Postdoc opportunity

August 1, 2011

I’d like to take this opportunity to announce a new postdoc opportunity. This three-year position is part of a challenging interdisciplinary european project aimed at applying ideas and techniques developed within quantum information theory, such as quantum entanglement, to the study of strongly interacting quantum fields. I’ve mentioned some of these ideas in previous posts, and you can get a feel for what we’ll be tackling by taking a look at these recent papers. Although the project is based on a quantum-information approach, I would particularly welcome applications not only from quantum information and condensed matter physics, but also from those with a background in high-energy physics, e.g., quantum field theory, string theory, and lattice gauge theory. If you are either a quantum information or a high-energy physicist looking for a new challenge, then I’d be glad to hear from you!

The quantum information group comprises three professors: Reinhard Werner, Andreas Ruschhaupt, and myself, along with some 20 postdocs, PhD students, Masters and BSc students, and is situated within the ITP at the Leibniz Universität Hannover. The group is closely associated with the QUEST centre of excellence, and benefits from strong collaborative links with researchers from, variously, mathematics, gravitational and high-energy research through to experimental quantum optics.

I’m personally very excited about this project, and I look forward to receiving your applications and welcoming new members to this challenging collaborative endeavour!

There will be several further opportunities over the coming months and years, including both postdoc and PhD positions, as well as BSc and Masters projects, so please check back every so often. Do feel free to contact me for further details.

The job advertisement can be found here, and the closing date is 02.09.2011.


The next big thing?

July 10, 2011

Quantum information theory has evolved in fascinating ways over the past two decades or so and I’ve been privileged to directly witness its development for ten of these years. In this post, I thought I’d have a go at predicting where it will go, and what the “next big thing” for quantum information theory will be.

Around the year 2000 quantum information theory seemed to be primarily focussed on two broad themes: building a quantum computer and developing quantum algorithms for it, and building a resource theory for quantum information via, e.g., quantum entanglement theory and quantum Shannon theory. To a large extent both of these themes continue strongly today. Although, I’d suggest that quantum Shannon theory has fared much better than the theory of quantum entanglement, in particular, that of entanglement measures, which seemed really important a decade ago but not so much now.

One thing that would have been harder to predict was the influence of quantum information theory on other areas of physics. For example, QI has now had some considerable impact in condensed matter physics, particularly with regard to the development of new classical simulation algorithms for complex quantum systems. From my considerably biased perspective I think that this second-order effect has been rather important. Also, there has been excitement about the role and influence of QI on biological physics.

So now to the question: what next for quantum information? I based the following list on topics that I personally find very interesting, and also on observations I’ve made about external pressures coming from funding agencies and from the job market.

1. Quantum computers

I firmly believe a quantum computer will be built, although I refuse to say how long this will take. One thing that I think may happen is the emphasis on fault tolerance thresholds in choosing a quantum computer architecture will diminish slightly as experimentalists engineer systems capable of supporting quantum coherence on longer timescales. I’m sure that cluster states will be exploited in some way in the successful quantum computer architectures. I also feel sure that as we get access to such systems this will spark our creativity in designing nontrivial things to do, i.e., in developing quantum algorithms using dissipative quantum processes.

2. Quantum algorithms

Thus I feel convinced that quantum algorithms development will continue, albeit slowly. One area which hasn’t received much attention — probably because it isn’t as glamourous as an exponential speedup — but which really should, is the development of quantum algorithms which give polynomial speedups for problems in P. These kind of speedups could turn out to be extremely important: if the best classical algorithm for a problem of major practical importance uses, say, {O(n^3)} operations, and you found a quantum algorithm using {O(n\log(n))} operations this would have major practical implications. I do hope that such speedups will become an area of more intense research and I feel relatively confident this area could take off. Unfortunately I don’t know enough about classical algorithms to give a firm prediction for which kinds of problems will be amenable to such quantum speedups (sorry!).

As mentioned above, another class of quantum algorithms which has been so far relatively unexplored, is that of dissipative quantum algorithms. (There are some exceptions here, see, e.g., and this, this, and, somewhat immodestly, this.) Such algorithms are extremely important because they give intermediate experimental implementations something to run!

3. Complex quantum systems

Quantum information will continue to play a role in the study of complex quantum systems. This is an easy prediction: QI trained people are generally quite good at thinking about quantum coherence, which plays a major role in the physics of strongly interacting quantum systems. I feel relatively confident in predicting that the physics of 2D and, to some extent, 3D lattice systems, will see major QI-inspired developments.

Another area which I am very enthusiastic about is that of quantum systems with continuous degrees of freedom, particularly, quantum fields. Lattice systems are, after all, an approximation to these systems, and it is clear that existing QI-inspired techniques will have some influence here (indeed, this is just beginning with the extension of MPS and MERA to the continuous setting). Additionally, if a good enough interplay can be developed then this would allow quantum field theorists to be able contribute to quantum information-type problems. Also, holographic correspondences such as the AdS/CFT correspondence have QI aspects, so we might see QI theorists and string theorists working together more strongly here.

