Statistical mechanics of the cluster Ising model

Physical Review A - Atomic, Molecular, and Optical Physics 84:2 (2011)

Authors:

P Smacchia, L Amico, P Facchi, R Fazio, G Florio, S Pascazio, V Vedral

Abstract:

We study a Hamiltonian system describing a three-spin-1/2 clusterlike interaction competing with an Ising-like antiferromagnetic interaction. We compute free energy, spin-correlation functions, and entanglement both in the ground and in thermal states. The model undergoes a quantum phase transition between an Ising phase with a nonvanishing magnetization and a cluster phase characterized by a string order. Any two-spin entanglement is found to vanish in both quantum phases because of a nontrivial correlation pattern. Nevertheless, the residual multipartite entanglement is maximal in the cluster phase and dependent on the magnetization in the Ising phase. We study the block entropy at the critical point and calculate the central charge of the system, showing that the criticality of the system is beyond the Ising universality class. © 2011 American Physical Society.

Unifying typical entanglement and coin tossing: on randomization in probabilistic theories

(2011)

Authors:

Markus P Müller, Oscar CO Dahlsten, Vlatko Vedral

Photon production from the vacuum close to the super-radiant transition: When Casimir meets Kibble-Zurek

(2011)

Authors:

Giovanni Vacanti, Stefano Pugnetti, Nicolas Didier, Mauro Paternostro, G Massimo Palma, Rosario Fazio, Vlatko Vedral

Geometric local invariants and pure three-qubit states

Physical Review A - Atomic, Molecular, and Optical Physics 83:6 (2011)

Authors:

MS Williamson, M Ericsson, M Johansson, E Sjöqvist, A Sudbery, V Vedral, WK Wootters

Abstract:

We explore a geometric approach to generating local SU(2) and SL(2,C) invariants for a collection of qubits inspired by lattice gauge theory. Each local invariant or "gauge" invariant is associated with a distinct closed path (or plaquette) joining some or all of the qubits. In lattice gauge theory, the lattice points are the discrete space-time points, the transformations between the points of the lattice are defined by parallel transporters, and the gauge invariant observable associated with a particular closed path is given by the Wilson loop. In our approach the points of the lattice are qubits, the link transformations between the qubits are defined by the correlations between them, and the gauge invariant observable, the local invariants associated with a particular closed path, are also given by a Wilson looplike construction. The link transformations share many of the properties of parallel transporters, although they are not undone when one retraces one's steps through the lattice. This feature is used to generate many of the invariants. We consider a pure three-qubit state as a test case and find we can generate a complete set of algebraically independent local invariants in this way; however, the framework given here is applicable to generating local unitary invariants for mixed states composed of any number of d-level quantum systems. We give an operational interpretation of these invariants in terms of observables. © 2011 American Physical Society.

The thermodynamic meaning of negative entropy.

Nature 474:7349 (2011) 61-63

Authors:

Lídia del Rio, Johan Aberg, Renato Renner, Oscar Dahlsten, Vlatko Vedral

Abstract:

The heat generated by computations is not only an obstacle to circuit miniaturization but also a fundamental aspect of the relationship between information theory and thermodynamics. In principle, reversible operations may be performed at no energy cost; given that irreversible computations can always be decomposed into reversible operations followed by the erasure of data, the problem of calculating their energy cost is reduced to the study of erasure. Landauer's principle states that the erasure of data stored in a system has an inherent work cost and therefore dissipates heat. However, this consideration assumes that the information about the system to be erased is classical, and does not extend to the general case where an observer may have quantum information about the system to be erased, for instance by means of a quantum memory entangled with the system. Here we show that the standard formulation and implications of Landauer's principle are no longer valid in the presence of quantum information. Our main result is that the work cost of erasure is determined by the entropy of the system, conditioned on the quantum information an observer has about it. In other words, the more an observer knows about the system, the less it costs to erase it. This result gives a direct thermodynamic significance to conditional entropies, originally introduced in information theory. Furthermore, it provides new bounds on the heat generation of computations: because conditional entropies can become negative in the quantum case, an observer who is strongly correlated with a system may gain work while erasing it, thereby cooling the environment.