303 research outputs found
Faraday-Talbot Effect from a Circular Array of Pillars
When an oil bath is vertically oscillating with an acceleration above some critical value, known as the Faraday threshold, the bath surface becomes unstable and nonlinear standing wave patterns emerge. One phenomenon that has been observed above the Faraday threshold is the formation of Faraday-Talbot carpets, resulting from near-field diffraction. The optical Talbot effect occurs when a monochromatic wave passes through a diffraction grating. In the near-field, the formation of self- images is observed at integer multiples of what is known as the Talbot length. These two-dimensional patterns have various applications including X-ray imaging and atom and particle trapping. Two- dimensional Faraday-Talbot wave patterns have been observed in an oil bath oscillating above the Faraday threshold containing a row of evenly spaced, protruding pillars. These pillars generate sloshing waves which serve as active sources of monochromatic Faraday waves, the interference of which generates the Faraday-Talbot wave patterns. These patterns were observed to trap bouncing and walking droplets at the location of the pillar images. As an extension of the two-dimensional linear Faraday-Talbot effect, we present novel stable and transient Faraday-Talbot carpets created from a circular array of evenly spaced pillars. An understanding of the formation of stable Faraday- Talbot carpets can act as an analogy to atom and particle trapping and may provide insights into particle trapping mechanisms
Frustrated three-leg spin tubes: from spin 1/2 with chirality to spin 3/2
Motivated by the recent discovery of the spin tube
[(CuCltachH)Cl]Cl, we investigate the properties of a frustrated
three-leg spin tube with antiferromagnetic intra-ring and inter-ring couplings.
We pay special attention to the evolution of the properties from weak to strong
inter-ring coupling and show on the basis of extensive density matrix
renormalization group and exact diagonalization calculations that the system
undergoes a first-order phase transition between a dimerized gapped phase at
weak coupling that can be described by the usual spin-chirality model and a
gapless critical phase at strong coupling that can be described by an effective
spin-3/2 model. We also show that there is a magnetization plateau at 1/3 in
the gapped phase and slightly beyond. The implications for
[(CuCltachH)Cl]Cl are discussed, with the conclusion that this
system behaves essentially as a spin-3/2 chain.Comment: 8 pages, 9 figures, revised versio
Planar Laser Induced Fluorescence Mapping of a Carbon Laser Produced Plasma
We present measurements of ion velocity distribution profiles obtained by
laser induced fluorescence (LIF) on an explosive laser produced plasma (LPP).
The spatio-temporal evolution of the resulting carbon ion velocity distribution
was mapped by scanning through the Doppler-shifted absorption wavelengths using
a tunable, diode-pumped laser. The acquisition of this data was facilitated by
the high repetition rate capability of the ablation laser (1 Hz) which allowed
the accumulation of thousand of laser shots in short experimental times. By
varying the intensity of the LIF beam, we were able to explore the effects of
fluorescence power against laser irradiance in the context of evaluating the
saturation versus the non-saturation regime. The small beam size of the LIF
beam led to high spatial resolution of the measurement compared to other ion
velocity distribution measurement techniques, while the fast-gated operation
mode of the camera detector enabled the measurement of the relevant electron
transitions
Direct measurement of high-lying vibrational repumping transitions for molecular laser cooling
Molecular laser cooling and trapping requires addressing all spontaneous
decays to excited vibrational states that occur at the level, which is accomplished by driving repumping transitions out of
these states. However, the transitions must first be identified
spectroscopically at high-resolution. A typical approach is to prepare
molecules in excited vibrational states via optical cycling and pumping, which
requires multiple high-power lasers. Here, we demonstrate a general method to
perform this spectroscopy without the need for optical cycling. We produce
molecules in excited vibrational states by using optically-driven chemical
reactions in a cryogenic buffer gas cell, and implement frequency-modulated
absorption to perform direct, sensitive, high-resolution spectroscopy. We
demonstrate this technique by measuring the spectrum of the
band in YbOH.
We identify the specific vibrational repump transitions needed for photon
cycling, and combine our data with previous measurements of the
band to determine all
of the relevant spectral constants of the state.
