Date & time | Speaker & affiliation | Talk title & abstract |
Jan 9 4:00pm | no talk | |
Jan 16 4:00pm | Adam Kaminski (AMES lab & Iowa State University) | From coupled CuO chains to CuO2 planes:
solving cuprate puzzle
Abstract: Copper oxygen planes - the nest of high temperature
superconductivity have long resisted theoretical treatment by various
analytical and numerical methods. One approach proposed in the past was
to start with weakly coupled 1D CuO chains and then increase the coupling
to get insights about properties of the planes. In this talk I will
present the data from such system and compare it to rigorous theoretical
calculations.
|
Jan 23 4:00pm | Martin Greven (Stanford) | Recent neutron
scattering results for the high-temperature superconductors
Nd2-xCexCuO4+δ
and HgBa2CuO4+δ
Abstract: High-temperature
superconductivity develops near antiferromagnetic (AF) phases, and it
is possible that magnetic excitations contribute to the
superconducting (SC) pairing mechanism. In order to assess the role
of antiferromagnetism, it is essential to understand the doping and
temperature dependence of the two-dimensional AF spin correlations.
The phase diagram is
asymmetric with respect to electron and hole doping, and for the
comparatively less-studied electron-doped materials, the AF phase
extends much further with doping and it appears to overlap with the
SC phase: the archetypical compound
Nd2-xCexCuO4+δ
shows bulk superconductivity above x~0.13, while evidence for AF
order has been found up to x~0.17. However, our new inelastic
magnetic neutron scattering measurements point to the distinct
possibility that superconductivity does not co-exist with genuine
long-range antiferromagnetism [1]. We furthermore show evidence that
the pseudogap phenomenon in the electron-doped materials arises from
a build-up of AF spin correlations. Finally, we present our latest
results for the AF spin excitations [2], which force us to conclude
that recent claims for the existence of a magnetic resonance in the
electron-doped cuprates have to be reinterpreted.
In a separate effort,
we have succeeded in growing sizable single crystals of HgBa2CuO4+δ,
the single-layer hole-doped compound with the highest superconducting
transition temperature. Our inelastic neutron scattering results
reveal that the magnetic resonance occurs at an unexpectedly high
energy [3]. Finally, we discuss very recent polarized neutron
diffraction data that clearly reveal the existence of "hidden"
magnetic order in the pseudogap phase of HgBa2CuO4+δ
[4]. |
Jan 30 4:00pm | Joel Moore (UC Berkeley & LBNL) | Spin Hall and spin drag effects in two- and three-dimensional materials
Abstract:
Recent experimental and theoretical work reveals several ways in
which spin transport differs fundamentally from charge transport. This
talk first reviews the spin drag effect observed in semiconductor
quantum wells as an example of how interactions modify spin transport more
strongly than charge transport. We then discuss the "topological insulator"
phase of two- and three-dimensional materials, which shows a robust spin
Hall effect carried by edge states and may have been observed recently
in HgTe structures.
|
Feb 6 4:00pm | no talk | |
Feb 13 4:00pm | no talk | |
Feb 20 4:00pm | Vadim Oganesyan (Yale) | Quantum and classical localization of interacting particles at
finite temperature.
Abstract:
Ergodicity of many-particle motion is a fundamental assumption that
underlies, among other things, the powerful statistical mechanics
description of nature. The ergodic hypothesis can break down under
some conditions, most notably in the presence of strong random
potentials leading the phenomenon of Anderson localization. The
theory of Anderson localization assumes no interactions among
particles and it is of considerable practical interest to know whether
the phenomenon can persist more generally. I review some recent ideas
and results on spectral and transport properties of quantum and
classical many-body systems. Within limitations of our methods we
observe that localized states of classical particles are unstable
against non-linearities, while interacting quantum particles can
remain insulating.
|
Feb 27 4:00pm | Maria D'Orsogna (Cal. State Northridge) | Patterns, Stability and collapse for two-dimensional
biological swarms
Abstract:
One of the most fascinating biological phenomena is the self-
organization
of individual members of a species moving in unison with one another,
forming elegant and coherent aggregation patterns.
Schools of fish, flocks of birds and swarms of insects
arise in response to external stimuli or by direct interaction, and
are
able to fulfill tasks much more efficiently than single agents.
How do these patterns arise? What are their properties?
How are individual characteristics linked to collective behaviors?
In this talk we discuss various aspects of biological swarming as seen
through the eyes of a physicist.
In particular, we investigate a non-linear system of
self propelled agents that interact via pairwise attractive and
repulsive
potentials. We are able to predict distinct
aggregation morphologies, such as flocks and vortices, and by
utilizing statistical mechanics tools,
to relate the interaction potential to the collapsing or
dispersing behavior of aggregates as the number of constituents
increases.
We also discuss passage to the continuum and possible applications
of this work to the development of artificial swarming teams.
|
Mar 5 4:00pm | no talk | |
Mar 12 4:00pm | no talk | |
Mar 19 4:00pm | Oleg Kogan (Caltech) | Renormalization group method for predicting
frequency clusters in a chain of nearest-neighbor
phase oscillators.
Abstract:
Collective behavior of systems with quenched disorder
is an active area of research. In the classical
arena, one such problem is synchronization of
self-sustaining oscillators with randomly-distributed
intrinsic frequencies. These form a class of models
for a variety of natural and man-made systems, ranging
from neural networks to integrated arrays of
nanomechanical oscillators. In this talk I will begin
with an overview of some known facts about such
models, including the paradigm known as the Kuramoto
model and circumstances under which it may exhibit a
transition to a state of global frequency
"entrainment". It is known that such transition does
not occur in a 1-dimensional chain of self-sustaining
phase oscillators coupled via nearest-neighbor
interaction. However, the system does develop
interesting collective structures such as clusters of
common frequency. In the second part of the talk I
will describe our effort to predict properties of such
clusters by means of a renormalization group (RG)
method. The method is designed to work in the regime
of strong randomness, where the distribution of
intrinsic frequencies and couplings has long tails.
We implement the RG numerically and obtain statistics
of cluster sizes and frequencies. Our results are
consistent with those obtained by direct numerical
solution of the chain's equation of motion.
|
Mar 26 4:00pm | sping break |
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