Seminars
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Seminars
will be held held
at room S-141 in the Physics and
Astronomy Department building on
Mondays at 4:00 PM, unless noted
otherwise.
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Spring/Summer 2015
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February 6, 2015 (Thurs, 2:30pm,
YITP Common
Room)
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Dongling
Deng
University of
Michigan
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Probing
knots and Hopf
insulators
with ultracold
atoms
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(Host:
Tzu-Chieh Wei)
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Knots
and links are
fascinating
and intricate
topological
objects that
have played a
prominent role
in physical
and life
sciences.
Their
influence
spans from DNA
and molecular
chemistry to
vortices in
superfluid
helium,
defects in
liquid
crystals and
cosmic strings
in the early
universe.
Here, we show
that knotted
structures
also exist in
a peculiar
class of three
dimensional
topological
insulators---the
Hopf
insulators. In
particular, we
demonstrate
that the spin
textures of
Hopf
insulators in
momentum space
are twisted in
a nontrivial
way, which
implies
various knot
and link
structures. We
further
illustrate
that the knots
and nontrivial
spin textures
can be probed
via standard
time-of-flight
images in cold
atoms as
preimage
contours of
spin
orientations
in
stereographic
coordinates.
The extracted
Hopf
invariants,
knots, and
links are
validated to
be robust to
typical
experimental
imperfections.
Our work
establishes
the existence
of knotted
structures in
cold atoms and
may have
potential
applications
in spintronics
and quantum
information
processing.
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February 9, 2015
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Dr.
Alexander
Turbiner
National
Autonomous
University of
Mexico, Mexico
City
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Helium-like
Coulomb
system: two
critical
charges, 2nd
excited state
of He- ion,
and all that
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(Host:
Tom Bergeman)
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Reduced
Coulomb
problem of two
electrons in
the field of
charged fixed
center $Z$
$(H^-, He,
Li^+, \ldots)$
is discussed.
Current
situation with
$1/Z$
expansion is
reviewed,
numerical
deficiencies
of previously
firmly-established
results are
indicated.
First nuclear
critical
charge
(corresponding
the zero
ionization
energy) is
established
with high
accuracy
(Drake et al,
2014;
Olivares-Pilon
et al, 2014)).
Second nuclear
critical
charge
predicted by
Stillinger and
Stillinger
(1966, 1974)
is calculated
as well as its
associated
square-root
branch point
singularity
with exponent
3/2. It
implies (i)
the level
crossing
$1S-2S$ and
(ii) the
existence of
the bound
state embedded
to continuum.
It seems it
leads to the
existence of
the
spin-singlet,
second excited
state of
negative
hydrogen ion
of the same
symmetry as
the ground
state situated
very close to
threshold,
which looks as
an
experimental
challenge to
detect.
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February 23, 2015
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Dr.
Ben Sparks
The University
of Melbourne,
Australia
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Towards
Single-Shot
Ultra-fast
Molecular
Imaging with a
Cold Atom
Electron &
Ion Source
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(Host:
Eden Figueroa)
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The
holy grail of
ultrafast
electron
microscopy is
the production
of single-shot
diffraction
images of
non-crystalline
structures, as
they will
allow for the
study of
structural
dynamics of
chemical and
biological
processes by
creating
‘molecular
movies’ [1],
with spatial
resolution of
0.1 nm and
temporal
resolution of
0.1 ps [2,3].
To achieve
this goal we
require a
source that
can produce a
large number
of electrons
in a very
small volume.
One way of
producing such
bunches is by
ionising
clouds of cold
atoms [4-5].
The electrons
produced from
such a source
will be very
cold (~10 K)
and therefore
will be much
more focusable
than standard
hot electron
sources and
have a longer
coherence
length (~10
nm) allowing
for imaging of
structures
such as
proteins. The
cost and
bench-top
nature of cold
atom electron
sources is
also an
advantage over
the
billion-dollar
x-ray free
electron
lasers that
are currently
endeavouring
to produce
diffraction
from single
molecules.
Here we
present the
latest
experimental
results from
our rubidium
cold atom
electron and
ion source
[6,7],
demonstrating
its ability to
shape charged
bunches (to
help overcome
bunch
expansion due
to the
self-repulsive
Coulomb
interactions
[8]), as well
as
Rydberg-excitation
(to overcome
disorder-induced
heating for
creating
sub—nm focused
ion spots
[9]), and
single-shot
electron
diffraction
patterns
produced.
