4 Corners Southwest Ontario Condensed Matter Physics Symposium 2014

13 talks

May 01, 2014 - May 01, 2014

C14022

Collection Type Conference/School

Description 4 Corners Southwest Ontario Condensed Matter Physics Symposium 2014

Displaying 1 - 12 of 13

Welcome Address

Michel Gingras University of Waterloo

May 01, 2014
PIRSA:14050012
Localization-Protected Quantum Order

David Huse Princeton University

May 01, 2014
PIRSA:14050013
Entanglement, Ergodicity, and Many-Body Localization

Dmitry Abanin

May 01, 2014
PIRSA:14050020
Exotic Magnetism on the FCC Lattice of 5dn Double Perovskites

Edwin Kermarrec McMaster University

May 01, 2014
PIRSA:14050026
Renormalization Group Analysis of a Non-Fermi Liquid System

Ipsita Mandal University of Stavanger (UiS)

May 01, 2014
PIRSA:14050014
Non-Abelian String and Particle Braiding in 3+1D Topological Order

Juven Wang Harvard University

May 01, 2014
PIRSA:14050015
Experimental Sightings of the Quantum Spin Liquid

Young Lee Massachusetts Institute of Technology (MIT)

May 01, 2014
PIRSA:14050016
Fractionalized Charge Excitations in a Spin Liquid on Partially-Filled

Gang Chen Fudan University

May 01, 2014
PIRSA:14050024
Generic Spin Model for Honeycomb Iridates Beyond the Kitaev Limit

Jeffrey Rau University of Toronto

May 01, 2014
PIRSA:14050025
Using β-NMR to Solve Hard Problems in Soft Condensed Matter

James Forrest

May 01, 2014
PIRSA:14050023
Strain Induces Helical Flat Band & Interface Superconductivity in Topological Crystalline Insulators

Evelyn Tang Rice University

May 01, 2014
PIRSA:14050017
Measurements of Noice in Condensed Matter Systems Using Superconducting Qubits and Resonators

Adrian Lupascu Institute for Quantum Computing (IQC)

May 01, 2014
PIRSA:14050018

Welcome Address

Michel Gingras University of Waterloo

May 01, 2014
PIRSA:14050012
Localization-Protected Quantum Order

David Huse Princeton University

May 01, 2014
PIRSA:14050013

Systems that are many-body Anderson localized can exhibit symmetry-breaking long-range order or topological order in regimes where such order would be destroyed at equilibrium by thermal fluctuations. The ordering is dynamical: an ordered initial state stays ordered, being "protected" by the localization of all fluctuations. The simplest examples are quantum Ising models with static randomness. For the random quantum Ising chain this feature has been "known" but apparently not appreciated for close to half a century.

Ref.: Huse, et al., Phys. Rev. B 88, 014206 (2013).
Entanglement, Ergodicity, and Many-Body Localization

Dmitry Abanin

May 01, 2014
PIRSA:14050020

We are used to describing systems of many particles by statistical mechanics. However, the basic postulate of statistical mechanics – ergodicity – breaks down in so-called many-body localized systems, where disorder prevents particle transport and thermalization. In this talk, I will present a theory of the many-body localized (MBL) phase, based on new insights from quantum entanglement. I will argue that, in contrast to ergodic systems, MBL eigenstates are not highly entangled. I will use this fact to show that MBL phase is characterized by an infinite number of emergent local conservation laws, in terms of which the Hamiltonian acquires a universal form. Turning to the experimental implications, I will describe the response of MBL systems to quenches: surprisingly, entanglement shows logarithmic in time growth, reminiscent of glasses, while local observables exhibit power-law approach to “equilibrium” values. I will support the presented theory with results of numerical experiments. I will close by discussing other directions in exploring ergodicity and its breaking in quantum many-body systems.
Exotic Magnetism on the FCC Lattice of 5dn Double Perovskites