4. Classical physics

My final prediction concerns the influence of QI on classical physics. The thing is, QI trained people are not only good at thinking about quantum coherence, but also about correlations in general (see, e.g., the continuing developments in the study of Bell’s inequalities, cryptography based on no-signalling, etc.). Correlations are always hard to think about, but the thing we’ve learnt in studying QI in the context of condensed matter is that if you have a way to think about correlations in a better way then this can lead to new simulation algorithms. Here I have in mind, for example, the study of fluid dynamics, as applied to the climate (see this for a longer discussion), and other problems of classical many body physics such as traffic flow via this, community detection, and image recognition. The nice thing about these areas is that they are much more directly connected with our everyday life. Any contribution here would have a much more direct impact on important problems facing humanity.

What do you think?


The variational principle in quantum mechanics, lecture 12

July 7, 2011

1. Lecture 12: the time-dependent variational principle for dissipative dynamics

The time-dependent variational principle of Dirac is a powerful method to simulate the real and imaginary time dynamics of strongly correlated quantum systems. The original formulation has, as far as I can tell, only been formulated in the case of pure states. The generalisation to quantum systems undergoing dissipative dynamics is nontrivial and appears not to have been attempted. Here we describe a natural generalisation.

The pdf version can be found here.

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The variational principle in quantum mechanics, lecture 11

July 1, 2011

1. Lecture 11: the time-dependent variational principle and mean-field theory

In this and the following lectures we are going to apply the time-dependent variation principle (TDVP) to the variational classes we have met previously, namely, product states for quantum spin systems, mean-field states for bosons and fermions, and matrix product states.

The pdf version of these notes can be found here. Read the rest of this entry »


The variational principle in quantum mechanics, lectures 9 and 10

June 23, 2011

In lecture 9 we continued reading the papers on matrix product states that we began in lectures 7 and 8.

1. Lecture 10: the time-dependent variational principle

In this lecture we will discuss the time-dependent variation principle (TDVP), which is a powerful method to simulate the nonequilibrium dynamics of a general quantum system while remaining within a given variational class. The TDVP is due, as far as I’m aware, to Dirac. Additionally, describing the TDVP isn’t especially difficult, so it is rather surprising that this elegant method it hasn’t made into standard textbooks. The general framework of the time-dependent variational principle can be found in [P. Kramer and M. Saraceno, Geometry of the Time-Dependent Variational Principle in Quantum Mechanics (Springer-Verlag, Berlin) (1981)].

These notes can be found in pdf format here.

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Antrittsvorlesung

June 9, 2011

On Tuesday June 7th I gave my Antrittsvorlesung (= inaugural lecture) entitled “Größenverhältnisse und Information” (= “Scale and information”). You can find the slides here. The german text of the lecture can be found here and the english text here.


The variational principle in quantum mechanics, lecture 7 and 8

June 2, 2011

In lectures 7 and 8 we will discuss the papers:

“Efficient classical simulation of slightly entangled quantum computations”,

found here

and

“Efficient simulation of one-dimensional quantum many-body systems”

found here

by Guifre Vidal.


The variational principle in quantum mechanics, lecture 6

May 18, 2011

1. Lecture 6: density functional theory

In the previous two lectures we discussed several examples of mean-field theory where the variational class is the class of gaussian states or single-particle product states. It turns out that mean-field theory is extremely useful in practice and can give powerful insights into the physics of many strongly interacting systems. This is because it leads to equations which are essentially tractable analytically. Additionally, the solutions often have a direct physical interpretation. Thirdly, the results obtained can often be very good indeed and often match experimentally obtained values to a high precision. Indeed, I’m sure that mean-field theory will continue to be a very useful tool for many years to come, and it should certainly be the first port of call when trying to understand a new system.

In this lecture we turn our attention to another method known as density functional theory (DFT). This can be viewed as, in part, an application of the variational method, although it is not a pure application in the sense of our previous examples.

The pdf version of the lecture notes can be found here. Read the rest of this entry »


The variational principle in quantum mechanics, lecture 5

May 11, 2011

1. Lecture 5: Mean-field theory and the Gross-Pitaevskii equation

In the previous lecture we saw two applications of the variational principle to the class of product states and fermionic gaussian states, respectively. In both cases we obtained an effective equation for the ground-state properties involving only a single effective particle (a single spin in the first case and a single majorana fermion in the second case).

In this lecture we continue our study of mean-field theory in the bosonic setting, in particular to the description of Bose-Einstein condensates. Here we find a similar result: we’ll obtain a nonlinear effective equation for the condensate in terms of a single effective particle degree of freedom. Before we do this we need to review some of the formalism for the description of quantum fields and coherent states.

The pdf version of the notes can be found here. Read the rest of this entry »


The variational principle in quantum mechanics, lecture 4

May 5, 2011

1. Lecture 4: Mean-field theory and Hartree-Fock theory

In this lecture we’ll describe a general strategy to approximately solving the many body problem introduced in the previous lecture. This approach falls broadly under the rubric of mean-field theory and is better known, in various contexts, as Hartree-Fock theory, the self-consistent field method, and the Gutzwiller ansatz.

The idea behind mean-field theory is simple: we take as a variational class one that neglects all quantum correlations between particles and apply the variational method. In the application of the variational method one then sees that the influence of all the other particles on a given one are treated in an averaged way. Our treatment of the Helium atom in lecture 2 could be seen as an application of mean-field theory in an embryonic form.

To explain mean-field theory in this lecture we’ll consider a sequence of simplified examples.

These lecture notes can be found in pdf form here.

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