References:
[1] R. Dwyer
et al., Phil.
Trans. R. Soc.
364, 741
(2006)
[2] B. J.
Siwick et al.,
Science 302,
1382 (2003)
[3] R.
Srinivasan et
al., Helv.
Chim. Act. 86,
1763 (2008)
[4] B. J.
Claessens et
al., Phys.
Rev. Lett. 95,
164801 (2005)
[5] B. J.
Claessens et
al., Phys.
Plasmas 14,
093101 (2007)
[6] A. J.
McCulloch et
al., Nature
Phys. 7, 785
(2011)
[7] A. J.
McCulloch et
al., Nature
Commun. 4,
1692 (2013)
[8] O. J.
Luiten et al.,
Phys. Rev.
Lett. 93,
094802 (2004)
[9] e.g., see
M.
Robert-de-Saint-Vincent,
C. S. Hofmann,
H. Schempp, G.
Günter, S.
Whitlock, and
M.
Weidemüller,
Phys. Rev.
Lett. 110,
045004 (2013);
G. Bannasch,
T. C. Killian,
and T. Pohl,
Phys. Rev.
Lett. 110,
253003 (2013).
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March 9, 2015
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Prof.
Alexander
Gaeta
Cornell
University
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Chip-Based Optical
Frequency
Combs
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(Host:
Tom Allison)
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Optical frequency combs
are having and
will have
enormous
impact on many
areas of
science and
technology,
including time
and frequency
metrology,
precision
measurement,
telecommunications,
and
astronomy.
I will
describe our
recent
research on a
novel type of
frequency comb
that is based
on parametric
nonlinear
optical
processes in
silicon-based
microresonators.
The dynamical
behavior of
how combs are
generated in
such a system
is complex and
include phase
transitions,
mode locking
and
synchronization,
and
femtosecond
pulse
generation.
Ultimately,
such
chip-based
combs offer
great promise
for creating
devices that
are highly
integrated and
stable and can
operate from
the visible to
mid-infrared
regimes.
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March 23, 2015
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Prof.
Lopez Vieyra
National
Autonomous
University of
Mexico, Mexico
City
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Stable He^- can Exist in
a Strong
Magnetic Field
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(Host:
Tom Bergeman)
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The existence of bound
states of the
system (\alpha
, e, e, e) in
a magnetic
field B is
studied using
the
variational
method. It is
shown that for
B > 0.13
a.u. (1 a.u. =
2.35 x 10^9 G)
this system
gets bound
with total
energy below
the one of the
(\alpha, e, e)
system. It
manifests the
existence of
the stable He-
atomic
ion. Its
ground state
is a spin
doublet ${}^2
(-1)^+$ at
0.74 a.u. >
B > 0.13
a.u. and it
becomes a spin
quartet ${}^4
(-3)^+$
for larger
magnetic
fields. For
0.8 a.u. >
B > 0.7
a.u. the He-
ion has two
(stable) bound
states ${}^2
(-1)^+$ and
${}^4 (-3)^+$.
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April 13, 2015
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Prof.
Jean-Pierre
Wolf
University of
Geneva,
Switzerland
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Towards Quantum Bioassays
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(Host:
Tom Weinacht)
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The identification and
discrimination
of molecules
that exhibit
almost
identical
structures and
spectra using
fluorescence
spectroscopy
is difficult.
By addressing
the molecular
dynamics in
“real time”
and by making
use of
molecular
quantum
interference,
quantum
control
already
demonstrated
its unique
capability of
selectively
exciting or
braking
specific
molecular
bonds. In
order to
evaluate the
capability of
optimal
control for
discriminating
between the
optical
emissions of
nearly
identical
molecules, a
specific
strategy
called
“optimal
dynamic
discrimination
(ODD) [1-3]
was developed.
The capability
of ODD was
demonstrated
on the
discrimination
amongst
riboflavin and
flavin
mononucleotide
in aqueous
solution,
which are
structurally
and
spectroscopically
very similar.
Closed-loop,
adaptive pulse
shaping
discovers a
set of 400 nm
pulses that
induce
disparate
nonlinear
responses from
the two
flavins and
allows for
concomitant
flavin
discrimination
of ~16\sigma.
Additionally,
attainment of
ODD permits
quantitative,
analytical
detection of
the individual
constituents
in a flavin
mixture.
