26 resultados para Democratic theory

em Universitätsbibliothek Kassel, Universität Kassel, Germany


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Almost all Latin American countries are still marked by extreme forms of social inequality – and to an extent, this seems to be the case regardless of national differences in the economic development model or the strength of democracy and the welfare state. Recent research highlights the fact that the heterogeneous labour markets in the region are a key source of inequality. At the same time, there is a strengthening of ‘exclusive’ social policy, which is located at the fault lines of the labour market and is constantly (re-)producing market-mediated disparities. In the last three decades, this type of social policy has even enjoyed democratic legitimacy. These dynamics challenge many of the assumptions guiding social policy and democratic theory, which often attempt to account for the specificities of the region by highlighting the purported flaws of certain policies. We suggest taking a different perspective: social policy in Latin American should not be grasped as a deficient or flawed type of social policy, but as a very successful relation of political domination. ‘Relational social analysis’ locates social policy in the ‘tension zone’ constituted by the requirements of economic reproduction, demands for democratic legitimacy and the relative autonomy of the state. From this vantage point, we will make the relation of domination in question accessible for empirical research. It seems particularly useful for this purpose to examine the recent shifts in the Latin American labour markets, which have undergone numerous reforms. We will examine which mechanisms, institutions and constellations of actors block or activate the potentials of redistribution inherent in such processes of political reform. This will enable us to explore the socio-political field of forces that has been perpetuating the social inequalities in Latin America for generations.

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Bei der vorliegenden Arbeit handelt es sich um ein Vorhaben aus dem Bereich der Praxisforschung. Den Untersuchungsgegenstand bildet das Beteiligungsmodell für Kinder und Jugendliche der Stadt Kassel. Im Zentrum der Betrachtung steht dabei die Rolle der Erwachsenen im Zuge der Durchführung von Beteiligungsprojekten mit Kindern und Jugendlichen in Kassel, einer Großstadt mit rund 185.000 Einwohnern. Die Basis der Untersuchung bilden 17 Kriterien für professionelles Verhalten Erwachsener in Beteiligungsprozessen, die zunächst aus vier pädagogischen Richtungen abgeleitet werden. Es handelt sich dabei um die Ansätze folgender Pädagogen: • Janusz Korczak (1878-1942), polnischer Arzt, Literat, Pädagoge, • Kurt Löwenstein (1885-1939), Gründer und Förderer der sozialistischen Kinderfreunde-Bewegung, • Loris Malaguzzi (1920-1994), italienischer Pädagoge und „Urvater“ der Reggio-Pädagogik und • Olaf Axel Burow (geb. 1951), Begründer der Gestaltpädagogik. Das Hauptziel der Arbeit besteht in der Erarbeitung eines Kriterienkataloges für professionelles Verhalten Erwachsener in Beteiligungsprozessen mit Kindern und Jugendlichen. Nach der Einleitung, einer Beschreibung des der Arbeit zugrunde liegenden Verständnisses von Partizipation und der Darstellung angewandter Untersuchungsinstrumente werden im zweiten Teil neben einem Überblick über historische Vorläufer des Ansatzes Kinder und Jugendliche an der Gestaltung ihrer Lebenswelt zu beteiligen, allgemeine Grundlagen der Beteiligung von Kindern und Jugendlichen geliefert (rechtliche, Formen und Methoden der Beteiligung, Prüfsteine für gute Beteiligung...). Dieser einführende Teil endet mit der Entwicklung grundlegender Kriterien, die bei der Durchführung von Partizipationsprozessen mit Kindern und Jugendlichen berücksichtigt werden sollten bzw. müssen. Im dritten Teil werden die vier oben erwähnten pädagogischen Richtungen vorgestellt und interpretiert. Aus den vier Ansätzen werden zum einen 13 Kriterien für partizipative Erziehung herausgearbeitet zum anderen 17 Kriterien für professionelles Verhalten Erwachsener in Partizipationsprozessen abgeleitet. Anhand dieser Kriterien entsteht auch eine Definition für partizipative Erziehung. Im Zentrum des folgenden vierten Teiles der Arbeit steht zunächst die Beschreibung des Beteiligungsmodells der Stadt Kassel. Dabei bilden die Rolle der Kinderbeauftragten und die Tätigkeiten des Vereins Spielmobil Rote Rübe, der die Entwicklung des Beteiligungsansatzes mitbestimmt, sowie intensiv in die Durchführung der Beteiligungsprojekte involviert ist, die Schwerpunkte der Betrachtung. Nach einer ausführlichen Auseinandersetzung mit der Theorie und der Praxis der Kassler Beteiligungslandschaft werden die in Teil drei entwickelten Kriterien für professionelles Verhalten Erwachsener in Beteiligungsprozessen anhand der aktuellen Situation in der Stadt Kassel auf ihre Praxistauglichkeit hin untersucht und überarbeitet. Auch die in Teil drei verfasste Definition für Beteiligung erfährt einige geringfügige Veränderungen. In diesem Zusammenhang erfolgt auch eine Auseinandersetzung mit Veränderungsmöglichkeiten bzw. eine Beschreibung von Verbesserungsvorschlägen des projektorientierten Beteiligungsmodells der Stadt Kassel.