Edwin Kermarrec McMaster University

May 01, 2014
PIRSA:14050026

In the search for new exotic quantum states, the impact of strong spin-orbit interaction has been recently underlined with the discovery of the Jeff = ½ spin orbital Mott state in the 5d5 layered perovskites iridates [1]. The double perovskite structure, where the magnetic ions form a face-centered-cubic (fcc) sublattice, can accommodate a large variety of 5d transition metal elements, and therefore offers an ideal playground for systematic studies of the exotic magnetic and non-magnetic ground states stabilized by strong spin-orbit coupling [2]. Here, we report time-of-flight neutron scattering measurements on the antiferromagnetic, frustrated, cubic double perovskite system Ba2YOsO6. Its non-distorted fcc lattice is decorated with magnetic Os5+ (5d3) ions which undergo a magnetic transition to a long range ordered antiferromagnetic state below TN = 70 K, as revealed by magnetic Bragg peaks occuring at the [100] and [110] positions. Our inelastic data reveals a large spin gap to the spin-wave excitations Δ = 19(2) meV, unexpected for an orbitally quenched, d3 electronic configuration. We compare this result to the recent observation of a Δ=5 meV spin gap in the related cubic double perovskite Ba2YRuO6 (Ru5+, 4d3) [3], and conclude to a stronger spin-orbit coupling present in the heavier, 5d, osmate system.

[1] B. J. Kim et al., Science 323, 1329 (2009).
[2] G. Chen, R. Pereira and L. Balents, Phys. Rev. B 82, 174440 (2010);
G. Chen and L. Balents, Phys. Rev. B 84, 094420 (2011).
[3] J. P. Carlo et al., Phys. Rev. B 88, 024418 (2013).
Renormalization Group Analysis of a Non-Fermi Liquid System

Ipsita Mandal University of Stavanger (UiS)

May 01, 2014
PIRSA:14050014

We devise a renormalization group analysis for quantum field theories with Fermi surface to study scaling behaviour of non- Fermi liquid states in a controlled approximation. The non-Fermi liquid fixed points are identified from a Fermi surface in (m+1) spatial dimensions, while the co-dimension of Fermi surface is also extended to a generic value. We also study superconducting instability in such systems as a function of dimension and co-dimension of the Fermi surface. The key point in this whole analysis is that unlike in relativistic QFT, the Fermi momentum kF enters as a dimensionful parameter, thus modifying the naive scaling arguments. The effective coupling constant is found to be a combination of the original coupling constant and kF.
Non-Abelian String and Particle Braiding in 3+1D Topological Order

Juven Wang Harvard University

May 01, 2014
PIRSA:14050015

String and particle excitations are examined in a class of 3+1D topological order described by a discrete gauge theory with a gauge group G and a 4-cocycle twist ω4∈H4(G,R/Z) of G's cohomology group. We demonstrate the topological spin and the spin-statistics relation for the closed strings, and their multi-string braiding. The 3+1D twisted gauge theory can be characterized by a representation of SL(3,Z) modular transformation, which we find its generators Sxyz and Txy in terms of the gauge group G and the 4-cocycle ω4. As we compactify one of the 3D's direction z into a compact circle inserted with a gauge flux b, we can use the generators of SL(2,Z) subgroup of SL(3,Z), Sxy and Txy, to study the dimension reduction of the 3D topological order C3D to a direct sum of degenerate states of 2D topological orders C2Db in different fluxb sectors: C3D=⊕bC2Db. The 2D topological orders C2Db are described by 2D gauge theories of the group G twisted by the 3-cocycles ω3(b)dimensionally reduced from the 4-cocycle ω4. We show that the SL(2,Z) generators, Sxy and Txy, fully encodes a particular type of three-string braiding statistics for the connected sum of two Hopf links 221#221 configuration. With certain 4-cocycle twist, we find that, by threading a third string through two-string unlink 021 into three-string Hopf links 221#221 configuration, Abelian two-string statistics is promoted to non-Abelian three-string statistics. (Work done in arxiv.org/abs/1404.7854)
Experimental Sightings of the Quantum Spin Liquid

Young Lee Massachusetts Institute of Technology (MIT)

