No abstract

It is shown that effective quantum-state and entanglement transfer can be obtained by inducing a coherent dynamics in quantum wires with homogeneous intrawire interactions. This goal is accomplished by tuning the coupling between the wire endpoints and the two qubits there attached, to an optimal value. A general procedure to determine such value is devised, and scaling laws between the optimal coupling and the length of the wire are found. The procedure is implemented in the case of a wire consisting of a spin-1 2 XY chain: results for the time dependence of the quantities which characterize quantum-state and entanglement transfer are found of extremely good quality and almost independent of the wire length. The present approach does not require ad hoc engineering of the intrawire interactions nor a specific initial pulse shaping, and can be applied to a vast class of quantum channels.One of the most commonly requested conditions in quantum communication and computation protocols is that two distant parties, typically Alice and Bob, share a couple of entangled qubits. When the physical objects encoding the qubits can travel, as in the case of optical photons, the above goal can be accomplished by creating the entangled couple in a limited region of space and then letting the qubits fly where necessary. On the other hand, when qubits are realized via intrinsically localized physical objects, as in the case of S = 1 2 spins or atomic systems, a different strategy must be adopted (see for instance Ref. 1 and references therein). One such strategy is the following: first, two neighboring qubits (A and A ′ ) are prepared in an entangled state, by means of a shortrange interaction; then, the mixed state of one of the two qubits (say A) is transferred to a third distant qubit via a quantum channel. If state-transfer is perfect the procedure results in a pair of distant entangled qubits A ′ and B, as requested.Aim of this paper is to set a general framework where such strategy can be successful. In particular, (i) we define a procedure for controlling such dynamics, and hence the quality of the transmission process, by specific operational settings; (ii) we show that the quality of the quantum-state and entanglement transfer is not substantially affected by the length of the wire; (iii) we apply the procedure to the spin-1 2 XY chain and show that high-quality quantum-state and entanglement transfer are obtained.Let us first recall that for the strategy depicted above to make sense, one has to equip oneself with a quantum channel capable of transferring mixed states. How to obtain such a channel is the problem to which many authors have proposed different solutions [1][2][3][4][5][6][7], some based on the idea of engineering the channel itself, by the specific design of its internal interactions, others on that of intervening on the initialization process, by preparing the wire in a configuration found to serve the purpose. In both cases, a severe external action on the physical system is required.Here a different poin...

We study the finite-temperature behaviour of two-dimensional S = 1/2 Heisenberg antiferromagnets with very weak easy-axis and easy-plane exchange anisotropies. By means of quantum Monte Carlo simulations, based on the continuous-time loop and worm algorithm, we obtain a rich set of data that allows us to draw conclusions about both the existence and the type of finite-temperature transition expected in the considered models. We observe that the essential features of the Ising universality class, as well as those of the Berezinskii-Kosterlitz-Thouless (BKT) one, are preserved even for anisotropies as small as 10 −3 times the exchange integral; such outcome, being referred to the most quantum case S = 1/2, rules out the possibility for quantum fluctuations to destroy the long or quasi-long range order, whose onset is responsible for the Ising or BKT transition, no matter how small the anisotropy. Besides this general issue, we use our results to extract, out of the isotropic component, the features which are peculiar to weakly anisotropic models, with particular attention for the temperature region immediately above the transition. By this analysis we aim to give a handy tool for understanding the experimental data relative to those real compounds whose anisotropies are too weak for a qualitative description to accomplish the goal of singling out the genuinely two-dimensional critical behaviour.