February 27

Speaker: Karen Michaeli, MIT

Title: "Probing interactions with thermal transport"

Abstract:

Thermal and thermoelectric conductivities are ideal probes of interaction effects in correlated electron systems.  This is because, in contrast to an electric current,  a heat current can be transmitted also by neutral quasiparticles. For instance, energy can be carried by excitations that mediate interactions between other quasiparticles. In my talk I will present two examples of the dramatic effect of interactions on thermal and thermoelectric transport phenomena.  The first is the Nernst effect in the vicinity of the superconducting phase transition. I will demonstrate that the giant Nernst signal, experimentally observed in amorphous films far above Tc, is caused by the fluctuations of the superconducting order parameter. Moreover, I will discuss the anomalous behavior of the Nernst effect near the magnetic-field-induced quantum critical phase transition. The second example is thermal conductivity in spin liquids. Spin liquids can form in the vicinity of the Mott metal-insulator transition when the charge is gapped while the spin degrees of freedom strongly fluctuate. These low energy excitations, dubbed spinons, can conduct heat. The spinons also exhibit a magnetic interaction that leads to non-Fermi liquid behavior. I will show that even in the absence of disorder this strong interaction provides an efficient relaxation mechanism for heat and spin currents, keeping them finite at the lowest temperatures

May 1

Speaker: Julio Barreiro, Max Planck Institute of Quantum Optics & University of Munich, Germany

Title:  “Harnessing additional degrees of freedom and the environment to experimentally enable quantum applications and simulations”

Abstract

Quantum simulations and applications of quantum information usually have experimentally demanding requirements. I will show how these were circumvented in several experiments with photons and ions by using resources additional to the systems of interest. In particular, we take advantage of other degrees of freedom and the environment, either intrinsic or engineered, through dissipation and decoherence. As an example, although full quantum dense coding is impossible with linear optics, we realized it by using entanglement in an additional degree of freedom of a pair of photons. Another challenging task is quantum error correction. By dissipatively providing fresh ancillas to the algorithm, a qubit was repetitively corrected for in three iterations in a system of trapped ions. In the context of quantum simulations, an auxiliary qubit was engineered as a controlled environment that allowed us to demonstrate a toolbox for the simulation of open systems. Finally, I will discuss how similar approaches can lead to an arbitrary many-body simulator in a system of ultracold atoms in optical lattices.