Most of the
absorption
bands of
important
biomolecules
(DNA bases and
proteins) lie,
however,
deeper in the
UV. For this
reason we
developed a
novel deep-UV
all reflective
pulse shaper
based on MOEMS
(Micro-opto-electromechanical
systems)[4],
which has
laser pulse
shaping
capabilities
down to 30 nm
(XUV).
We present
recent
experiments on
the quantum
control of the
fluorescence
of free
aminoacids
(Tryptophan
and
Tyrosin[5]),
dipeptides
(e.g.Trp-Leu,
Trp-Ala,
Trp-Gly) and
large proteins
(antibodies
and albumin).
In this latter
case, we
demonstrated
that major
serum
proteins,
namely
immunoglobulins
(IgG and IgM)
and albumin
can be
discriminated
and
quantified,
label free, in
actual
patients’
blood serum
samples. These
results pave
the way to the
future
development of
“quantum
control based
bio-assays”.
(1) M. Roth,
L. Guyon, J.
Roslund, V.
Boutou, F.
Courvoisier,
J.P. Wolf, H.
Rabitz,
Phys.Rev.Lett
102, 253001
(2009)
(2) J.
Petersen, R.
Mitric, V.
Bonacic-Koutecky,
J.-P. Wolf, J.
Roslund, H.
Rabitz,
Phys.Rev.Lett.
105, 073003
(2010)
(3) J.
Roslund, M.
Roth, L.
Guyon, V.
Boutou, F.
Courvoisier,
J-P Wolf, H.
Rabitz,
J.Chem.Phys.
134, 034511
(2011)
(4) J.
Extermann, S.
M.Weber, D.
Kiselev, L.
Bonacina, S.
Lani, F.
Jutzi,W.
Noell, N. F.
de Rooij, J-P
Wolf, Opt Exp
19, 7580-7586
(2011)
(5) A.
Rondi,
L. Bonacina,
A. Trisorio,
C. Hauri,
J.-P. Wolf,
Phys.Chem.Chem.Phys.
14, 9317-9322
(2012)
(6) S. Afonina
et al, Appl.
Phys. B, 111,
541-549
(2013)ba
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April 20, 2015
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Dr.
Johanan
Odhner
Temple
University
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Filamentation: Pulse
Dynamics and
Applications
in
Spectroscopy
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(Host:
Tom Weinacht)
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Filamentation of high
power
femtosecond
laser pulses
is of growing
interest for
applications
such as
atmospheric
sensing,
control of
plasma
discharges
(artificial
lightning),
laser
plasma-induced
droplet
nucleation
(artificial
cloud and rain
formation),
and backward
lasing. It is
also widely
used for
continuum
generation for
spectroscopy
and as a means
to compression
laser pulses
to just a few
optical cycles
of the carrier
wavelength. A
necessity for
developing a
rigorous
understanding
the
filamentation
process is the
means to study
the
filamentation
process in
situ without
disturbing the
filamentation
process
itself. This
has proved to
be
particularly
challenging
for filaments
generated in
gaseous media,
where pulse
intensities
can reach as
high as 10^14
W/cm2, making
traditional
diagnostic
techniques
inapplicable.
In this talk
we explore two
new methods
for probing
the pulse
reshaping
dynamics
directly in
gas phase
filaments, as
well as some
of the
spectroscopic
tools and
applications
that have
resulted from
those
studies.
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June 16, 2015 (Tue, 11am)
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Prof.
Giuseppe
Vallone
University of
Padova, Italy
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From Bell inequalities to
quantum
information
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(Host:
Eden Figueroa)
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Quantum mechanics (QM) is
one of the
most amazing
and
revolutionary
discoveries of
the last
century. Among
its
counterintuitive
predictions we
can recall the
uncertainty
principle, the
wave-particle
duality, the
superposition
of quantum
states, the
entanglement
and the Bell
inequalities.
The
predictions of
QM have been
verified in
several
experiments
and
now quantum
mechanics is
at the basis
of Quantum
Information
(QI), that
studies the
ability to
manipulate and
transmit
information in
a totally
innovative way
with respect
to the
possibilities
offered by
classical
physics. After
a brief
introduction
to the
fundamental
concepts of
quantum
mechanics, we
will present
some QI
applications
such as
quantum
communication,
Quantum Key
Distribution,
and random
number
generators.
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June 17, 2015 (Wed, 2pm)
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Prof.
