Physics Asked on July 23, 2021
In quantum computing, one of the central areas of study is to determine efficient quantum circuits – described by unitaries – to prepare a state $|psirangle$ from the initial computational basis state $|0cdots 0rangle$.
I am currently interested the mathematical abstraction of this problem; to be specific, if we have a $d$ dimensional Hilbert space, an initial state $|0rangle$ and a final state $|psirangle$, can we say anything about the set of unitaries $U$ such that $U|0rangle = |psirangle$? In particular, I am wondering about the following two things:
My guess to the first question is that this set of unitaries forms a submanifold of $U(d)$ of dimension $d^2 – d$ isomorphic to $U(d) / mathbb{C}^d$, but I am completely unsure about the second. Are there known answers to these questions, or in general is there anything that can be said about this class of unitaries?
Say your state space is $D = 2^d$ dimensions. Without loss of generality, consider an orthonormal basis of states we will label by $| i rangle$, where $i = 1 ldots D$, where $|1rangle = | psi rangle$, and $|i rangle$ for $i > 1$ are other random states.
In this basis, a few things become clear. If we have any block diagonal matrix of the form $$ U' = begin{pmatrix} 1 & mathbf{0} mathbf{0} & U_{D-1}end{pmatrix} $$ where $U_{D-1}$ is any $(D-1) times (D-1)$ matrix, then we clearly have $$ U' |psirangle = U' |1rangle = |1 rangle = |psi rangle. $$
Therefore, we have a whole $U(D-1)$ worth of transformations that preserve $|psi rangle$. If we have your matrix $U_0$, composing it with one of these matrices $U'$ will preserve the property that $(U' U_0) |0 ldots 0 rangle = |psi rangle$. In fact, once we have $U_0$, we can get all the other such matrices by simply multiplying it in this way $U' U_0$.
Correct answer by user1379857 on July 23, 2021
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