This technique achieves high signal-to-noise, can be further improved to
measure increasingly high-lying vibrational states, and is applicable to other
molecular species favorable for laser cooling.Comment: 14 pages, 5 figure
Statistics of Heat Transfer in Mesoscopic Circuits
A method to calculate the statistics of energy exchange between quantum
systems is presented. The generating function of this statistics is expressed
through a Keldysh path integral. The method is first applied to the problem of
heat dissipation from a biased mesoscopic conductor into the adjacent
reservoirs. We then consider energy dissipation in an electrical circuit around
a mesoscopic conductor. We derive the conditions under which measurements of
the fluctuations of heat dissipation can be used to investigate higher order
cumulants of the charge counting statistics of a mesoscopic conductor.Comment: 9 pages, 6 figure
A pseudointegrable Andreev billiard
A circular Andreev billiard in a uniform magnetic field is studied. It is
demonstrated that the classical dynamics is pseudointegrable in the same sense
as for rational polygonal billiards. The relation to a specific polygon, the
asymmetric barrier billiard, is discussed. Numerical evidence is presented
indicating that the Poincare map is typically weak mixing on the invariant
sets. This link between these different classes of dynamical systems throws
some light on the proximity effect in chaotic Andreev billiards.Comment: 5 pages, 5 figures, to appear in PR
Stub model for dephasing in a quantum dot
As an alternative to Buttiker's dephasing lead model, we examine a dephasing
stub. Both models are phenomenological ways to introduce decoherence in chaotic
scattering by a quantum dot. The difference is that the dephasing lead opens up
the quantum dot by connecting it to an electron reservoir, while the dephasing
stub is closed at one end. Voltage fluctuations in the stub take over the
dephasing role from the reservoir. Because the quantum dot with dephasing lead
is an open system, only expectation values of the current can be forced to
vanish at low frequencies, while the outcome of an individual measurement is
not so constrained. The quantum dot with dephasing stub, in contrast, remains a
closed system with a vanishing low-frequency current at each and every
measurement. This difference is a crucial one in the context of quantum
algorithms, which are based on the outcome of individual measurements rather
than on expectation values. We demonstrate that the dephasing stub model has a
parameter range in which the voltage fluctuations are sufficiently strong to
suppress quantum interference effects, while still being sufficiently weak that
classical current fluctuations can be neglected relative to the nonequilibrium
shot noise.Comment: 8 pages with 1 figure; contribution for the special issue of J.Phys.A
on "Trends in Quantum Chaotic Scattering
Stochastic Path Integral Formulation of Full Counting Statistics
We derive a stochastic path integral representation of counting statistics in
semi-classical systems. The formalism is introduced on the simple case of a
single chaotic cavity with two quantum point contacts, and then further
generalized to find the propagator for charge distributions with an arbitrary
number of counting fields and generalized charges. The counting statistics is
given by the saddle point approximation to the path integral, and fluctuations
around the saddle point are suppressed in the semi-classical approximation. We
use this approach to derive the current cumulants of a chaotic cavity in the
hot-electron regime.Comment: 4 pages, 1 eps figure, REVTe
Aspects of metallic low-temperature transport in Mott-insulator/ band-insulator superlattices: optical conductivity and thermoelectricity
We investigate the low-temperature electrical and thermal transport
properties in atomically precise metallic heterostructures involving
strongly-correlated electron systems. The model of the Mott-insulator/
band-insulator superlattice was discussed in the framework of the slave-boson
mean-field approximation and transport quantities were derived by use of the
Boltzmann transport equation in the relaxation-time approximation. The results
for the optical conductivity are in good agreement with recently published
experimental data on (LaTiO/(SrTiO superlattices and allow us to
estimate the values of key parameters of the model. Furthermore, predictions
for the thermoelectric response were made and the dependence of the Seebeck
coefficient on model parameters was studied in detail. The width of the
Mott-insulating material was identified as the most relevant parameter, in
particular, this parameter provides a way to optimize the thermoelectric power
factor at low temperatures
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