May 01, 2014
PIRSA:14050016

New states of matter may be produced if quantum effects and frustration conspire to prevent the ground state from achieving classical order. An example of a new quantum phase is the quantum spin liquid. Such spin liquids cannot be characterized by local order parameters; rather, they are distinctive by their possession of long range quantum entanglement. I will describe recent experimental progress in the quest to study quantum spin liquids in frustrated magnets. The kagome lattice, composed of corner-sharing triangles, is highly frustrated for antiferromagnetic spins. Materials based on the kagome lattice with spin-1/2 are ideal hosts for quantum spin liquid ground states. I will discuss our group’s work which includes single crystal growth, bulk characterization, and neutron scattering measurements of the S=1/2 kagome lattice material ZnCu3(OH)6Cl2 (also known as herbertsmithite). Our inelastic neutron scattering measurements of the spin correlations in a single crystal sample reveal that the excitations are fractionalized, a hallmark signature of spin liquid physics.
Fractionalized Charge Excitations in a Spin Liquid on Partially-Filled

Gang Chen Fudan University

May 01, 2014
PIRSA:14050024

Electron charge may fractionalize in a quantum spin liquid Mott insulator. We study the Mott transition from a metal to a cluster Mott insulator in the 1/4- and 1/8-filled pyrochlore lattice systems. Such Mott transitions can arise due to charge localization in clusters or in tetrahedron units, driven by the nearest-neighbor repulsion. The resulting cluster Mott insulator is a quantum spin liquid with spinon Fermi surface, but at the same time a novel fractionalized charge liquid with charge excitations carrying half the electron charge. There exist two emergent U(1) gauge fields or "photons" that mediate interactions between spinons and charge excitations, and between fractionalized charge excitations themselves, respectively. In particular, it is suggested that the emergent photons associated with the fractionalized charge excitations can be measured in X-ray scattering experiments. This and other experimental signatures of the quantum spin and fractionalized charge liquid state are discussed in light of candidate materials with partially-filled bands on pyrochlore lattices. “Fractionalized Charge Excitations in a Spin Liquid on Partially-Filled Pyrochlore Lattice” Electron charge may fractionalize in a quantum spin liquid Mott insulator. We study the Mott transition from a metal to a cluster Mott insulator in the 1/4- and 1/8-filled pyrochlore lattice systems. Such Mott transitions can arise due to charge localization in clusters or in tetrahedron units, driven by the nearest-neighbor repulsion. The resulting cluster Mott insulator is a quantum spin liquid with spinon Fermi surface, but at the same time a novel fractionalized charge liquid with charge excitations carrying half the electron charge. There exist two emergent U(1) gauge fields or "photons" that mediate interactions between spinons and charge excitations, and between fractionalized charge excitations themselves, respectively. In particular, it is suggested that the emergent photons associated with the fractionalized charge excitations can be measured in X-ray scattering experiments. This and other experimental signatures of the quantum spin and fractionalized charge liquid state are discussed in light of candidate materials with partially-filled bands on pyrochlore lattices.
Generic Spin Model for Honeycomb Iridates Beyond the Kitaev Limit

Jeffrey Rau University of Toronto

May 01, 2014
PIRSA:14050025

Recently, realizations of Kitaev physics have been sought in the A2IrO3 family of honeycomb iridates, originating from oxygen-mediated exchange through edge-shared octahedra. However, for the J=1/2 Mott insulator in these materials exchange from direct d-orbital overlap is relevant, and it was proposed that a Heisenberg term should be added to the Kitaev model. Here we provide the generic nearest-neighbour spin Hamiltonian when both oxygen-mediated and direct overlap are present, containing a bond dependent off-diagonal exchange in addition to Heisenberg and Kitaev terms. We analyze this complete model using a combination of classical techniques and exact diagonalization. Near the Kitaev limit, we find new magnetic phases, 120 degree and incommensurate spiral order, as well as extended regions of zigzag and stripy order. Possible applications to Na2IrO3 and Li2IrO3 are discussed.
Using β-NMR to Solve Hard Problems in Soft Condensed Matter

