
NANOMETRIC-SIZE WIRES CAN BE TUNED EITHER AS INSULATORS OR AS METALS AT WISH
In this paper we report the electrical transport properties of nanometric
wires created by using a very promising nanolithography technique,
focused-ion-beam-induced deposition (FIBID), much simpler than standard
techniques. In FIBID, a gas is decomposed by its interaction with focused
accelerated ions. The grown nanowires are formed by a mixture of platinum
and carbon and, depending on its composition ratio, they behave either as a
metal or as an insulator. As the composition can be tuned by the growth
parameters, nanostructures with completely different electrical
characteristics can be created in a simple one-step process. With this work
we have unified a wide range of previously observed phenomena, and it has
been possible to correlate the electronic properties of the material with
the carbon-platinum ratio. Besides, some of the samples present an
interesting conduction property, hardly found in other systems, as it is the
decrease of the differential conductance with the applied voltage. These
nanowires could be used to create new nano-circuits with several
functionalities.
***
LA12227ER
The Power of Harmony in Vortex Streets
When a fluid flows around a long slender object - called a bluff body - then
impressive structures of contra-rotating vortices appear in the wake behind
it forming a vortex street. A recent study in Physical Review E reveals that
fascinating vortex streets appear in bluff-body wakes if the flow is
perturbed.
A bluff-body wake is essentially a wave-maker which is the source of Aeolian
tones. Thus, changes in the flow speed will be similar to the differences
between pure musical tones, called harmonics, so knowing how much and how
fast it changes (amplitude and frequency) is enough to determine the
characteristics of the wake. It turns out that nonharmonic perturbations,
i.e., changes in the waveform quality but not the main amplitude or
frequency, have a remarkable effect on the vortex dynamics, and
consequently, on the magnitude and phase of the forces exerted on the body.
Understanding this phenomenon is important because it determines the
transfer of energy between the fluid and the body. This knowledge may hold
the key to harnessing the energy from ocean currents and atmospheric winds
more efficiently, or avoiding catastrophic vibrations of offshore
structures.
***
EBR1036

Universal dynamics of jamming particles
We find that a dense assembly of macroscopic particles in a viscous medium
exhibits an exotic cooperative phenomenon, the length and time scales of
which diverge at a certain density in the same manner as that of a
super-cooled liquid. To make the situation more accessible, just imagine
walking across a crowded party room or a rush-hour train, which is almost
impossible unless the people are cooperative. This is actually what happens
in amorphous solids, where the particles are so densely-packed that they
cannot rearrange themselves unless the particles are "cooperative". The
nature of such cooperative motion is the central question in the physics of
glassy materials, as it involves important quantities such as viscosity or
heat capacity. In this paper, using molecular dynamics simulation, we
investigate the nature of the cooperative rearrangement of a dense
particulate system; i.e., how much time does it takes and how many particles
must be cooperative upon the rearrangement. The results bear striking
similarities with a super-cooled liquid.
Figure(EBR1036.jpg): Colored in red is the cooperatively rearranged
particles, which is heterogeneously distributed.
***
LX11486BR

Building Fullerenes Out of Boron
The soccer-ball-shaped C60 buckyball can be viewed as the
smallest molecule in a family of icosahedral carbon fullerenes
that approach the flat graphene sheet when the number of atoms
becomes large. In an article to be published in Physical Review B,
researchers have used computer simulations to show that boron,
carbon's neighbor in the periodic table, can form an analogous family
of stable fullerenes that ranges from the buckyball-like B80 to a
flat boron sheet. Each boron fullerene has a precise structural
relationship to its carbon counterpart, and also has the same number
of valence electrons. In both the icosahedral fullerenes and their boron
analogs, the electronic band gap, which arises from quantum confinement
of electrons, decreases with increasing cluster size. However, unlike
the carbon clusters, for which the band gap approaches zero only in the
limit of infinite size, the boron fullerenes are predicted to transition
to a metallic state at a cluster size of about 2000 atoms.
***
LW11626
A hidden process of sleep
Sleep, an essential part of our lives, commonly consists of
frequent transitions between various sleep states
(including spontaneous awakening periods). In this paper,
we propose a new method, based on a Markov transition matrix,
to quantitatively analyze this time course of sleep.
