Physics & Astronomy Condensed Matter Seminar
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Abstract: I will discuss the problem of strange metals, where the traditional notion of Fermi liquid quasiparticles ceases to apply. I will view the problem through the lens of a model of electrons with Hubbard-U Coulomb repulsion and a disordered Yukawa coupling to a two-dimensional bosonic bath, which can be solved in an extended dynamical mean field theory scheme. The model exhibits a quantum critical point, at which the repulsive component of the electron interactions strongly enhances the effects of the quantum critical bosonic fluctuations on the electrons, leading to a breakdown of Fermi liquid physics and the formation of a strange metal with `Planckian' quasiparticle decay rates at low temperatures, although with no holographic dual. Furthermore, the eventual Mott transition that occurs as the repulsion is increased seemingly bounds the maximum decay rate in the strange metal. I will also discuss some applications and collaborations based on this work to the iron-based superconductors and moire materials. Time permitting, I will conclude with future directions to include nonlocal effects.
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Title: Hybrid quantum phononics with superconducting qubits*
Abstract: Superconducting qubits, and the experimental architecture of circuit quantum
electrodynamics (cQED), have emerged as not only a promising platform for quantum
computation but also for investigating fundamental and applied aspects of
synthetic/hybrid quantum systems composed of qubits coupled to other quantum systems
or degrees of freedom. In particular, the ability to leverage the properties of
superconducting qubits to investigate and manipulate phononic degrees of freedom opens
the door to exploring new regimes of circuit quantum optics using high-frequency sound.
Due to the intrinsically strong nonlinearity provided by the qubit, these types of hybrid
“quantum acoustic” systems have the potential to access a broad class of quantum states
of motion beyond what is achievable with effectively linear optomechanical or
electromechanical interactions.
In this talk I will describe some of our recent experimental results investigating the
fundamental physics of hybrid systems based on superconducting qubits coupled to
piezoelectric surface and bulk acoustic wave devices and how these systems can be used
to develop next-generation technologies for quantum sensing, computation, and
communication. As I will describe, these engineered systems, in which quantum
information stored in the qubit can be controllably coupled to the microscopic surface
and bulk phonon modes of a piezoelectric crystal, are an ideal platform for investigating
the exotic behavior of synthetic open quantum systems and phononic interference in the
quantum regime. Additionally, I will describe how these devices pave the way to exciting
new technologies ranging from quantum-limited surface sensing to phonon-based
bosonic quantum memories.
*This work was supported by the National Science Foundation via Grant No. ECCS-2142846 (CAREER)
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Speaker: Leonid Levitov (M.I.T)
Title: Spin chirality, quasiparticle dynamics and signatures of exotic superconductivity
Speaker: Cyprian Lewandowski, Florida State University
Speaker: Herbert Fertig. Indiana University
Title: A Tale of Two Bilayers
Abstract: Modern materials physics has made available true two-dimensional electron systems, in the form of atomic networks bonded only across a single plane. These van der Waals systems may be formed from a variety of materials, with different electronic properties, which may be combined into bilayer heterostructures with properties not found in either layer individually. In this talk we will describe quantum coherent states of two such systems, in which nesting plays an important role in determining the ground state phase diagram. The first of these is a phosphorene – graphene bilayer, for which one finds Fermi surfaces with strong nesting overlaps, leading to spin-density wave ground states for sufficiently strong interactions. The second involves an idealized bilayer in which each layer supports a particle-hole symmetric band structure, possibly with non-trivial topology. For half-filling, we find that nesting of the Fermi surfaces on opposite layers leads to different exciton condensate states, separated by a first order transition line which ends in an unusual zero temperature critical endpoint. We demonstrate that this endpoint is a signature of Lifshitz transitions hosted by the individual layers in the absence of interactions. In this way their Fermi surface topologies leave an imprint in the interacting phase diagram, in regions where the states themselves are fully gapped and lack Fermi surfaces.