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This paper is an attempt to analyze bonds and their relevance within the confines of economics. They are discussed as both exogenous and endogenous variables. More specifically, the bonds of democratic politics are compared with those of non-democratic politics. It is argued that only those societies that have at their disposition certain kinds of bonds will be able to sustain democracy. It is further argued that the differential effects of democratic vs. non-democratic regimes on the respective bonds are rather weak. But then again, different kinds of democratic institutions might well have an effect on the prevalent bonds found in a society.

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The object of research presented here is Vessiot's theory of partial differential equations: for a given differential equation one constructs a distribution both tangential to the differential equation and contained within the contact distribution of the jet bundle. Then within it, one seeks n-dimensional subdistributions which are transversal to the base manifold, the integral distributions. These consist of integral elements, and these again shall be adapted so that they make a subdistribution which closes under the Lie-bracket. This then is called a flat Vessiot connection. Solutions to the differential equation may be regarded as integral manifolds of these distributions. In the first part of the thesis, I give a survey of the present state of the formal theory of partial differential equations: one regards differential equations as fibred submanifolds in a suitable jet bundle and considers formal integrability and the stronger notion of involutivity of differential equations for analyzing their solvability. An arbitrary system may (locally) be represented in reduced Cartan normal form. This leads to a natural description of its geometric symbol. The Vessiot distribution now can be split into the direct sum of the symbol and a horizontal complement (which is not unique). The n-dimensional subdistributions which close under the Lie bracket and are transversal to the base manifold are the sought tangential approximations for the solutions of the differential equation. It is now possible to show their existence by analyzing the structure equations. Vessiot's theory is now based on a rigorous foundation. Furthermore, the relation between Vessiot's approach and the crucial notions of the formal theory (like formal integrability and involutivity of differential equations) is clarified. The possible obstructions to involution of a differential equation are deduced explicitly. In the second part of the thesis it is shown that Vessiot's approach for the construction of the wanted distributions step by step succeeds if, and only if, the given system is involutive. Firstly, an existence theorem for integral distributions is proven. Then an existence theorem for flat Vessiot connections is shown. The differential-geometric structure of the basic systems is analyzed and simplified, as compared to those of other approaches, in particular the structure equations which are considered for the proofs of the existence theorems: here, they are a set of linear equations and an involutive system of differential equations. The definition of integral elements given here links Vessiot theory and the dual Cartan-Kähler theory of exterior systems. The analysis of the structure equations not only yields theoretical insight but also produces an algorithm which can be used to derive the coefficients of the vector fields, which span the integral distributions, explicitly. Therefore implementing the algorithm in the computer algebra system MuPAD now is possible.

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A microscopic theory is presented for the photoacoustic effect induced in solids by x-ray absorption. The photoacoustic effect results from the thermalization of the excited Auger electrons and photoelectrons. We explain the dependence of the photoacoustic signal S on photon energy and the proportionality to the x-ray absorption coefficient in agreement with recent experiments on Cu. Results are presented for the dependence of S on photon energy, sample thickness, and the electronic structure of the absorbing solid.

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We present a theory which permits for the first time a detailed analysis of the dependence of the absorption spectrum on atomic structure and cluster size. Thus, we determine the development of the collective excitations in small clusters and show that their broadening depends sensitively on the tomic structure, in particular at the surface. Results for Hg_n^+ clusters show that the plasmon energy is close to its jellium value in the case of spherical-like structures, but is in general between w_p/ \wurzel{3} and w_p/ \wurzel{2} for compact clusters. A particular success of our theory is the identification of the excitations contributing to the absorption peaks.