Paolo
Villoresi
University of
Padova, Italy
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Quantum
Communications
for Distant
Correspondents
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(Host:
Eden Figueroa)
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The paradigm shift that
Quantum
Communications
represent vs.
classical
counterpart
allows
envisaging the
application of
global
cryptographic
key
distribution
as well as of
other quantum
technologies.
Quantum
Communications
on planetary
scale require
complementary
channels
including
ground and
satellite
links. As the
former have
progressed up
to commercial
stage using
fiber-cables,
it's crucial
the study of
links for
space QC and
eventually the
demonstration
of protocols
such as
quantum-key-distribution
(QKD) and
quantum
teleportation
along
satellite-to-ground
or
intersatellite
links. In
recent
announcements,
the launch of
dedicated
mission was
envisaged.
Indeed, the
sharing of
quantum states
among ground
and orbiting
terminal may
be considered
as feasible
according to
present
optical
technologies.
However, the
extension of
the Quantum
Communications
and
Technologies
to long
distances, on
the surface of
the Earth as
well as from
the Earth to
an orbiting
terminal in
Space, is
influenced by
difficulties,
among which
the moving
terminals, the
large losses,
the effects on
the optical
propagation of
the turbulent
medium.
Indeed, the
quantum state
that is
prepared and
sent at the
transmitter
side
experiences a
transformation
in the spatial
spectrum in
addition to
the vacuum
diffraction,
that requires
strategies to
be
compensated.
We will
address the
experimental
studies on the
faithful
transmission
of qubits from
Space to
ground and
from distant
terminals on
the Earth
which
demonstrates
the means for
realizing
Quantum
Communications
on these
channels.
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July 13, 2015
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Dr.
Reihaneh
Shahrokhshahi
University of
Virginia
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A cavity enhanced
narrow-band
multi-photon
source for
applications
in quantum
information
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(Host:
Eden Figueroa)
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Photons prepared in Fock
states have
been a subject
of great
interest due
to the
non-Gaussian
(negative)
nature of
their Wigner
function.
These quantum
states are the
essence of the
quantum nature
of light and
have
applications
in quantum
cryptography,
quantum
information
processing and
universal
quantum
computing. The
generation of
the Fock
states has
been most
commonly
achieved by
using
spontaneous
parametric
down-conversion
(SPDC) in
nonlinear
crystals, but
the fidelity
and the
success rate
of Fock state
generation was
limited by the
multimode
nature of SPDC
photons. In
this talk, I
will describe
the
investigation
of
cavity-enhanced
SPDC modes for
higher-fidelity
photon pair
generation. We
have built an
intrinsically
stable OPO,
whose
well-defined
cavity modes
were used to
herald
photons, with
up to 80%
success rate
in preliminary
results. The
heralding and
measurements
were performed
by
photon-number-resolving,
high-quantum-efficiency,
transition
edge sensors,
built at NIST
by Sae Woo
Nam's group.
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July 16, 2015 (Thurs, 2:30pm,
YITP Common
Room)
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Dr.
Gyanyu Zhu
Northwestern University
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Wonders in flat bands:
from quantum
liquid
crystals to
self-correcting
quantum memory
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(Host:
Tzu-Chieh Wei)
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In this talk, I will
discuss two
cases where
flat bands in
frustrated
lattice models
lead to
emergence of
interesting
physics.
In the first
part, I talk
about a family
of interacting
boson models
based on a
kagome lattice
with local
synthetic
gauge flux,
which can be
realized in
optical
lattices with
ultra-cold
atoms or
circuit-QED
lattices with
interacting
photons. Such
models have a
lowest flat
band in the
single-particle
spectrum. The
flat band is
spanned by
eigenstates
forming
localized
loops on the
lattice, with
the maximally
compact loop
states
typically
breaking the
discrete
rotational
symmetry of
the lattice.
When populated
by
locally-interacting
particles, the
close packing
of such
maximally
compact loop
states leads
to a nematic
loop crystal
ground state.
We predict
that
increasing the
filling beyond
the close
packing
fraction leads
to the
formation of
quantum liquid
crystals
including a
nematic
supersolid and
a nematic
superfluid
phase. We also
show how the
nematicity can
be probed by
time-of-flight
experiments or
phase
imprinting
techniques
[1].
In the second
part, I
discuss how
4-body spin
interactions
can emerge in
a 2D flat-band
lattice with
"Aharonov-Bohm
cages", and in
the presence
of
light-matter
interactions.