The transition matrix is determined by statistical analyses of
113 obstructive sleep apnea (OSA) patients who suffer complete or
partial pharyngeal obstruction during sleep. We find that
duration probabilities of each sleep state fit to a modified
exponential distribution, in contrast to recent reports of
a scale-free form for wake and an exponential form for sleep.
This result suggests that sleep can be understood in a unified framework,
providing important constraints for theoretical modeling of sleep.
OSA patients are often aided with continuous positive airway pressure
(CPAP) treatment to improve their sleep quality. We further analyze
sleep of the same subject, but treated with CPAP, and compared with
the pre-treatment ones, suggesting potential applications of our method
in sleep clinics.
***
LX11217
Atomic-scale imaging with ultrasound
In Medicine, ultrasound is successfully used as a non-invasive
tool to image an unborn baby in the mother's womb. As its
counterpart in nanotechnology, we introduce the non-invasive
Damping Force Spectroscopy (DFS) technique capable of imaging
subsurface structures and vibrational modes on the atomic scale by
observing the damping of an oscillating atomic force microscope
(AFM) tip in the "non-contact" regime.
We apply DFS to peapods, consisting of carbon nanotubes filled
with metallofullerenes (hollow C_82 'buckyballs' containing a Dy
atom inside). Spatial maps of the damping signal show atomic-scale
features superior to state-of-the-art topographic AMF images. Not
only can DFS clearly distinguish between empty and filled peapods,
but can also reveal the location and packing of the
metallofullerenes in nanotubes of different diameter as well as
changes of the local vibrational modes.
We trace back the microscopic origin of the damping signal to a
hysteresis in the interaction between the AFM tip and the elastic
peapod. First principles total energy and molecular dynamics
calculations allow us to provide a quantitative interpretation of
the DFS signal by identifying which vibrational modes may be
excited by the AFM tip at a particular location.
***
LV11546
Low power magneto-optical recording in a ferromagnetic semiconductor
Continuing miniaturization is a constant and important goal
of the information industry. A primary obstacle is that smaller bit
sizes require higher coercive field in order to provide stable and
low-noise recording. The strong and highly localized magnetic fields
then needed to switch individual bits are difficult to produce. One
promising approach to address this issue is heat assisted magnetic
recording (HAMR), where a magnetic medium is locally heated by light,
leading to a rapid reduction of its coercive field. This method however
requires large powers and is thus not efficient to commercial. An
alternative approach using light of much lower power would be highly
desirable. In this Letter, we have realized a concept for non-thermal
magneto-optical (MO) recording using very low illumination power. Our
approach is based on light-induced de-pinning of domain walls, rather
than modification of the magnetic interaction. Using this concept we
demonstrated a complete cycle of MO recording with non volatile data
storage. We believe that our findings have the potential to evolve
into an important paradigm for use in information storage technology.
***
LB11686
Violation of mirror symmetry in atoms confirms properties of electroweak vacuum
In physics, the vacuum is never still. Each particle carries a cloud of continuously sprouting virtual particle-antiparticle pairs. The strength of the mutual interaction between two particles becomes dependent on their relative collision energy: at higher energies, the collision partners tend to penetrate deeper inside the shielding clouds. For feeble electroweak interactions, the Standard Model of elementary particles yields an answer for such an energy-dependence (or "running"). Particle colliders provide reference points at high energies. Relatively inexpensive table-top experiments on violation of mirror symmetry in atoms probe the vacuum at low energies. However, for these low energies, where the shielding clouds are penetrated the least, previous analyses were consistent with no running.
Here we improve the accuracy of probing the least-energetic electroweak interaction. We extract the strength of the parity-violating interaction of atomic electrons with quarks of the caesium nucleus by combining previous measurements by C. Wieman group with our calculations. The refined analysis required detailed understanding of correlated motion of 55 electrons of cesium atom. This is not an easy task as the number of memory units required for storing full quantum-mechanical wavefunction exceeds the estimated number of atoms in the Universe. Special tools and approximations were developed. Overall, compared to previous analyses, reaching the next level of accuracy required a factor of 1,000 increase in computational complexity.
