Hasard et destin dans le Anton Reiser de Karl Philipp Moritz

International audienceThe distinction between literary chance and chance as experience (E. Köhler) allows the originality of Moritz's autobiographical novel to be disengaged. This study of the motif of chance in book II ofAnton Reiser shows the establishment of a narrative method characterized by repressing the literary treatment of chance and maintaining of chance as a category of lived experience. In this text, the fortunate and unfortunate chances do not found the literary necessity of an exemplary destiny, but are the occasion for throwing light on the double determination, exterior and interior, that affects the character's existence, an existence that is experienced under the sign of a radical contingency. It is in this first obscurity that psychological analysis operates, not to establish the horizon of Providence, but to disengage the general lessons of an existence, and to give to its hero, at this moment, the consistency of a novelistic character.La distinction entre les deux catégories du « hasard vécu » (erlebter Zufall) et du « hasard littéraire » (literarischer Zufall), empruntée à Erich Köhler, permet d'aborder l'étude du roman autobiographique de Karl Philipp Moritz, Anton Reiser, en faisant ressortir l'ambivalence d'un projet "romanesque" en un sens nouveau. On montre ici comment le recul de la figuration du hasard littéraire au profit de la figuration du hasard vécu exprime la remise en cause du roman traditionnel et la recherche de nouvelles formes permettant de saisir et de donner forme à la consistance de la vie intérieure

Time-resolved photoemission of correlated electrons driven out of equilibrium

We describe the temporal evolution of the time-resolved photoemission response of the spinless Falicov-Kimball model driven out of equilibrium by strong applied fields. The model is one of the few possessing a metal-insulator transition and admitting an exact solution in the time domain. The nonequilibrium dynamics, evaluated using an extension of dynamical mean-field theory, show how the driven system differs from two common viewpoints - a quasiequilibrium system at an elevated effective temperature (the "hot" electron model) or a rapid interaction quench ("melting" of the Mott gap) - due to the rearrangement of electronic states and redistribution of spectral weight. The results demonstrate the inherent trade-off between energy and time resolution accompanying the finite width probe pulses, characteristic of those employed in pump-probe time-domain experiments, which can be used to focus attention on different aspects of the dynamics near the transition.Comment: Original: 5 pages, 3 figures; Replaced: updated text and figures, 5 pages, 4 figure

Coverage-dependent adsorption sites for K/Cu(001) and Cs/Cu(001) determined by surface X-ray diffraction

Surface X-ray diffraction has been used to analyze in situ the room-temperature adsorption behaviour and the structure of K and Cs on Cu(100) at submonolayer coverages. Adsorption of K takes place in fourfold hollow sites up to coverages of about 0.25 monolayers (ML), where 1 ML corresponds to 1.53 × 1015 atoms/cm2. At higher coverages the formation of a quasi-hexagonal incommensurate adlayer is observed. In contrast, for Cs adsorption we observe from the very beginning the formation of the quasi-hexagonal structure up to the completion of the adlayer at about 0.30 ML. For K adsorption in the hollow sites we determine an adsorption height, d = 2.25(15) Å, corresponding to an effective K radius of reff = 1.6(1) Å close to the ionic radius of 1.33 Å. We do not observe a change in the effective radius as a function of coverage. For the quasi-hexagonal Cs structure we find an (average) adsorption height d = 2.94 Å corresponding to an effective radius of reff = 2.18 and 1.93 Å, for the limiting ca hollow- and bridge-site adsorption, respectively. The analysis of the superlattice reflections corresponding to the quasi-hexagonal incommensurate structures indicated that the K adlayer is strongly modulated. The first Fourier component of the substrate-induced modulation was determined to u01 = 1.29(3) Å. In contrast, for Cs/Cu(001) static modulation is much less important (u01 0.2 Å). Variation of the Cs adlayer density by changing the substrate temperature allows continuous expansion and contraction of the adsorbate unit cell. No commensurate-incommensurate transition has been observed