Fall 2013
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September 3, 2013 at 11:00am
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Prof.
Michele
Modugno,
University of
the Basque
Country,
Bilbao (Spain)
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Tight
binding models
for ultracold
atoms in
optical
lattices
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(Host:
Dominik
Schneble)
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I
will discuss
how to
construct
tight-binding
models for
ultracold
atoms in
optical
lattices, by
means of the
maximally
localized
Wannier
functions for
composite
bands.
Specific
examples will
be given for
the case
graphene-like
potentials
with two
degenerate
minima per
unit cell,
where a
tight-binding
model with up
to
third-nearest
neighbors is
capable to
reproduce the
structure of
the Dirac
points in a
range of
typical
experimental
parameters
(see the
recent
experiment by
Tarruell et
al., Nature
483, 302
(2012)). I
will also
briefly review
other recent
theoretical
results,
including
anomalous
Bloch
oscillations,
shortcuts to
adiabaticity,
and quantum
backflow.
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September 17, 2013
(P&A COLLOQIUM)
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Prof.
Brian DeMarco
University of
Illinois at
Urbana
Champaign
|
Ultracold
Disordered
Quantum Gases
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(Host:
Dominik
Schneble)
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Disorder
is the rule,
rather than
the exception,
in nature.
Despite this,
we understand
little about
how disorder
affects
interacting
quantum
matter. I will
give an
overview of
our
experiments
using
ultracold atom
gases to probe
paradigms of
interacting
disordered
quantum
particles. We
introduce
disorder to
naturally
clean atomic
gases cooled
to billionths
of a degree
above absolute
zero using
focused
optical
speckle. I
will explain
how we observe
Anderson
localization-a
spectacular
phenomenon in
which
interference
prevents waves
from
propagating in
a disordered
medium-of
quantum matter
in three
dimensions. I
will also show
how we combine
speckle with
an optical
crystal to
emulate a
completely
tunable and
precisely
characterized
disordered
quantum solid.
In these
optical
lattice
experiments,
we realize
disordered
Hubbard models
that we use to
answer
critical
questions
regarding how
disorder
impacts the
properties of
electronic
solids, such
as
superconductors
and metals.
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September 20, 2013 at 1:00pm
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Dr.
Stephen Hogan,
University
College London
(UK)
|
Guiding,
decelerating
and trapping
cold Rydberg
atoms
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(Host:
Hal
Metcalf)
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The
development of
methods to
manipulate the
translational
motion of
atoms and
molecules in
Rydberg states
using
inhomogeneous
electric
fields [1,2],
has led to the
realisation of
Rydberg atom
and molecule
optics
elements
including
mirrors [3],
lenses [4] and
traps [5-6].
These devices
have
applications
in (i) the
development of
hybrid
approaches to
quantum
information
processing
involving
Rydberg atoms
and microwave
circuits, (ii)
the
preparation of
gas-phase
molecular
samples at
temperatures
below 1 K, for
studies of
slow decay
processes and
low-energy
scattering,
and (iii) the
confinement
and
manipulation
of
anti-hydrogen
atoms. In this
talk I will
describe
experiments
with hydrogen
Rydberg atoms
in
three-dimensional
electrostatic
traps, with an
emphasis on
the role of
radiative
processes in
the decay of
the trapped
samples, and
recently
developed
surface-based
guides,
decelerators
and traps for
atoms and
molecules in
Rydberg
states.
[1] W.
H. Wing, Phys.
Rev. Lett.,
45, 631 (1980)
[2] T. Breeden
and H.
Metcalf, Phys.
Rev. Lett.,
47, 1726
(1981)
[3] E. Vliegen
and F. Merkt,
Phys. Rev.
Lett., 97,
033002 (2006)
[4] E.
Vliegen, P.
Limacher and
F. Merkt, Eur.
Phys. J. D,
40, 73 (2006)
[5] S. D.
Hogan and F.
Merkt, Phys.
Rev. Lett.,
100, 043001
(2008)
[6] S. D.
Hogan, P.
Allmendinger,
H.
Sassmannshausen,
H. Schmutz and
F. Merkt,
Phys. Rev.
Lett., 108,
063008 (2012)
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October 14, 2013
|
Dr.
Michael
Spanner,
NRC, Ottawa
|
Toward
ab-initio
simulations of
strong-field
ionization of
molecules
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(Host:
Tom
Weinacht)
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A
growing trend
in today's
ultrafast
laser
community is
strong-field
attosecond
science.
A core process
in attosecond
physics is
ultrafast
strong-field
ionization.
