No escape for " relativistic" electron in graphene quantum dots!
The recent discovery of elusive two-dimensional form of carbon
called graphene has unusual electronic
properties that may be useful in the design of new electronic
devices. Electrons in graphene behave
as massless chiral fermions , i.e., ``relativistic'' electrons.
Due to this unique property, the electrons in graphene cannot
be localized by any confinement potential (Klein's paradox).
In this case we need to discuss not the localization but the
trapping of the electrons by confinement potential. The electron
trapping is strongly affected by the sharpness of the confinement
potential, the most efficient trapping is
realized in a smooth confinement potential and
for electronic states with large angular momentum.
Although it is easier to create a confinement potential with
smooth boundary, the quantum dots
with sharp boundary are also important. We show that
for the quantum dots with sharp boundaries there
is a completely new mechanism of trapping. This trapping is
due to interference effect and as a result, it can be observed
for all values of angular momentum.
For smooth boundary the trapping is due to a tunneling and can
be achieved only for large values of angular momentum.
We show that even in the case of
confinement potential with sharp boundaries we can realize the
trapping of the ``relativistic'' electron for a very long time.
For special parameters of the confinement potential, which
can be achieved by an additional tuning of the potential,
the escape rate from some states of the quantum dot can be
exactly zero. Therefore, the ``relativistic'' electrons
in such states are em strongly localized with
infinite trapping time. This localization is achieved
not due to a large trapping potential barrier, but due to
interference effects within the quantum dot.
This opens another possibility for tuning of the trapping
properties of an electron in graphene quantum dots.
***
LL10963
Trapping a rainbow in a simple broadband plasmonic structure
Artists and poets have often dreamed of holding a rainbow in their hand. Meanwhile, more practical engineers and scientists have sought to control pulses of light in novel optical circuits with nanoscale dimensions. In this paper, the authors attempt to do both, and present a detailed discussion of a relatively simple graded metal grating structure to realize such a dream. This structure is capable of slowing down or even stopping light waves over a very wide spectral band at different locations along the surface of the structure. The separation between the adjacent localized frequencies can be tuned freely by changing the grade of the grating depths. The propagation characteristics of these trapped surface modes can be controlled by the surface geometry. Such a feature could open a door to the control of the light wave on-a-chip or even realize novel applications such as a spectrometer integrated on-a-chip for chemical diagnostics, spectroscopy and signal processing applications. Importantly, the current graded grating structures developed for “trapped rainbow” storage of light in the THz domain could be scaled to telecom frequencies for future possible applications of integrated optical and nano-photonic circuits.
***
LL11055
How to reach consensus faster? Slow down!
Imitation of neighboring states ('opinions') may eventually lead to an
ordered state in a spin system ('consensus') - but sometimes it may
take an enormous time to reach consensus, dependent on the system
size. We present an interaction mechanism which allows to drastically
shorten the consensus time - by adding inertia to the individual
transitions. This is counterintuitive as it decelerates the dynamics
on the microlevel, but accelerates the ordering dynamics on the
macrolevel. We find that there is an optimal value at which the
individual 'stubbornness' has to grow over time, to maximize this
effect.
***
LL11471B
Knocking nonlinear modes into existence in uranium
Dynamical modes, which become thermally activated in uranium at high
temperatures, were successfully generated out of equilibrium in cold
crystals using x-ray and neutron scattering. Results show that these
modes are created by amplitude fluctuations that mirror the modes
themselves, providing the first direct evidence of the intrinsic
nature of a localized nonlinear lattice mode in a three-dimensional
crystal. The problem of localized modes in nonlinear lattices has
been of great intellectual interest since the 1950's and has been
studied by the greatest minds, beginning with the pioneering
simulations of Fermi, Pasta and Ulam at Los Alamos. This early work
was motivated not only by the existence of these breather-like modes,
but also by the implications that they pose to the ergodic hypothesis
and the foundations of statistical mechanics. The discovery of these
modes in real materials, however, has more pragmatic ramifications
and applications. Supporting data on uranium shows that these
nonlinear modes influence almost every property, including heat
capacity, thermal transport, thermal expansion, and possibly
mechanical deformation. The influence on thermal transport is
particularly exciting as it opens up new possibilities for the
manipulation of heat in next-generation energy technology. The scale
of the modes also suggests that they could be interfaced with
nanotechnology. Furthermore, evidence suggests that ILMs in uranium
may also act as an incipient driver for a solid-state phase transition.
