Articles
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06/25/2024--
03/19/2024
Well-posedness of the stochastic thin-film equation with an interface potential
We consider strictly positive solutions to a class of fourth-order
conservative quasilinear SPDEs on the $d$-dimensional torus modeled after the
stochastic thin-film equation. We prove local Lipschitz estimates in Bessel
potential spaces under minimal assumptions on the parameters and corresponding
stochastic maximal $L^p$-regularity estimates for thin-film type operators with
measurable in-time coefficients. As a result, we deduce local well-posedness of
the stochastic thin-film equation as well as blow-up criteria and instantaneous
regularization for the solution. In dimension one, we additionally close
$\alpha$-entropy estimates and subsequently an energy estimate for the
stochastic thin-film equation with an interface potential so that global
well-posedness follows. We allow for a wide range of mobility functions
including the power laws $u^n$ for $n\in [0,6)$ as long as the interface
potential is sufficiently repulsive.
Antonio Agresti
Max Sauerbrey
05/08/1998--
05/08/1998
Probing Black-Hole Physics in the Laboratory Using High Intensity Femtosecond Lasers
It is shown how laboratory experiments performed with high intensity
femtosecond lasers can probe the physics of black holes in the near-horizon
regime. The acceleration generated by the high intensity laser ranging from
$10^{13}$g to more than $10^{18}$g is identified with the gravitational
acceleration at stretched horizons. In the black-hole's asymptotic region, the
stretched-horizon-reflected light shows a measurable universal phase
acceleration of $c^4/4GM$.
PACS numbers: 04.70.Bw, 97.60.Lf, 52.40.Nk, 52.50.Jm
G. Schäfer
R. Sauerbrey
01/10/2006--
01/10/2006
On the Observation of Vacuum Birefringence
We suggest an experiment to observe vacuum birefringence induced by intense
laser fields. A high-intensity laser pulse is focused to ultra-relativistic
intensity and polarizes the vacuum which then acts like a birefringent medium.
The latter is probed by a linearly polarized x-ray pulse. We calculate the
resulting ellipticity signal within strong-field QED assuming Gaussian beams.
The laser technology required for detecting the signal will be available within
the next three years.
T. Heinzl
B. Liesfeld
K. -U. Amthor
H. Schwoerer
R. Sauerbrey
A. Wipf
05/24/2019--
05/24/2019
A high-gain Quantum free-electron laser: emergence & exponential gain
We derive an effective Dicke model in momentum space to describe collective
effects in the quantum regime of a free-electron laser (FEL). The resulting
exponential gain from a single passage of electrons allows the operation of a
Quantum FEL in the high-gain mode and avoids the experimental challenges of an
X-ray FEL oscillator. Moreover, we study the intensity fluctuations of the
emitted radiation which turn out to be super-Poissonian.
Peter Kling
Enno Giese
C. Moritz Carmesin
Roland Sauerbrey
Wolfgang P. Schleich
03/24/2021--
03/24/2021
High-gain quantum free-electron laser: long-time dynamics and requirements
We solve the long-time dynamics of a high-gain free-electron laser in the
quantum regime. In this regime each electron emits at most one photon on
average, independently of the initial field. In contrast, the variance of the
photon statistics shows a qualitatively different behavior for different
initial states of the field. We find that the realization of a seeded Quantum
FEL is more feasible than self-amplified spontaneous emission.
Peter Kling
Enno Giese
C. Moritz Carmesin
Roland Sauerbrey
Wolfgang P. Schleich
05/17/2023--
05/17/2023
Frequency perturbation integral for piezoelectric quartz crystal microbalances based on scalar differential equations
We study frequency shifts in a piezoelectric quartz resonator induced by a
surface mass layer for sensor applications. The scalar differential equations
for thickness-shear modes in a quartz plate are used. A first-order
perturbation analysis is performed. The frequency shift is obtained and is
expressed by a perturbation integral. It produces the well-known Sauerbrey
equation for mass sensitivity in the special case of a uniform mass layer. As
an application of the perturbation integral, frequency shifts due to a
nonuniform mass layer are calculated.