In this
process, a
strong laser
field ionizes
an atom or
molecule
during a
single
half-cycle of
the driving
laser
field.
Sub-cycle
ionization
leads to a
number of
interesting
phenomema
including
high-harmonic
generation and
attosecond
pulse
generation.
In this talk,
I will outline
some recent
attempts at
modelling
sub-cycle
strong-field
ionization
from molecules
from an
ab-initio-type
electronic
structure
perspective.
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October 21, 2013
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Chris
Corder,
Brian Arnold,
and Hal
Metcalf, SBU
|
Laser
Cooling of
Helium
Metastable
Atom Beams
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This
is the first
of an
experiment to
have some of
our seminar
days devoted
to research
within our
five
groups.
This talk will
be given by
Chris Corder,
Brian Arnold,
and Hal
Metcalf
together.
It will begin
with a brief
discussion of
the role of
energy,
momentum, and
entropy in
laser
cooling.
The underlying
background
will address
the question
of whether
laser cooling
is possible
without
spontaneous
emission.
Chris will
then describe
how the
bichromatic
optical force
can test
experimentally
the topic of
laser cooling
without
spontaneous
emission.
He will
describe the
bichromatic
dressed atom
picture, his
apparatus, the
details of
avoiding
spontaneous
emission, and
present his
results. Brian
Arnold has
done Monte
Carlo
simulations of
the
experiment,
and he will
describe how
the program
works and its
results, and
together Chris
and Brian will
compare the
data and the
simulation
results
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November 4, 2013
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Dr.
Valentin Murg,
Universität
Wien (Austria)
|
Adiabatic
Preparation of
a Heisenberg
Antiferromagnet
Using an
Optical
Superlattice
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(Host:
Dominik
Schneble/Vladimir
Korepin)
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We
analyze the
possibility to
prepare a
Heisenberg
antiferromagnet
with cold
fermions in
optical
lattices,
starting from
a band
insulator and
adiabatically
changing the
lattice
potential. The
numerical
simulation of
the dynamics
in 1D allows
us to identify
the conditions
for success,
and to study
the influence
that the
presence of
holes in the
initial state
may have on
the protocol.
We also extend
our results to
two-dimensional
systems.
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November 11, 2013
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Vincent
Tagliamonti,
University of
Connecticut,
Storrs
|
Strong
Field
Ionization of
a Diatomic
Molecule using
1w2w Ultrafast
Laser Pulses
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(Host:
Tom
Weinacht)
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I
will discuss
two
experiments
examining the
effects of
strong field
ionization in
diatomic
iodine in the
presence of a
two-color
(1w2w)
femtosecond
laser
pulse.
The spatial
asymmetry of
the 1w2w pulse
breaks the
spatial
symmetry of
ionization
allowing for
control over
directions of
ion yields
while
providing
insight into
the physics of
ionization. In
particular,
this work
studies
excited states
of the doubly
ionized
molecule which
are produced
via two
processes,
described as
asymmetric
production and
depletion of a
charge
asymmetric
dissociation
channel. In
the production
experiment a
pump-probe
technique is
used to excite
I2 to the B
state of the
neutral which
is
subsequently
ionized by a
two-color
(800- and
400-nm) probe
pulse. By
varying the
relative phase
of the two
colors we are
able to probe
the asymmetric
dissociation
of (I2)2+ →
I2+ + I and we
observe
spatial
asymmetries in
the ion yield
of this (2,0)
channel.
Because the
durations (35
fs) of the
pump and probe
pulses are
much shorter
than the
vibrational
period of the
B state (700
fs) we can
fully resolve
the dynamics
as a function
of
internuclear
separation
R. The
depletion
experiment
uses a pump
pulse at 800
nm to create a
wave packet in
the(2,0). As
the molecule
dissociates, a
two-color
probe pulse is
used to study
the dynamics
as a function
of R. We
find a
critical
region of RÂin
which there is
spatially
asymmetric
enhanced
ionization of
the (2,0)
channel to a
counterintuitive
(1,2) channel.
In this region
the neutral
iodine atom is
ionized such
that one
electron is
released to
the continuum
and another is
transferred to
the 2+ ion.
The production
experiment
results in a
description of
ionization
into coherent
mixed states
of the
dication while
the depletion
experiment
reveals
prominent
multielectron
dynamics near
R
critical.
The first
experimental
evidence for
enhanced
ionization in
1994 by
Corkum, et al,
and the
applicability
of one and two
electron
ionization
dynamics will
be discussed
through simple
models and
quantum
mechanical
simulations.
