88 research outputs found
A mapping approach for configuration management tools to close the gap between two worlds and to regain trust: Or how to convert from docker to legacy tools (and vice versa)
In this paper we present the tool 'DockerConverter', an approach and a software to map a Docker configuration to various matured systems and also to reverse engineer any available Docker image in order to increase the confidence (or trust) into it. We show why a mapping approach is more promising than constructing a Domain Specific Language and why we chose a Docker image instead of the Dockerfile as the source model. Our overall goal is to enable Semantic Web research projects and especially Linked Data enterprise services to be better integrated into enterprise applications and companies
Quantum Chaos in Open versus Closed Quantum Dots: Signatures of Interacting Particles
This paper reviews recent studies of mesoscopic fluctuations in transport
through ballistic quantum dots, emphasizing differences between conduction
through open dots and tunneling through nearly isolated dots. Both the open
dots and the tunnel-contacted dots show random, repeatable conductance
fluctuations with universal statistical proper-ties that are accurately
characterized by a variety of theoretical models including random matrix
theory, semiclassical methods and nonlinear sigma model calculations. We apply
these results in open dots to extract the dephasing rate of electrons within
the dot. In the tunneling regime, electron interaction dominates transport
since the tunneling of a single electron onto a small dot may be sufficiently
energetically costly (due to the small capacitance) that conduction is
suppressed altogether. How interactions combine with quantum interference are
best seen in this regime.Comment: 15 pages, 11 figures, PDF 2.1 format, to appear in "Chaos, Solitons &
Fractals
Statistical Properties of Level Widths and Conductance Peaks in a Quantum Dot
We study the statistics of level widths of a quantum dot with extended
contacts in the absence of time-reversal symmetry. The widths are determined by
the amplitude of the wavefunction averaged over the contact area. The
distribution function of level widths for a two-point contact is evaluated
exactly. The distribution resembles closely the result obtained when the
wavefunction fluctuates independently at each point, but differs from the
one-point case. Analytical calculations and numerical simulations show that the
distribution for many-point contacts has a power-law behavior at small level
widths. The exponent is given by the number of points in the lead and diverges
in the continuous limit. The distribution of level widths is used to determine
the distribution of conductance peaks in the resonance regime. At intermediate
temperatures, we find that the distribution tends to normal and fluctuations in
the height of the peaks are suppressed as the lead size is increased.Comment: 13 pages, RevTeX 3, six uuencoded postscript figures, CMT-ERM-940
Pauli principle and chaos in a magnetized disk
We present results of a detailed quantum mechanical study of a gas of
noninteracting electrons confined to a circular boundary and subject to
homogeneous dc plus ac magnetic fields , with
). We earlier found a one-particle {\it classical}
phase diagram of the (scaled) Larmor frequency
{\rm vs} that
separates regular from chaotic regimes. We also showed that the quantum
spectrum statistics changed from Poisson to Gaussian orthogonal ensembles in
the transition from classically integrable to chaotic dynamics. Here we find
that, as a function of and , there are clear
quantum signatures in the magnetic response, when going from the
single-particle classically regular to chaotic regimes. In the quasi-integrable
regime the magnetization non-monotonically oscillates between diamagnetic and
paramagnetic as a function of . We quantitatively understand this behavior
from a perturbation theory analysis. In the chaotic regime, however, we find
that the magnetization oscillates as a function of but it is {\it always}
diamagnetic. Equivalent results are also presented for the orbital currents. We
also find that the time-averaged energy grows like in the
quasi-integrable regime but changes to a linear dependence in the chaotic
regime. In contrast, the results with Bose statistics are akin to the
single-particle case and thus different from the fermionic case. We also give
an estimate of possible experimental parameters were our results may be seen in
semiconductor quantum dot billiards.Comment: 22 pages, 7 GIF figures, Phys. Rev. E. (1999
Universal Parametric Correlations of Conductance Peaks in Quantum Dots
We compute the parametric correlation function of the conductance peaks in
chaotic and weakly disordered quantum dots in the Coulomb blockade regime and
demonstrate its universality upon an appropriate scaling of the parameter. For
a symmetric dot we show that this correlation function is affected by breaking
time-reversal symmetry but is independent of the details of the channels in the
external leads. We derive a new scaling which depends on the eigenfunctions
alone and can be extracted directly from the conductance peak heights. Our
results are in excellent agreement with model simulations of a disordered
quantum dot.Comment: 12 pages, RevTex, 2 Postscript figure
Magnetic-field dependence of energy levels in ultrasmall metal grains
We present a theory of mesoscopic fluctuations of g tensors and avoided
crossing energies in a small metal grain. The model, based on random matrix
theory, contains both the orbital and spin contributions to the g tensor. The
two contributions can be experimentally separated for weak spin-orbit coupling
while they merge in the strong coupling limit. For intermediate coupling,
substantial correlations are found between g factors of neighboring levels.Comment: 9 pages, 5 figure
Defining and controlling double quantum dots in single-walled carbon nanotubes
We report the experimental realization of double quantum dots in
single-walled carbon nanotubes. The device consists of a nanotube with source
and drain contact, and three additional top-gate electrodes in between. We show
that, by energizing these top-gates, it is possible to locally gate a nanotube,
to create a barrier, or to tune the chemical potential of a part of the
nanotube. At low temperatures we find (for three different devices) that in
certain ranges of top-gate voltages our device acts as a double quantum dot,
evidenced by the typical honeycomb charge stability pattern.Comment: 9 pages, 3 figure
Research-Data Management Planning in the German Mathematical Community
In this paper we discuss the notion of research data for the field of
mathematics and report on the status quo of research-data management and
planning. A number of decentralized approaches are presented and compared to
needs and challenges faced in three use cases from different mathematical
subdisciplines. We highlight the importance of tailoring research-data
management plans to mathematicians' research processes and discuss their usage
all along the data life cycle
One-dimensional metallic behavior of the stripe phase in LaSrCuO
Using an exact diagonalization method within the dynamical mean-field theory
we study stripe phases in the two-dimensional Hubbard model. We find a
crossover at doping from diagonal stripes to vertical
site-centered stripes with populated domain walls, stable in a broad range of
doping, . The calculated chemical potential shift and the doping dependence of the magnetic incommensurability are in
quantitative agreement with the experimental results for doped
LaSrCuO. The electronic structure shows one-dimensional
metallic behavior along the domain walls, and explains the suppression of
spectral weight along the Brillouin zone diagonal.Comment: 4 pages, 4 figure
Universal Correlations of Coulomb Blockade Conductance Peaks and the Rotation Scaling in Quantum Dots
We show that the parametric correlations of the conductance peak amplitudes
of a chaotic or weakly disordered quantum dot in the Coulomb blockade regime
become universal upon an appropriate scaling of the parameter. We compute the
universal forms of this correlator for both cases of conserved and broken time
reversal symmetry. For a symmetric dot the correlator is independent of the
details in each lead such as the number of channels and their correlation. We
derive a new scaling, which we call the rotation scaling, that can be computed
directly from the dot's eigenfunction rotation rate or alternatively from the
conductance peak heights, and therefore does not require knowledge of the
spectrum of the dot. The relation of the rotation scaling to the level velocity
scaling is discussed. The exact analytic form of the conductance peak
correlator is derived at short distances. We also calculate the universal
distributions of the average level width velocity for various values of the
scaled parameter. The universality is illustrated in an Anderson model of a
disordered dot.Comment: 35 pages, RevTex, 6 Postscript figure
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