Jiashi Yang
07/01/2019--
07/01/2019
State-of-the-art in selection of variables and functional forms in multivariable analysis -- outstanding issues
How to select variables and identify functional forms for continuous
variables is a key concern when creating a multivariable model. Ad hoc
'traditional' approaches to variable selection have been in use for at least 50
years. Similarly, methods for determining functional forms for continuous
variables were first suggested many years ago. More recently, many alternative
approaches to address these two challenges have been proposed, but knowledge of
their properties and meaningful comparisons between them are scarce. To define
a state-of-the-art and to provide evidence-supported guidance to researchers
who have only a basic level of statistical knowledge many outstanding issues in
multivariable modelling remain. Our main aims are to identify and illustrate
such gaps in the literature and present them at a moderate technical level to
the wide community of practitioners, researchers and students of statistics. We
briefly discuss general issues in building descriptive regression models,
strategies for variable selection, different ways of choosing functional forms
for continuous variables, and methods for combining the selection of variables
and functions. We discuss two examples, taken from the medical literature, to
illustrate problems in the practice of modelling. Our overview revealed that
there is not yet enough evidence on which to base recommendations for the
selection of variables and functional forms in multivariable analysis. Such
evidence may come from comparisons between alternative methods. In particular,
we highlight seven important topics that require further investigation and make
suggestions for the direction of further research.
Willi Sauerbrei
Aris Perperoglou
Matthias Schmid
Michal Abrahamowicz
Heiko Becher
Harald Binder
Daniela Dunkler
Frank E. Harrell Jr
Patrick Royston
Georg Heinze
03/23/2020--
03/23/2020
On the Heisenberg limit for detecting vacuum birefringence
Quantum electrodynamics predicts the vacuum to behave as a non-linear medium,
including effects such as birefringence. However, for experimentally available
field strengths, this vacuum polarizability is extremely small and thus very
hard to measure. In analogy to the Heisenberg limit in quantum metrology, we
study the minimum requirements for such a detection in a given strong field
(the pump field). Using a laser pulse as the probe field, we find that its
energy must exceed a certain threshold depending on the interaction time.
However, a detection at that threshold, i.e., the Heisenberg limit, requires
highly non-linear measurement schemes - while for ordinary linear-optics
schemes, the required energy (Poisson or shot noise limit) is much larger.
Finally, we discuss several currently considered experimental scenarios from
this point of view.
N. Ahmadiniaz
T. E. Cowan
R. Sauerbrey
U. Schramm
H. -P. Schlenvoigt
R. Schützhold
05/07/2020--
05/07/2020
Load impedance of immersed layers on the quartz crystal microbalance: a comparison with colloidal suspensions of spheres
The analytical theories derived here for the acoustic load impedance measured
by a quartz crystal microbalance (QCM), due to the presence of layers of
different types (rigid, elastic and viscous) immersed in a fluid, display
generic properties, such as "vanishing mass" and positive frequency shifts,
which have been observed in QCM experiments with soft-matter systems. These
phenomena seem to contradict the well-known Sauerbrey relation at the heart of
many QCM measurements, but here we show that they arise as a natural
consequence of hydrodynamics. We compare our one-dimensional immersed plate
theory with three-dimensional simulations of rigid and flexible
sub-micron-sized suspended spheres, and with experimental results for adsorbed
micron-sized colloids which yield a "negative acoustic mass". The parallel
behaviour unveiled indicates that the QCM response is highly sensitive to
hydrodynamics, even for adsorbed colloids. Our conclusions call for a revision
of existing theories based on adhesion forces and elastic stiffness at contact,
which should in most cases include hydrodynamics.
M. Meléndez
A. Vázquez-Quesada
R. Delgado-Buscalioni
04/14/2020--
11/28/2019
Quantum and classical phase-space dynamics of a free-electron laser
In a quantum mechanical description of the free-electron laser (FEL) the
electrons jump on discrete momentum ladders, while they follow continuous
trajectories according to the classical description. In order to observe the
transition from quantum to classical dynamics, it is not sufficient that many
momentum levels are involved. Only if additionally the initial momentum spread
of the electron beam is larger than the quantum mechanical recoil, caused by
the emission and absorption of photons, the quantum dynamics in phase space
resembles the classical one. Beyond these criteria, quantum signatures of
averaged quantities like the FEL gain might be washed out.
C. Moritz Carmesin
Peter Kling
Enno Giese
Roland Sauerbrey
Wolfgang P. Schleich
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