***
BRR1100
Necktie gaps in modulated two-dimensional electron gas
A periodic potential modulation of two-dimensional electron gas (2DEG)
can give rise to the esthetic "necktie" gaps within the intersubband
single-particle excitations (SPEs). The necktie gaps are found to
center at the zone boundaries in the spectrum showing the excitation
energy vs. the Bloch vector. This phenomenon is apart from the known
minigap plasmons existing inside the gap between the intrasubband and
intersubband SPEs. These are very interesting characteristics of such
an anisotropic system with spatially modulated charge density and with
a weak sinusoidal tunneling in the energy dispersion. Such minigap
engineering makes these nanostructures to nanoplasma physics as
photonic bandgap crystals are to optics and sonic bandgap crystals
are to acoustics. One can also envision a tandem structure made up of
many such modulated 2DEG systems. The samples of such smaller
periodicity (with a period d < 30 nm) with persisting necktie gaps
would be useful as nanofilters and will allow neither the collective
(plasmon) nor the single-particle excitations to propagate in the
given frequency range.
***
BP10589B
Landau theory of crystallization and
the capsid structures of small icosahedral viruses
Viruses enclose their genetic material in a protective
protein coat called a capsid. Inside the infected cell
coat proteins self-assemble into a rigid spherical
shell with the symmetry of a regular icosahedron.
Since nearly fifty years virologists analyze protein
positions in icosahedral capsid structures using a
simple geometrical model by Caspar and Klug, which
imposes drastic limitations on the number and types of
possible structures. Recent advances in
cryo-electronic microscopy have evidenced however a
whole series of examples violating these rules. In the
present work we developed a model which describes in a
uniform way both the structures satisfying Caspar-Klug
rules and those violating them. For that aim we
generalized Landau theory of phase transitions, a
powerful tool which has been used by the physicists to
understand many problems of condensed matter physics,
to explain the protein self-assembly in icosahedral
viral shells. We established the method which
calculates the distribution of proteins in capsids and
clarifies their arrangement in the structures
violating old rules. An important influence of the
protein distribution in a capsid on the virus capacity
to infect the cell is illustrated.
***
LH11704B
Random medium may help in secure transmission of signals without coding
It is commonly believed that scattering prevents log-distance propagation of waves or quantum particles through random media. In absence of dissipation the amplitude of the time-inverted wave increases towards the source. We propose to explore this famous symmetry in secure communications. In one-dimensional case a wave propagating in random medium with mirror symmetry strongly decays towards the center of symmetry. Having passed the center, the wave hits the same scatterers but in the inverse order, i.e. it propagates “against time.” The amplitude of this wave increases towards the mirror image of the source, independently how far away the source and the image are. In random medium the wave decays exponentially due to the effect of Anderson localization, thus leading to strong suppression of the signal in close vicinity of the source. In this paper we show that two identical sets of resonant contours with random frequencies, being connected to the emitting and receiving ends of a transmission line, may provide secure communication without coding. The signal entering the line is suppressed to the level of noise and cannot be detected. But it is restored once it has passed through the receiving set of the contours.
***
BR10869
A pure 2D nucleation in semimetallic homoepitaxy of Bismuth
Due its fascinating electronic properties, thin films of the semimetal bismuth have enormous potential for applications in spintronic devices. As a firsthand demand, understanding of the growth processes of high quality thin films is necessary. In our present work we explain the microscopic processes and the parameters controlling the growth mechanism. Unlike most metallic systems, we observe a pure 2-dimensional nucleation even at low temperature (T = 80 K), from which we estimate a low step edge barrier in bismuth homoepitaxial growth. A threefold dendritic shape of the islands indicates a kinetic limitation of edge diffusion at such a low temperature, which can be overcome at higher temperatures (T > 300 K) changing the growth mode towards step-flow. This first study of growth mechanism on bismuth surfaces provides an excellent opportunity to the researcher for further investigation.