Our precision result confirms the fundamental running. Together with the results of high-energy collider experiments, we demonstrate the validity of the predicted running of the electroweak force over an energy range spanning four orders of magnitude (from ~ 10 MeV to ~ 100 GeV).
***
BZ10920
Progressively induced superconductivity in graphene
Graphene, the 1 atom thick carbon crystal, has striking electronic
properties. In particular, current is carried by seemingly mass-less
relativistic particles. This has a lot of interesting consequences, one
of these being the way charges are transferred from graphene to
superconducting electrodes. In graphene, as in any normal metal,
electrons (or holes) are scattered by impurities, giving rise to a
resistance. In a superconductor carriers condense into a coherent
many-body state of electron pairs (Cooper pairs). This leads to the
famous zero resistance state with a supercurrent at zero applied
voltage. What happens if we put a normal metal (N), or graphene, between
two superconductors (S)?
An electron from the normal metal that approaches the interface is
reflected as a hole, so that a pair of electrons can enter the
superconductor. This process depends on the probability of crossing the
interface between the two materials, the so called interface
transparency, which is rarely perfect . Whereas at zero voltage high
interface transparencies enable a large supercurrent through the normal
metal, at finite voltages and moderate transparencies, another process
takes place whereby an electron from the superconducting electrode
enters into the other after bouncing back and forth through the normal
metal between the two S electrodes (multiple Andreev reflections).
In this experiment, by improving the interface transparency between the
superconductor and graphene, we could favor one transport process over
the other. This was done by running a large current through the sample
for a short time. We first observed an increase of multiple Andreev
reflections with no supercurrent, and further annealing led to a high
supercurrent with barely visible multiple Andreev reflections.
***
EY10345
Nanoimprinted Polymer Films Control the Alignment of Rod-like Molecules
Polymer films nanoimprinted with checkerboard patterns of square wells of size varying from 200 nm to 800 nm align calamitic (rod-like) liquid crystals (LCs) vertically, horizontally or tilted depending on the depth/width ratio of the wells. Alignment of LCs is necessary for uniform optical properties of display pixels or enhancement of electrical conductivity of LC devices. Compared to other alignment methods such as mechanical rubbing or chemical modification of substrates, this method enables us to control the alignment of LCs accurately in a variety of direction solely varying the scale and depth of topographic patterns. The LCs prefer to lie down on polymer films that are smooth but when the films are topographically patterned, the increasing elastic energy density as the wells become narrower eventually overcomes the surface anchoring of the polymer and the average orientation of LCs makes a transition from planar to vertical. Nanoimprint uses polymerization of liquid while it is pressed by a mold with very fine patterns and this technique can produce many replicas at low cost. This work demonstrates great potential of using topographically patterned polymer films for the control of optical and electrical properties anisotropic soft matter for advanced and novel devices.
***
LZ10928
Slicing and dicing electronic wavefunctions
How much information does one need to describe the state of a physical
system? This question is intuitively simple in the realm of classical
physics: the information needed is roughly proportional to the size of
the system (at worst, one needs to specify the position of each atom).
But things become more intricate when quantum mechanics is at play. The
system is then described by a /wavefunction/, a complex mathematical
object whose information content can in principle grow exponentially
with the size of the system. Within some commonly used approximations of
quantum theory, the information needed appears to grow like the /square/
of the system size. A natural question then arises: when can a
wavefunction be described with an amount of information that is simply
/proportional/ to the system size?
This paper proposes a practical answer to that question by providing a
new way to decompose a wavefunction into pieces of decreasing sizes.
This process reveals to what extent a wavefunction can be "compressed"
in order to be represented with a minimal amount of information, while
preserving accuracy. An important practical implication of this result
is that it may simplify the way we model quantum mechanical systems
using computers. The vast amount of data needed to describe such systems
has severely limited the size of what can be "simulated" numerically.
Although this problem has been the subject of intensive research in the
past two decades, the present paper offers a promising new way to
describe quantum mechanical systems using as little information as possible.
***
AB10404
Why are ultracold atom Fermi superfluids so special?
Dilute atomic Fermi gases appear to be an unusual example of systems where
the attraction between fermions which leads to Cooper pairs is active over
a range of energies orders of magnitude larger than the Fermi energy.
