Weyl's unitary matrices, which were introduced in Weyl's 1927 paper on group
theory and quantum mechanics, are
p×p unitary matrices given by the
diagonal matrix whose entries are the
p-th roots of unity and the cyclic
shift matrix. Weyl's unitaries, which we denote by
u and $\mathfrak
v
,satisfy\mathfrak u^p=\mathfrak v^p=1_p
(thep\times p$ identity matrix)
and the commutation relation $\mathfrak u\mathfrak v=\zeta \mathfrak v\mathfrak
u
,where\zeta
isaprimitivep$-th root of unity. We prove that Weyl's
unitary matrices are universal in the following sense: if
u and
v are any
d×d unitary matrices such that
up=vp=1d and
uv=ζvu, then
there exists a unital completely positive linear map $\phi:\mathcal M_p(\mathbb
C)\rightarrow\mathcal M_d(\mathbb C)
suchthat\phi(\mathfrak u)= u$ and
ϕ(v)=v. We also show, moreover, that any two pairs of
p-th
order unitary matrices that satisfy the Weyl commutation relation are
completely order equivalent.
When
p=2, the Weyl matrices are two of the three Pauli matrices from
quantum mechanics. It was recently shown that
g-tuples of Pauli-Weyl-Brauer
unitaries are universal for all
g-tuples of anticommuting selfadjoint unitary
matrices; however, we show here that the analogous result fails for positive
integers
p>2.
Finally, we show that the Weyl matrices are extremal in their matrix range,
using recent ideas from noncommutative convexity theory.