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The static and dynamical polarizabilities of the Hg-dimer are calculated by using a Hubbard Hamiltonian to describe the electronic structure. The Hamiltonian is diagonalized exactly within a subspace of second-quantized electronic states from which only multiply ionized atomic configurations have been excluded. With this approximation we can describe the most important electronic transitions including the effect of charge fluctuations. We analyze the polarizability as a function of the intraatomic Coulomb interaction which represents the repulsion between electrons. We obtain that this interaction results in strong electronic correlations in the excited states and increases the first excitation energy of the dimer by 0.8 eV in comparison to a calculation which neglects correlations, resulting in a better agreement with the experiment.

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To determine the size dependence of the bonding in divalent-metal clusters we use a many-electron Hamiltonian describing the interplay between van der Waals (vdW) and covalent interactions. Using a saddle-point slave-boson method and taking into account the size-dependent screening of charge fluctuations, we obtain for Hg_n a sharp transition from vdW to covalent bonding for increasing n. We show also, by solving the model Hamiltonian exactly, that for divalent metals vdW and covalent bonding coexist already in the dimers.

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The Kr 4s-electron photoionization cross section as a function of the exciting-photon energy in the range between 30 eV and 90 eV was calculated using the configuration interaction (CI) technique in intermediate coupling. In the calculations the 4p spin-orbital interaction and corrections due to higher orders of perturbation theory (the so-called Coulomb interaction correlational decrease) were considered. Energies of Kr II states were calculated and agree with spectroscopic data within less than 10 meV. For some of the Kr II states new assignments were suggested on the basis of the largest component among the calculated CI wavefunctions.

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Absolute cross sections for the transitions of the Kr atom into the 4s^1 and 4p^4nl states of the Kr^+ ion were measured in the 4s-electron threshold region by photon-induced fluorescence spectroscopy (PIFS). The cross sections for the transitions of the Kr atom into the 4s^1 and 4p^4nl states were also calculated, as well as the 4p^4nln'l' doubly excited states, in the frame of LS-coupling many-body technique. The cross sections of the doubly-excited atomic states were used to illustrate the pronounced contributions of the latter to the photoionization process, evident from the measurements. The comparison of theory and experiment led to conclusions about the origin of the main features observed in the experiment.

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Using the independent particle model as our basis we present a scheme to reduce the complexity and computational effort to calculate inclusive probabilities in many-electron collision system. As an example we present an application to K - K charge transfer in collisions of 2.6 MeV Ne{^9+} on Ne. We are able to give impact parameter-dependent probabilities for many-particle states which could lead to KLL-Auger electrons after collision and we compare with experimental values.

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In continuation of our previous work on the quintet transitions 1s2s2p^2 ^5 P-1s2s2p3d ^5 P^0, ^5 D^0, results on other n = 2 - n' = 3 quintet transitions for elements N, 0 and F are presented. Assignments have been established by comparison with Multi-Configuration Dirac-Fock calculations. High spectral resolution on beam-foil spectroscopy was essential for the identification of most of the lines. For some of the quintet lines decay curves were measured, and the lifetimes extracted were found to be in reasonable agreement with MCDF calculations.

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The present thesis is a contribution to the study of laser-solid interaction. Despite the numerous applications resulting from the recent use of laser technology, there is still a lack of satisfactory answers to theoretical questions regarding the mechanism leading to the structural changes induced by femtosecond lasers in materials. We provide here theoretical approaches for the description of the structural response of different solids (cerium, samarium sulfide, bismuth and germanium) to femtosecond laser excitation. Particular interest is given to the description of the effects of the laser pulse on the electronic systems and changes of the potential energy surface for the ions. Although the general approach of laser-excited solids remains the same, the potential energy surface which drives the structural changes is calculated with different theoretical models for each material. This is due to the difference of the electronic properties of the studied systems. We use the Falicov model combined with an hydrodynamic method to study photoinduced phase changes in cerium. The local density approximation (LDA) together with the Hubbard-type Hamiltonian (LDA+U) in the framework of density functional theory (DFT) is used to describe the structural properties of samarium sulfide. We parametrize the time-dependent potential energy surface (calculated using DFT+ LDA) of bismuth on which we perform quantum dynamical simulations to study the experimentally observed amplitude collapse and revival of coherent $A_{1g}$ phonons. On the basis of a time-dependent potential energy surface calculated from a non-orthogonal tight binding Hamiltonian, we perform molecular dynamics simulation to analyze the time evolution (coherent phonons, ultrafast nonthermal melting) of germanium under laser excitation. The thermodynamic equilibrium properties of germanium are also reported. With the obtained results we are able to give many clarifications and interpretations of experimental results and also make predictions.