Quantcast
  • Register
PhysicsOverflow is a next-generation academic platform for physicists and astronomers, including a community peer review system and a postgraduate-level discussion forum analogous to MathOverflow.

Welcome to PhysicsOverflow! PhysicsOverflow is an open platform for community peer review and graduate-level Physics discussion.

Please help promote PhysicsOverflow ads elsewhere if you like it.

News

PO is now at the Physics Department of Bielefeld University!

New printer friendly PO pages!

Migration to Bielefeld University was successful!

Please vote for this year's PhysicsOverflow ads!

Please do help out in categorising submissions. Submit a paper to PhysicsOverflow!

... see more

Tools for paper authors

Submit paper
Claim Paper Authorship

Tools for SE users

Search User
Reclaim SE Account
Request Account Merger
Nativise imported posts
Claim post (deleted users)
Import SE post

Users whose questions have been imported from Physics Stack Exchange, Theoretical Physics Stack Exchange, or any other Stack Exchange site are kindly requested to reclaim their account and not to register as a new user.

Public \(\beta\) tools

Report a bug with a feature
Request a new functionality
404 page design
Send feedback

Attributions

(propose a free ad)

Site Statistics

205 submissions , 163 unreviewed
5,054 questions , 2,207 unanswered
5,345 answers , 22,721 comments
1,470 users with positive rep
818 active unimported users
More ...

  Decidability/algorithm for checking universality of a quantum gate set

+ 8 like - 0 dislike
1863 views

Given a finite set of quantum gates $\mathcal{G} = \{G_1, \dots, G_n\}$, is it decidable (in computation theoretic sense) whether $\mathcal{G}$ is a universal gate set? On one hand, "almost all" gate sets are universal, on the other, non-universal gate sets are still not well understood (in particular, of course, it is not known whether every non-universal gate set is classically simulatable), so I imagine giving an explicit algorithm for checking universality could be nontrivial.

This post has been migrated from (A51.SE)
asked Jan 20, 2012 in Theoretical Physics by Marcin Kotowski (405 points) [ no revision ]
Can you clarify the question? Joe's answer assumes you have a fixed number of qubits and all gates act on those, but for universality, we often assume gates can act on any subset of qubits. E.g., CNOT + all one-qubit gates are not universal if the one-qubit gates can only act on the first qubit, and CNOT is only from qubit 1 to qubit 2. In the latter case, we might want to extrapolate to many qubits to get universality. In that case, I think the anwer may be unknown.

This post has been migrated from (A51.SE)
@DanielGottesman: I agree about the limitations of my answer. Indeed, I believe it is undecidable in the latter case as follows: Take a cellular automata on an infinite lattice of qubits and use it to encode the halting problem (call this update unitary $U_1$). Then take a second lattice with a universal QCA (with update unitary $U_2$). We can define a new unitary $CU_2 = |0\rangle\langle0|_H\otimes I + |1\rangle\langle1|\otimes U_2$, where the subscript $H$ denotes a qubit which is set to $|1\rangle$ iff the first cellular automata halts.

This post has been migrated from (A51.SE)
Thus the gate $CU_2 \times U_1$ is universal if and only if the first Turing machine halts, and is hence undecidable.

This post has been migrated from (A51.SE)

1 Answer

+ 4 like - 0 dislike

For the case of Hamiltonians, rather than gates the answer is trivially yes: you simply enumerate the independent elements of the Lie algebra. Since the Lie algebra is a vector space with the addition of the Lie bracket operator. Since the space is finite, it has a finite basis, and which can easily be checked as to whether it is closed or open under the Lie bracket operation. Simply checking the Lie bracket of all pairs of orthogonal operators can be done in time polynomial in the dimensionality of the space, and a suitable operator basis can be found by the Gram-Schmidt method.

For gates, you don't really have the same option to resort to infinitesimals straight off, and need to construct gates with irrational eigenvalues so that you can arbitrarily well approximate the required infinitesimal generators. I guess that there is a relatively simple way to do this, but it is not immediately obvious to me.

In any case, taking the log of the gates to obtain a set of operators which generate them when exponentiated and checking whether these generated the full Lie algebra would provide a simple necessary but not sufficient criteria for universality.

This post has been migrated from (A51.SE)
answered Jan 20, 2012 by Joe Fitzsimons (3,575 points) [ no revision ]
Most voted comments show all comments
@AlexV: This is implicitly including the higher order terms, whenever the Lie bracket gives you a vector linearly independent of the previous ones. I simply chose to write it as a recursive process considering only pairs each time, since this makes it obvious that the process must terminate in finite time, due to the finite dimension of the space (and hence finite number of recursions). This is akin to saying that we do one round in which we consider higher order terms, but only up to the $d^2$ terms deep (where $d$ is the dimension of the Hilbert space).

This post has been migrated from (A51.SE)
O'K. But you should agree, that such process has exponential complexity with respect to number of qubits (and gates, if the numbers are proportional one). Now if we have some exotic set of gates and need to know if it is universal for any number of qubits, why such a problem should necessary be decidable?

This post has been migrated from (A51.SE)
@AlexV: Yes, absolutely it does have exponential time complexity in the number of qubits (but polynomial in the dimensionality of the space), but the point is that there is an exponential time algorithm for the Hamiltonian version of the problem. For gates, I'm not sure that this is still true, but I suspect it is. I think that you can probably approximate Hamiltonians via Solovay-Kitaev or decide that the group is finite in some bounded time, but this is conjecture. However, taking the log of the gates gives you a necessary but not sufficient criteria for universality.

This post has been migrated from (A51.SE)
@AlexV: I should point out, however, that there is often a polynomial time algorithm. Daniel Burgarth and Alastair Kay have both done a fair amount of work on this problem for restricted types of Hamiltonians.

This post has been migrated from (A51.SE)
I did not see a work of Daniel Burgarth and Alastair Kay on the particular theme, but in works of other authors most often appear the same $spin(n)$ theme, but it is necessary some time, to check the isomorphism. Anyway, in many classical problems we should consider $n \to \infty$ to lost decidability.

This post has been migrated from (A51.SE)
Most recent comments show all comments
Likely we are talking about different things - which vector space you are talking about? You do not know from very beginning the subalgebra generated by your gates - you need to construct that from given Hamiltonians to check if it whole Lie algebra.

This post has been migrated from (A51.SE)
There is yet another problem - I think, using example of non-universal set of gates discussed in my paper (and in many other places) we may construct example, then changing a gate on arbitrary small value may convert set to universal.

This post has been migrated from (A51.SE)

Your answer

Please use answers only to (at least partly) answer questions. To comment, discuss, or ask for clarification, leave a comment instead.
To mask links under text, please type your text, highlight it, and click the "link" button. You can then enter your link URL.
Please consult the FAQ for as to how to format your post.
This is the answer box; if you want to write a comment instead, please use the 'add comment' button.
Live preview (may slow down editor)   Preview
Your name to display (optional):
Privacy: Your email address will only be used for sending these notifications.
Anti-spam verification:
If you are a human please identify the position of the character covered by the symbol $\varnothing$ in the following word:
p$\hbar$ysics$\varnothing$verflow
Then drag the red bullet below over the corresponding character of our banner. When you drop it there, the bullet changes to green (on slow internet connections after a few seconds).
Please complete the anti-spam verification




user contributions licensed under cc by-sa 3.0 with attribution required

Your rights
...