How to define quantum Turing machines?

Problem Detail: 

In quantum computation, what is the equivalent model of a Turing machine? It is quite clear to me how quantum circuits can be constructed out of quantum gates, but how can we define a quantum Turing machine (QTM) that can actually benefit from quantum effects, namely, perform on high-dimensional systems?

Asked By : Ran G.

Answered By : Ran G.

^{(note: the full desciption is a bit complex, and has several subtleties which I prefered to ignore. The following is merely the high-level ideas for the QTM model)}

When defining a Quantum Turing machine (QTM), one would like to have a simple model, similar to the classical TM (that is, a finite state machine plus an infinite tape), but allow the new model the advantage of quantum mechanics.

Similarly to the classical model, QTM has:

1. $Q=\{q_0,q_1,..\}$ - a finite set of states. Let $q_0$ be an initial state.
2. $\Sigma=\{\sigma_0,\sigma_1,...\}$, $\Gamma=\{\gamma_0,..\}$ - set of input/working alphabet
3. an infinite tape and a single "head".

However, when defining the transition function, one should recall that any quantum computation must be reversible. Recall that a configuration of TM is the tuple $C=(q,T,i)$ denoting that the TM is at state $q\in Q$, the tape contains $T\in \Gamma^*$ and the head points to the $i$th cell of the tape.

Since, at any given time, the tape consist only a finite amount of non-blank cells, we define the (quantum) state of the QTM as a unit vector in the Hilbert space $\mathcal{H}$ generated by the configuration space $Q\times\Sigma^*\times \mathrm{Z}$. The specific configuration $C=(q,T,i)$ is represented as the state $$|C\rangle = |q\rangle |T\rangle |i\rangle.$$ _{(remark: Therefore, every cell in the tape isa $\Gamma$-dimensional Hilbert space.)}

The QTM is initialized to the state $|\psi(0)\rangle = |q_0\rangle |T_0\rangle |1\rangle$, where $T_0\in \Gamma^*$ is concatenation of the input $x\in\Sigma^*$ with many "blanks" as needed (there is a subtlety here to determine the maximal length, but I ignore it).

At each time step, the state of the QTM evolves according to some unitary $U$ $$|\psi(i+1)\rangle = U|\psi(i)\rangle$$

Note that the state at any time $n$ is given by $|\psi(n)\rangle = U^n|\psi(0)\rangle$. $U$ can be any unitary that "changes" the tape only where the head is located and moves the head one step to the right or left. That is, $\langle q',T',i'|U|q,T,i\rangle$ is zero unless $i'= i \pm 1$ and $T'$ differs from $T$ only at position $i$.

At the end of the computation (when the QTM reaches a state $q_f$) the tape is being measured (using, say, the computational basis).

The interesting thing to notice, is that each "step" the QTM's state is a superposition of possible configurations, which gives the QTM the "quantum" advantage.

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The answer is based on Masanao Ozawa, On the Halting Problem for Quantum Turing Machines. See also David Deutsch, Quantum theory, the Church-Turing principle and the universal quantum computer.

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Question Source : http://cs.stackexchange.com/questions/125