Equivalently, this attraction, which is tuned by a magnetic field induced
Feshbach resonance, is active over a momentum range which extends to
nearly a thousand times the Fermi momentum. This is known to lead, for
example, to universal high frequency features in the spectroscopy of cold
atomic gases, a phenomenon which has been playfully dubbed the case of the
`tail wagging the dog'. Our recent work on superfluidity of cold Fermi
atoms in an optical lattice appears to provide yet another simple and
remarkable example of such `high energy' physics dominating the behavior
of the superfluidity of these systems. We show two striking results for
such optical lattice superfluids which follow from the assumption that
Cooper pairing between atoms in the lattice only occurs between fermions
in the same band. We show that the Hartree energy shift which is
important for inhomogeneous superconductors is absent for cold Fermi
superfluids in an optical lattice even though their density is nonuniform.
Second, we show that even though the optical lattice Hamiltonian is only
periodic under discrete translations, the pair field is completely uniform
in space. Our results indirectly cast serious doubt on the validity of the
enormous number of theoretical proposals over the years which attempt to
model such atomic superfluids in an optical lattice through the one-band
attractive Hubbard model or its variants.
***
BYR1092B
Manganese ion off-centrality breaks the "d-zero-ness rule" in perovskites.
First principle calculations confirm that Mn ion substituting for Sr
occupies the off-central position in SrTiO3. So, we have proved the
existence of a dipole impurity which possess a magnetic moment and
thus couples both with the magnetic and with the electric field. The
calculations evidence that off-central Mn ion induces a polar state in
the host lattice. This state violates the apparent mutual exclusion of
magnetism and ferroelectricity in perovskites that is called the
"d-zero-ness rule". The rule acknowledges the observation that
transition metal ions can cause a ferroelectric instability only when
they have empty electronic d-shell (see e.g. D.Khomskii, Physics 2, 20
(2009)). Now it seems to be restricted to the d-ions occupying B
position in a perovskite compound ABO3.
***
BV10605
Computer simulation of carbon nanotubes immersed in a fluid under high
pressures.
Due to outstanding elastic properties, carbon nanotubes have been termed
as nature’s ultimate springs. However, some studies found that under
pressure (~2×109 Pa) the tubes loose their shape and collapse to become
ribbon-like whereas others found the tubes retain their shape till much
higher pressures (~1×1010 Pa). To understand the different experimental
results, we theoretically investigated the high pressure behavior of
carbon nanotubes immersed in argon fluid using computer simulations
viz., classical molecular dynamics. We find that when the tubes are
empty they collapse at quite low pressures and form different
configurations of slightly different energies depending on the
conditions in the simulations. On the other hand, when the fluid is
present inside and is surrounding the tubes, their behavior under
pressure is substantially different. Surprisingly, at lower densities of
argon fluid, the pressure required to cause radial collapse is lower
than that of the empty tubes. At higher densities the fluid supports the
tubes and the collapse pressure is found to be higher. Moreover, we find
that the Ar fluid inside the tubes becomes increasingly ordered at
higher pressures. Moreover, the order of argon atoms is constrained more
by the tube-Ar interactions than the inter-atomic interactions amongst
Ar atoms.
***
LA11898A
What is the wave function of a single free particle with a given energy?
Quantum mechanics does not give a procedure to answer this very basic and
fundamental question. It could take a form of a single plane wave, a
Gaussian, or infinite number of other forms. This ambiguity is also part of
the great debate between Einstein and Born. In this paper, we attempted to
answer this question in the frame work of Madelung fluid dynamics as the
generalization of the Schrodinger equation, by allowing a rotational quantum
flow. “We ask for the most probable wave functions of a single particle
with a given energy, by constraining the quantum probability density to
maximize the Shannon information entropy”. We show that there is class
solutions which are self-trapped, rotationally symmetric, spinning yet
stationary. The stationarity is shown to come from the balance between the
attractive force of a self-generated quantum potential and the repulsive
centrifugal force of the spinning velocity field. We also showed that in the
asymptotic limit, the wave function is no more spinning yet is still
stationary and turns out to be equal to the lowest stationary state of the
Schrodinger equation of a single particle trapped in a cylindrical tube
external potential.









