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Suppose we have $k$ Hermitian matrices $H_1, ..., H_k \in M_d(\mathbb{C})$. Define $\mathfrak{g} = \langle iH_1, ... iH_k \rangle_{\text{Lie}}$ to be the Lie algebra generated by these Hermitian matrices (i.e. the vector space spanned by these matrices and all possible nested commutators). Assume also that $\operatorname{dim} \mathfrak{g} < d^2$, so that these matrices don't generate the entire $U(d)$.

Denote $G \subset U(d)$ as the group generated by matrices of the type $e^{itH_j}$. Denote also as $e^{\mathfrak{g}}$ the set of all unitary matrices that are exponents of some elements in $\mathfrak{g}$.

My question is, how do $G$ and $e^{\mathfrak{g}}$ relate to each other?

  1. $e^{\mathfrak{g}} \subseteq G$. This direction is apparently shown by Lloyd (1995) by showing that $e^{[iA, iB]t}$ can be performed to arbitrary precision.
  2. $G \subseteq e^{\mathfrak{g}}$. This is where it gets tricky. For small enough $\epsilon$, we know that $e^{i\epsilon H_l} e^{i\epsilon H_m}$ will belong to $e^\mathfrak{g}$ from the Baker-Campbell-Hausdorff formula, but for general case it's unclear. In other words, is it possible, by repeated multiplication of matrices of the type $e^{iH_j t}$, to obtain a unitary $U = e^{iF}$ such that $iF \notin \mathfrak{g}$?
Alexey Uvarov
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1 Answers1

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Theorem. Given $H_1, \ldots, H_k\in\mathbb C^{d\times d}$ Hermitian let $\mathfrak{g} := \langle iH_1, ... iH_k \rangle_{\text{Lie}}$ denote the associated Lie algebra and let $e^{\mathfrak g}$ be the corresponding Lie group. Moreover, let $G \subseteq U(d)$ be the group generated by all individual one-parameter groups $\{e^{itH_j}:t\in\mathbb R\}$. Then $G=e^{\mathfrak g}$.

Proof. $e^{\mathfrak g}\subseteq G$: Note that $e^{\mathfrak g}$ is a connected Lie group so the inclusion in question follows from Lemma 6.2 in Jurdjevic, Sussmann, "Control Systems on Lie Groups", Journal of Differential Equations 12, p.313-329 (1972). As a side note, in the qubit case such decompositions are known as Z-Y decomposition (and its generalizations), refer to Theorem 4.1 ff. in Nielsen & Chuang.

$G\subseteq e^{\mathfrak g}$: Given any $x\in G$, by definition of $G$ there exist $m\in\mathbb N$ and real numbers $\{t_{ab}:a=1,\ldots,k, b=1,\ldots,m\}$ such that $x=\prod_{j=1}^m e^{it_{1j}H_1}\cdot\ldots\cdot e^{it_{kj}H_k}$. Re-writing $$ x=\prod_{j=1}^m e^{i|t_{1j}|{\rm sgn}(t_{1j})H_1}\cdot\ldots\cdot e^{i|t_{kj}|{\rm sgn}(t_{kj})H_k} $$ shows that $x$ lies in the reachable set of the bilinear control system $\dot x(t)=\sum_{j=1}^ku_j(t)H_jx(t)$, $x(0)={\bf1}$ where the $u_j$ are piecewise constant functions which only take values $1$ and $- 1$. But this reachable set is equal to $e^{\mathfrak g}$, cf. Theorem 5.1 ff. in the previously cited Jurdjevic & Sussmann paper; hence $x\in e^{\mathfrak g}$ which concludes the proof. $\square$

Finally let me stress that your first inclusion $e^{\mathfrak g}\subseteq G$ does not follow from the arguments made in the paper of Lloyd you cited. The reason for this is that he implicitly requires either $e^{\mathfrak g}$ or $G$ to be closed (which need not be true in general).

  • His first argument---the Lie product formula for commutators (Eq.(2) in his paper)---implies $e^{\mathfrak g}\subseteq\overline{G}$, where the closure $\overline{G}$ of $G$ comes into play because we have to allow for approximations = the limit $n\to\infty$. If $G$ is closed, then this does indeed show $e^{\mathfrak g}\subseteq G$. However, $G$ need not be closed: he common counterexample here are irrational windings on a torus, e.g., $H={\rm diag}(1,\sqrt2)$ in which case $$ G=\{e^{itH}:t\in\mathbb R\}\subsetneq\overline{\{e^{itH}:t\in\mathbb R\}}=\{{\rm diag}(e^{i\theta_1},e^{i\theta_2}),\theta_1,\theta_2\in\mathbb R\}\,, $$ refer also to Proposition 2.5 in Elliott's book "Bilinear Control Systems", Springer (2009).
  • In his second argument---the "noninfinitesimal" construction---Lloyd argues that "if $\mathfrak g$ has finite dimension, [the space $e^{\mathfrak g}$] is compact: As a result, at most, a number of transformations proportional to the number of generators of $\mathfrak g$ is required to reach any desired transformation in the space". The mistake made here is that $\dim\mathfrak g<\infty$ does in general not imply compactness of $e^{\mathfrak g}$; again, irrational windings on a torus show that $e^{\mathfrak g}$ need not be closed.
Frederik vom Ende
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