***
CD10135
Enhanced nuclear fusion rates within metals
Deuterium fusion reaction rates can be grossly enhanced within
metals. We established the verification of this finding under the
controlled conditions in accelerator experiments. It can be explained
by the electron screening effect which is well known in nuclear
astrophysics. It means that the repulsive force between the positively
charged nuclei is extenuated by the negative electrons in the
surrounding of the colliding nuclei thus lowering the Coulomb barrier
for the fusion. The dense electron gas in a metal lattice is more
effective than the electrons in a hydrogen molecule or a hot
solar-like plasma. Subsequently, also other groups made similar
experiments giving reason for a theoretical description attempt by a
model for stellar plasmas known as the Debye-Hückel model. Despite its
improperness for the frozen Fermi electron gas in the metal this model
was used to predict a method to remove nuclear waste by implantation
into metals at cryogenic temperatures. The possibly very high
movability of hydrogen in metals and target contaminations make
screening experiments very difficult and error-prone. In the paper we
present new experimental results, point out experimental pitfalls,
summarize our previous results and theoretical approaches including
extensive citations. We clearly showed that the Debye-Hückel model is
not appropriate for the description of the electron screening in
metals both for experimental and theoretical reasons. The
exponential-like enhancement of nuclear reaction rates in metallic
environments can make it possible to observe nuclear reactions between
charged particles even at room temperature.
***
LP11611
Who knew it would take nearly a century to create the Bohr atom?
The first successful model of the hydrogen atom was proposed by Danish
physicist Niels Bohr almost a century ago and comprised an electron in
classical circular "planet-like" orbit about the nucleus. With the
advent of quantum mechanics it was realized that the position of an
electron could not be precisely specified but rather it must be viewed
as being distributed within the atom. However, for highly excited
systems this microscopic quantum world should undergo a transition into
the macroscopic classical world. We have taken advantage of this to
produce the closest analog yet achieved to the Bohr model of the atom.
We manipulate atoms in highly excited Rydberg states using a
carefully-tailored series of short electric field pulses. Such Rydberg
atoms are the true giants of the atomic world having diameters
approaching micrometers and, if opaque, would be visible to the naked
eye. Starting with laser-excited quasi-one-dimensional Rydberg atoms we
have been able using electric field pulses to transfer the electron from
its initial highly elliptical orbit into a near circular orbit while at
the same time localizing the electron within this orbit. Measurements
show that the electron remains localized for several orbits and behaves
much as a classical particle. This creation of the Bohr atom illustrates
the power of atomic engineering using pulsed electric fields and has
potential applications in studies of classical and quantum chaos, of
information storage and processing in atoms, and of ultrafast
laser-matter interactions.
***
BR10658
A CASE OF KINETIC ARREST OF THE STRUCTURAL TRANSITION IN SHAPE MEMORY ALLOY
Magnetic shape memory materials are some ferromagnetic alloys in which,
large shape deformation is possible by an external magnetic field. The key
to their functional behavior is a structural transition called martensitic
transformation. We have studied one such alloy made up of Nickel,
Manganese and Tin. An interesting observation from our electrical
resistance measurement is that, on cooling the sample through the
martensitic transformation temperature in presence of an external magnetic
field, a fraction of the high temperature phase continues to persist down
to the lowest temperature of measurement. This is an example of kinetic
arrest of the high temperature phase by a magnetic field across a first
order phase transition such as martensitic transformation. The arrested
state was found to show very unusual metastable behavior along with a
tendency to transform into the stable low temperature phase. Surprisingly,
a close resemblance of this phenomenon is observed with the behavior of
some very different magnetic materials known as manganites. This scenario
is expressed in terms of a coupling between the magnetization and the
elastic strain, which produces an under-cooled state in materials with
strong magneto-structural correlations, such as manganites or the present
shape memory alloy.
***

LE11243B
Quantum dots squeezed into resonance
We demonstrate that local stress is a promising tool to apply energy shifts
to individual close-by semiconductor quantum dots in a deterministic
fashion. Semiconductor quantum dots lie at the heart of many exciting
devices and physical concepts, e.g. single photon sources, qubits, entangled
photons. A key task for almost all applications envisioned is a
deterministic control over the emission energy of individual quantum dots.
In our work we consider two quantum dots which are embedded into the wall of
a flexible micro tube optical ring resonator. Our calculations predict that
upon local deformation of the ring resonator reversible spectral shifts into
the red and blue of several tens of meV can be achieved (see schematic
attached). Depending on the relative position and magnitude of the applied
force the two quantum dots can be tuned into mutual resonance and into
resonance with the optical mode. These findings are experimentally
substantiated for In(Ga)As quantum dots with low density embedded in the
wall of a rolled-up micro tube ring resonator.



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