Based on such
an idea, one
can realize
the
surface-code
Hamiltonian in
the
ultra-strong
coupling
regime of a
circuit-QED
lattice, when
the
interaction
strength is
comparable to
the microwave
photon
frequency.
Two types of
4-body
stabilizer
interactions
are realized
by utilizing
the
electro-magnetic
duality in
circuit-QED.
In such case,
the
circuit-QED
vacuum has
topological
degeneracies
and can be
used as a
self-correcting
quantum
memory.
An alternative
approach
without
ultra-strong
coupling is to
simulate the
surface-code
Hamiltonian in
the rotating
frame, with
side-band
driving
through
modulating the
flux
penetrating
SQUID
couplers.
[1]
Guanyu Zhu,
Jens Koch and
Ivar
Martin,
arXiv:1411.0043.
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July 16, 2015 (Thurs,
4:00pm)
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Dr.
Aye Lu Win
Old Dominion
University
|
Catalysis of Stark-tuned
Interactions
between
Ultracold
Rydberg Atoms
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(Host:
Eden Figueroa)
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The experimental
investigations
of the
catalysis
effect in the
resonant
energy
transfer
between
ultracold 85Rb
Rydberg atoms
will be
presented. We
have
investigated
the energy
transfer
process of 34p
+ 34p →Â
34s + 35s, and
observed
Stark-tuned
Förster
resonances.
When
additional
Rydberg atoms
of 34d state
are included
in the
interaction,
an increase in
the population
of 34s states
atoms was
observed.
Although the
34d state
atoms do not
directly
participate in
the resonant
energy
transfer that
produces 34s
state atoms,
they add an
additional
interaction
channel 34p +
34d → 34d
+ 34p that is
resonant for
all electric
fields. We
have also
investigated
the time
dependence of
the resonant
interactions
of 34p +
34p→ 34s +
35s, compared
the
experimental
results with
the numerical
simulations of
simple models,
and found them
to be in good
agreement.
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August 3, 2015 (2:45pm) time
change
|
Azure
Hansen
University of Rochester
|
Topological spin textures
in spinor
Bose-Einstein
condensates
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(Host:
Tom Bergeman)
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We generate spin textures
in an 87-Rb
Bose-Einstein
condensate
with diverse
symmetry and
topological
properties,
including spin
monopoles,
non-Abelian
vortices,
fractional
vortices, and
coreless
vortices.
Using a
coherent
optical Raman
process we
transfer
spatially-dependent
phase and
polarization
properties
from complex
singular
optical modes
to the
condensate.
This allows us
to engineer
the internal
and external
momenta,
superfluid
velocities,
and spatial
spin
distribution
of the
condensate as
well as
control the
complex
relative
phases of the
magnetic spin
components.
This work will
allow us to
measure a new
geometric
phase in atom
optics, study
interactions
between spin
textures, and
determine the
ground state
spin
interactions
in spin-2
87-Rb
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August 7, 2015 (Friday,
3pm)
|
Prof.
Ágnes Vibók
University of
Debrecen,
Hungary
|
Signatures of
light-induced
conical
intersections
on the
dynamical
properties of
molecular
systems
|
(Host:
Tom Weinacht)
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Nonadiabatic effects are
ubiquitous in
physics,
chemistry and
biology. They
are strongly
amplified by
conical
intersections
(CIs) which
are
degeneracies
between
electronic
states of
triatomic or
larger
molecules. A
few years ago
it has been
revealed that
CIs in
molecular
systems can be
formed by
laser light
even in
diatomics. The
energetic and
internuclear
positions of
these
light-induced
conical
intersections
(LICIs) are
depend on the
laser
frequencies
while the
strength of
their
nonadiabatic
couplings can
be modified by
the field
intensities.
Strong impact
of these LICIs
on different
dynamical
properties of
the diatomics
has been
discussed in
several
papers.
Recently our
attention is
focused on the
description of
the
photodissociation
dynamics of
the D2+
molecule.
Kinetic energy
release (KER)
and angular
distribution
of the
photodissociation
probabilities
are calculated
with and
without LICIs
for different
values of
laser
parameters. By
analyzing this
dynamical
process
carefully, we
found a robust
effect in the
angular
distribution
of the
photofragments
which serves
as a direct
signature of
the LICI
providing
undoubted
evidence for
its existence.
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