James Forrest

May 01, 2014
PIRSA:14050023

Beta-detected nuclear spin relaxation of 8Li+ has been used to study important problems in polymer physics. In the first case we probe the depth dependence of molecular dynamics in high- and low-molecular-weight deuterated polystyrene (PS-d8). The average nuclear spin-lattice relaxation rate, 1/T1 avg, is a measure of the spectral density of the polymer dynamics at the Larmor frequency (41MHz at 6.55Tesla). The mean fluctuation rate decreases approximately exponentially with distance from the free surface, returning to bulk behavior for depths greater than ~10nm and the effective thickness of the surface region increases with increasing temperature. These results present challenges for the current understanding of dynamics near the free surface of polymer glasses. In the second case, we use the technique to make the first quantitative measurements of surface segregation in samples that are blends of two chemically identical polymers with different degrees of polymerization.
Strain Induces Helical Flat Band & Interface Superconductivity in Topological Crystalline Insulators

Evelyn Tang Rice University

May 01, 2014
PIRSA:14050017

Topological crystalline insulators in IV-VI compounds host novel topological surface states, that at low energy, consist of multi-valley massless Dirac fermions. We show that strain generically acts as an effective gauge field on these Dirac fermion surface states and creates pseudo-Landau orbitals without breaking time-reversal symmetry. We predict this is naturally realized in IV-VI semiconductor heterostructures due to the spontaneous formation of a misfit dislocation array at the interface, where the zero-energy Landau orbitals form a nearly flat band. We propose that the high density of states of this topological flat band gives rise to the experimentally observed interface superconductivity in IV-VI semiconductor multilayers at temperatures that are unusually high for semiconductors, and explains its non-BCS dependence on dislocation array period.
Measurements of Noice in Condensed Matter Systems Using Superconducting Qubits and Resonators

Adrian Lupascu Institute for Quantum Computing (IQC)

May 01, 2014
PIRSA:14050018

Superconducting qubits based on Josephson junctions and resonators are presently leading candidates for the implementation of quantum computing. These systems couple strongly to their environment, which often makes preservation of coherence challenging. This strong coupling can be turned into an advantage: it enables the investigation of noise and loss at low temperatures. I will discuss two topics. The first topic is the use of superconducting flux qubits to measure magnetic flux noise. The second topic is the measurement of microwave loss in amorphous dielectric materials. Experiments with superconducting coherent systems can be used to extract new information on flux noise and dielectric loss, not accessible using other methods used in the past, providing useful input to theoretical developments.

Title	Speaker(s)	Date	Talk Type	Info
Welcome Address	Michel Gingras	2014-05-01	Conference	View details
Localization-Protected Quantum Order	David Huse	2014-05-01	Conference	View details
Entanglement, Ergodicity, and Many-Body Localization	Dmitry Abanin	2014-05-01	Conference	View details
Exotic Magnetism on the FCC Lattice of 5dn Double Perovskites	Edwin Kermarrec	2014-05-01	Conference	View details
Renormalization Group Analysis of a Non-Fermi Liquid System	Ipsita Mandal	2014-05-01	Conference	View details
Non-Abelian String and Particle Braiding in 3+1D Topological Order	Juven Wang	2014-05-01	Conference	View details
Experimental Sightings of the Quantum Spin Liquid	Young Lee	2014-05-01	Conference	View details
Fractionalized Charge Excitations in a Spin Liquid on Partially-Filled	Gang Chen	2014-05-01	Conference	View details
Generic Spin Model for Honeycomb Iridates Beyond the Kitaev Limit	Jeffrey Rau	2014-05-01	Conference	View details
Using β-NMR to Solve Hard Problems in Soft Condensed Matter	James Forrest	2014-05-01	Conference	View details
Strain Induces Helical Flat Band & Interface Superconductivity in Topological Crystalline Insulators	Evelyn Tang	2014-05-01	Conference	View details
Measurements of Noice in Condensed Matter Systems Using Superconducting Qubits and Resonators	Adrian Lupascu	2014-05-01	Conference	View details

4 Corners Southwest Ontario Condensed Matter Physics Symposium 2014

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