6,943 research outputs found
Laser-induced nonsequential double ionization: kinematic constraints for the recollision-excitation-tunneling mechanism
We investigate the physical processes in which an electron, upon return to
its parent ion, promotes a second electron to an excited state, from which it
subsequently tunnels. Employing the strong-field approximation and saddle-point
methods, we perform a detailed analysis of the dynamics of the two electrons,
in terms of quantum orbits, and delimit constraints for their momentum
components parallel to the laser-field polarization. The kinetic energy of the
first electron, upon return, exhibits a cutoff slightly lower than ,
where is the ponderomotive energy, as in rescattered above-threshold
ionization (ATI). The second electron leaves the excited state in a direct
ATI-like process, with the maximal energy of . We also compute
electron-momentum distributions, whose maxima agree with our estimates and with
other methods.Comment: 13 pages, 4 figure
Stabilization not for certain and the usefulness of bounds
Stabilization is still a somewhat controversial issue concerning its very
existence and also the precise conditions for its occurrence. The key quantity
to settle these questions is the ionization probability, for which hitherto no
computational method exists which is entirely agreed upon. It is therefore very
useful to provide various consistency criteria which have to be satisfied by
this quantity, whose discussion is the main objective of this contribution. We
show how the scaling behaviour of the space leads to a symmetry in the
ionization probability, which can be exploited in the mentioned sense.
Furthermore, we discuss how upper and lower bounds may be used for the same
purpose. Rather than concentrating on particular analytical expressions we
obtained elsewhere for these bounds, we focus in our discussion on the general
principles of this method. We illustrate the precise working of this procedure,
its advantages, shortcomings and range of applicability. We show that besides
constraining possible values for the ionization probability these bounds, like
the scaling behaviour, also lead to definite statements concerning the physical
outcome. The pulse shape properties which have to be satitisfied for the
existence of asymptotical stabilization is the vanishing of the total classical
momentum transfer and the total classical displacement and not smoothly
switched on and off pulses. Alternatively we support our results by general
considerations in the Gordon-Volkov perturbation theory and explicit studies of
various pulse shapes and potentials including in particular the Coulomb- and
the delta potential.Comment: 12 pages Late
Quantum interference in laser-induced nonsequential double ionization in diatomic molecules: the role of alignment and orbital symmetry
We address the influence of the orbital symmetry and of the molecular
alignment with respect to the laser-field polarization on laser-induced
nonsequential double ionization of diatomic molecules, in the length and
velocity gauges. We work within the strong-field approximation and assume that
the second electron is dislodged by electron-impact ionization, and also
consider the classical limit of this model. We show that the electron-momentum
distributions exhibit interference maxima and minima due to the electron
emission at spatially separated centers. The interference patterns survive the
integration over the transverse momenta for a small range of alignment angles,
and are sharpest for parallel-aligned molecules. Due to the contributions of
transverse-momentum components, these patterns become less defined as the
alignment angle increases, until they disappear for perpendicular alignment.
This behavior influences the shapes and the peaks of the electron momentum
distributions.Comment: 12 pages, 7 figures; some discussions have been extended and some
figures slightly modifie
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Analytical treatment of stabilization
We present a summarizing account of a series of investigations whose central topic is to address the question whether atomic stabilization exists in an analytical way. We provide new aspects on several issues of the matter in the theoretical context when the dynamics is described by the Stark Hamiltonian. The main outcome of these studies is that the governing parameters for this phenomenon are the total classical momentum transfer and the total classical displacement. Whenever these two quantities vanish, asymptotically weak stabilization does exist. For all other situations we did not find any evidence for stabilization. We found no evidence that strong stabilization might occur. Our results agree qualitatively with the existing experimental findings
Towards multimodal affective expression:merging facial expressions and body motion into emotion
Affect recognition plays an important role in human everyday life and it is a substantial way of communication through expressions. Humans can rely on different channels of information to understand the affective messages communicated with others. Similarly, it is expected that an automatic affect recognition system should be able to analyse different types of emotion expressions. In this respect, an important issue to be addressed is the fusion of different channels of expression, taking into account the relationship and correlation across different modalities. In this work, affective facial and bodily motion expressions are addressed as channels for the communication of affect, designed as an emotion recognition system. A probabilistic approach is used to combine features from two modalities by incorporating geometric facial expression features and body motion skeleton-based features. Preliminary results show that the presented approach has potential for automatic emotion recognition and it can be used for human robot interaction
Categorical Groups, Knots and Knotted Surfaces
We define a knot invariant and a 2-knot invariant from any finite categorical
group. We calculate an explicit example for the Spun Trefoil.Comment: 40 pages, lots of figures. Second version: Added example and
discussion, clarification of the fact that the maps associated with
Reidemeister Moves are well define
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