^{k_n} x_1^{\ell_1} x_2^{\ell_2} \cdots x_n^{\ell_n}.$

Weyl's view of quantum mechanics

The application that led Hermann Weyl to an explicit introduction of the Heisenberg group was the question of why the Schrödinger picture and Heisenberg picture are physically equivalent. Abstractly there is a good explanation: the group H_n is a central extension of R²ⁿ by a copy of R, and as such is a semidirect product. Its representation theory is relatively simple (a special case of the later Mackey theory ), and in particular there is a uniqueness result for unitary representations with given action of the central element z (in the Lie algebra) or the one-parameter subgroup it creates under the exponential map, which is the central extension. This abstract uniqueness accounts for the equivalence of the two physical pictures.

The same uniqueness result was used by David Mumford for discrete Heisenberg groups, in his theory of abelian varieties. This is a large generalization of the approach used in Jacobi's elliptic functions, which is the case of the modulo 2 Heisenberg group, of order 8.

Categories: Group theory | Lie groups | Quantum mechanics

Your American History Reference Guide! - Heisenberg group

Heisenberg group

Examples

General Heisenberg group

The connection with the Weyl algebra

Weyl's view of quantum mechanics

Your American History Reference Guide!
- Heisenberg group