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November 18, 2013
|
Dr.
Arthur Mills,
University of
British
Columbia
|
XUV
Frequency
Combs for
Photoemission
Spectroscopy
of Condensed
Matter Systems
|
(Host:
Tom
Allision )
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XUV
frequency
combs
generated via
high harmonic
generation in
femtosecond
enhancement
cavities
(fsEC) are
coherent,
table-top
sources of XUV
and VUV
capable of
operating at
very high
repetition
rates (>10
MHz) and high
flux
(>10^12
photons/s).
Given this
level of
performance
these fsEC
sources are
beginning to
see use in
more
experiments as
their
characteristics
are better
understood,
optimized and
controlled. In
this talk I
will discuss
our progress
toward
application of
fsEC sources
(in the 6-25
eV photon
energy range)
to
angle-resolved
photoemission
spectroscopy
(ARPES) of
condensed
matter
systems,
including
equilibrium
studies and
time-resolved
pump-probe
measurements.
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November 25, 2013
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Dr.
Doug Broege,
Stanford
University
|
Impulsive
alignment in
dense
molecular
ensembles:
high
temperatures
and new
directions
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(Host:
Tom
Weinacht
)
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An
aligned
molecular
ensemble is
useful in many
experiments
geared toward
structure
determination
ranging from
spectroscopy
to x-ray
scattering.
One technique,
known as
impulsive, or
field-free
alignment, is
the result of
a strong
torque applied
over a short
period of
time.
The wavepacket
created by
this torque
exhibits field
free alignment
along the axis
of
polarization
immediately
following the
impulse, and
at
revivals.
We describe
measurements
of these
wavepackets
carried out at
temperatures
over 400
degrees K in
molecular
iodine, and
the effects
that
centrifugal
distortion and
vibrational
excitation
have on its
revivals.
We will also
discuss a
technique
developed to
align
molecular
ensembles
along the
direction of
laser
propagation
without the
need for a
crossed-beam
geometry.
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December 9, 2013
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Dr.
Sid Cahn,
Yale
University
|
The
Search for
Nuclear
Anapole
Moments in
Diatomic
Molecules
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(Host:
Hal
Metalf)
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Nuclear
spin-dependent
parity
nonconservation
(NSD-PNC)
effects arise
from exchange
of the Z^0
boson
(parameterized
by the
electroweak
coupling
constants
C2{P,N})
between
electrons and
the nucleus,
and from the
interaction of
electrons with
the nuclear
anapole
moment, a
parity-odd
magnetic
moment. The
latter scales
with the
nucleon number
A of the
nucleus as
A^(3/2), while
the Z^0
coupling is
independent of
A; the former
will be the
dominant
source of
NSD-PNC in
nuclei with A
= 20. NSD-PNC
effects can be
dramatically
amplified in
diatomic
molecules by
bringing two
levels of
opposite
parity close
to degeneracy
in a strong
magnetic
field. This
opens the
prospect for
measurements
across a broad
range of
nuclei. As a
precursor to
the
measurement of
the nuclear
anapole moment
of 137Ba, we
have
experimentally
observed and
characterized
opposite-parity
level
crossings in
138BaF. These
are found to
be in
excellent
agreement with
parameter-free
predictions
and indicate
that the
sensitivity
necessary for
NSD-PNC
measurements
should be
within
reach.
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Wed, December 11, 2013, 2:30pm
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Dr.
Andrew Grier,
Laboratoire
Kastler-Brossel,
ENS, Paris
|
Atoms
at Resonance:
Scattering and
losses of a
Bose gas at
unitarity
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(Host:
Dominik
Schneble)
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Tunability
of the
two-body
scattering
properties in
ultracold
atomic gases
has proven to
be a powerful
tool in recent
years,
providing the
first direct
experimental
evidence of
long-predicted
Efimov states
and allowing
for quantum
simulation of
unreachable or
computationally
intractable
systems.
In this talk,
we will review
recent
experimental
and
theoretical
results
centered
around
ultracold
atomic Bose
gases taken
close to a
scattering
resonance
where the
two-body
scattering
cross-section
diverges.
We will focus
on
measurements
of the decay
of a
non-degenerate
gas both at
and in the
vicinity of
the scattering
resonance due
to three-body
recombination
processes.
We will
present a
theoretical
framework for
understanding
the rate of
these events
based on
universal
Efimovian
physics, and
use this
theory to
explore how
one might
stabilize a
unitary Bose
gas.
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