Condensed Matter Seminar
Our condensed matter seminars are held on Tuesdays at 3:30pm in Chemistry-Physics Building, Room 179, unless otherwise noted below. A number of the department colloquium may also be of interest.
Condensed Matter Seminar: Pontus Laurell
Spin chirality, quasiparticle dynamics and signatures of exotic superconductivity
Speaker: Leonid Levitov (M.I.T)
Title: Spin chirality, quasiparticle dynamics and signatures of exotic superconductivity
Condensed Matter Seminar
Speaker: Cyprian Lewandowski, Florida State University
A Tale of Two Bilayers
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.
Condensed Matter Seminar: Emergent Quantum Phenomena in Crystalline Graphene
Speaker: Long Ju, MIT
Title: Emergent Quantum Phenomena in Crystalline Graphene
Abstract: Condensed matter physics has witnessed many emergent quantum phenomena driven by electron correlation and topology. Such phenomena have been mostly observed in conventional crystalline materials where flat electronic bands are available. In recent years, moiré superlattices built upon two-dimensional (2D) materials emerged as a new platform to engineer and study electron correlation and topology. In this talk, I will introduce a family of synthetic quantum materials, based on crystalline multilayer graphene, as a new platform to engineer and study emergent phenomena driven by many-body interactions. This system hosts flat-bands in highly ordered conventional crystalline materials and dresses them with proximity effects enabled by rich structures in 2D van der Waals heterostructures. As a result, a rich spectrum of emergent phenomena including correlated insulators, spin/valley-polarized metals, integer and fractional quantum anomalous Hall effects, as well as chiral superconductivities have been observed in our experiments. I will also discuss the implications of these observations for topological quantum computation.
Imaging composite fermions with scanning tunneling microscopy
Speaker:Dr. Songyang Pu, University of Tennessee, Knoxville,
Title: Imaging composite fermions with scanning tunneling microscopy
Abstract: A composite fermion (CF) is a topological quasiparticle that emerges from a nonperturbative attachment of vortices to electrons in strongly correlated two-dimensional materials. Similar to noninteracting fermions that form Landau levels in a magnetic field, CFs can fill analogous “Lambda” levels, giving rise to the fractional quantum Hall (FQH) effect of electrons. Here, we show that Lambda levels can be directly visualized through the characteristic peak structure in the signal obtained via spectroscopy with scanning tunneling microscopy (STM) on a FQH state. Complementary to transport, which probes the low-energy properties of CFs, we show that high-energy features in STM spectra can be interpreted in terms of Lambda levels. We numerically demonstrate that STM spectra can be accurately modeled using Jain's CF theory. Our results show that STM provides a powerful tool for revealing the anatomy of FQH states and identifying physics beyond the noninteracting CF paradigm.
Chiral Wigner Crystal Phases Induced by Berry Curvature
Brian Skinner
The Ohio State University
Department of Physics
Title: Chiral Wigner Crystal Phases Induced by Berry Curvature
Abstract: In 1934 Eugene Wigner first predicted that a gas of electrons is susceptible to a freezing transition when its density is low enough due to the long-range Coulomb interaction between electrons. This Wigner crystal (WC) state has only very recently been realized and visualized in two dimensional materials without applied magnetic field. Here I discuss new forms of the Wigner crystal state that can arise in materials with Berry curvature. I focus specifically on bilayer graphene, and discuss the phase diagram and the different ordered states of the Wigner crystal.
TBA
TBA
Ising-like models on Euclidean black holes
Abstract: The thermodynamic interpretation of Schwarzschild black holes has a rich history spanning five decades. In 1973 Bardeen et al. derived the laws of black hole mechanics which suggested a correspondence between (i) temperature and black hole’s mass, specifically T=(8πM)-1 and (ii) entropy and black hole area: S=A/4. In 1975 Hawking found that a Schwarzschild black hole radiates as if it were a blackbody with temperature T=(8πM)-1. This meant that the temperature-mass relationship discovered earlier was more than a correspondence. In 1977 Gibbons and Hawking proposed the action of Euclidean Schwarzschild (which also has T=(8πM)-1) as a means to understand black hole thermodynamics. They recovered S=A/4.
In this talk we will test if Euclidean Schwarzschild behaves like a heat bath for quantum matter that propagates on it. For simplicity we will use matter with restricted excitations – Ising spins. We will discover that increasing M causes the spins to undergo a second order phase transition from disorder to order and that the phase transition occurs at sub-Planckian M.