Now on ScienceBlogs: 'The Secret World of Naked Snakes': a ZSL event

Seed Media Group

Collective Imagination

Search

rss.jpg   Subscribe to RSS feed

Profile

davidog.pngDave Bacon is a theoretical ski bum who is also a pseudo professor. His research is on quantum computing, his scientific passions extend to everything in physics, mathematics, computer science and beyond, and his personal pleasures include making wine, playing poker, skiing, camping, and daydreaming (although not all of those at the same time.) Nothing he says on this blog should be construed as having anything to do with his employer or his dog.


Recent Comments

Recent Posts

Other Information

The use of Occam's razor on this website is strickly prohibited.

Cows are well approximated by a sphere.
rss.jpg   Subscribe to RSS feed

« Drunkard's Tennis and the Advice of Winners | Main | Tiger Versus the Theoreticians »

Rhythm is a Quantum Concatenated Code

Category: PhysicsQuantum ComputingSelf: Meet Center. Center: Meet Self.
Posted on: June 16, 2008 10:41 AM, by Dave Bacon

Share:

I do believe this is the first time I've performed the paper dance on the scienceblogs incarnation of this blog. Yep, it's that time again: it's the paper dance!

"A far away light in the futuristic place we might be; It's a tiny world just big enough to support the kingdom of one knowledgeable; I feel a wave of loneliness and head back down I'm going too fast (I'm going too fast)"

arXiv:0806.2160
The Stability of Quantum Concatenated Code Hamiltonians
Authors: D. Bacon

Abstract: Protecting quantum information from the detrimental effects of decoherence and lack of precise quantum control is a central challenge that must be overcome if a large robust quantum computer is to be constructed. The traditional approach to achieving this is via active quantum error correction using fault-tolerant techniques. An alternative to this approach is to engineer strongly interacting many-body quantum systems that enact the quantum error correction via the natural dynamics of these systems. Here we present a method for achieving this based on the concept of concatenated quantum error correcting codes. We define a class of Hamiltonians whose ground states are concatenated quantum codes and whose energy landscape naturally causes quantum error correction. We analyze these Hamiltonians for robustness and suggest methods for implementing these highly unnatural Hamiltonians.

Share this: Stumbleupon Reddit Email + More

TrackBacks

TrackBack URL for this entry: http://scienceblogs.com/mt/pings/74180

Comments

1

Dave, this is a good idea. Although I think you can do similar things with "natural" Hamiltonians also. In fact I think most Hamiltonians provide what can be thought of as passive quantum error correction. Your approach might help illuminate why / under what conditions this is true.

Posted by: Geordie | June 16, 2008 11:12 AM

2

Yay!

Aweful post title btw... I now have a truly aweful song stuck in my head.

Posted by: mick | June 16, 2008 11:32 AM

3

I am confused by the usage of 'we' in single-author papers. I know that 'I' is considered arrogant and turns a lot of people off, but 'we' is nonsensical.

Posted by: Jon | June 16, 2008 1:27 PM

4

I call it the "scientific we."

David Mermin once fought for using "I" in Physical Review Letters. He won, and then wrote the paper using "we."

Posted by: Dave Bacon | June 16, 2008 2:27 PM

5

I second Jon's comment (at least in principle). That is, while I'm not confused by it, I don't like it. I use "we" whenever possible to indicate "the reader and I", e.g. in "Now, by taking the square root of this negative number, we see that Chewbacca is a wookie." In other circumstances, though, I feel that "I" is just plain the right way to go -- and I propose a guerrilla group dedicated to the educated use of the first-person singular in papers...

Posted by: Robin Blume-Kohout | June 16, 2008 2:38 PM

6

I'm going to point some of my buddy's at this paper as it seems to rhyme with things they are working on.

The whole construction smells of "mutually unbiased bases" or MUB theory, in that it considers tensor products of other than all spin-z states. And I think you can generalize from the Pauli algebra to other Clifford algebras. The ideals and primitive idempotents of a Clifford algebra are defined by maximal sets of commuting non trivial square roots of unity (other than -I). For example, with the Dirac algebra, given two Dirac bilinears A and B that commute and square to +1, a complete set of primitive idempotents is (1 +- A)(1 +- B)/4.

Also, "canonical choose" needs a change.

Posted by: Carl Brannen | June 16, 2008 7:41 PM

7

We find that it is a brilliant paper.

I am in a mixed state of humble and proud to have assisted in a tiny way with the error correction via the natural blog-dynamics of these systems.

I guarantee that my 4 arXiv papers have more insidious errors.

When last week's Caltech Commencement address by Robert Krulwich shows up on the Caltech web site, it would be well worth your mentioning on Quantum Pontiff. It was one of the best talks I've ever seen, on narrative in science, managing to quote Schrodinger, Heisenberg, Galileo, and episodes of "Friends."

Posted by: Jonathan Vos Post | June 17, 2008 1:06 PM

8

Although I think you can do similar things with "natural" Hamiltonians also. In fact I think most Hamiltonians provide what can be thought of as passive quantum error correction.

Well there are a bunch of questions here. First I think that most Hamiltonians don't provide a degeneracy corresponding to a quantum error correcting code subspace. So I think it might be possible that generic ground states have quantum error correcting properties, they aren't necessarily good for protecting encoded quantum information. But the real question isn't whether the ground state is a good code state: the real question is what happens when you bump it. I suspect that systems which have quantum error correcting properties and which are also robust under perturbation aren't quite as ubiquitous.

Posted by: Dave Bacon | June 17, 2008 1:39 PM

9

What type of perturbation are you thinking of? Like unknown low frequency type perturbations on your control parameters during annealing?

Posted by: Geordie | June 17, 2008 1:56 PM

Post a Comment

(Email is required for authentication purposes only. On some blogs, comments are moderated for spam, so your comment may not appear immediately.)





ScienceBlogs

Search ScienceBlogs:

Go to:

Advertisement
Enter to win a free copy of The Monty Hall Problem
Visit the Collective Imagination blog
Advertisement
Collective Imagination

© 2006-2009 Seed Media Group LLC. ScienceBlogs is a registered trademark of Seed Media Group. All rights reserved.

Sites by Seed Media Group: Seed Media Group | ScienceBlogs | SEEDMAGAZINE.COM