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Das am 01.01.2002 in Kraft getretene Gesetz zur Regelung von öffentlichen Angeboten zum Erwerb von Wertpapieren und von Unternehmensübernahmen (WpÜG) beschränkt sich - anders als noch der Diskussionsentwurf des WpÜG - nicht auf die Regelung von öffentlichen Angeboten zum Erwerb von Wertpapieren, die auf den Erwerb der Kontrolle an einer Zielgesellschaft gerichtet sind oder eine bereits bestehende Kontrollmehrheit voraussetzen, sondern trifft darüber hinaus mit den §§ 10 - 28 WpÜG Bestimmungen für jegliche öffentlichen Angebote zum Erwerb von Wertpapieren. Die naheliegende Frage, ob hierzu auch öffentliche Angebote zum Rückerwerb eigener Aktien, namentlich aufgrund Hauptversammlungsermächtigung gemäß § 71 Abs. 1 Nr. 8 S. 1 AktG, rechnen, lässt das Gesetz unbeantwortet. Erste Stellungnahmen in der Literatur gehen davon aus, daß das WpÜG auch auf solche self tender offers unmittelbar Anwendung finde, einzelne nicht passende Bestimmungen der §§ 10 - 28 WpÜG allerdings teleologisch zu reduzieren seien. Die Verfasser widersprechen der These einer unmittelbaren Anwendbarkeit des WpÜG auf öffentliche Angebote zum Rückerwerb eigener Aktien und befassen sich sodann mit der Frage, ob einzelne Vorschriften des WpÜG auf self tender offers analoge Anwendung finden.
Am 26.02.2002 hat die von der Bundesministerin der Justiz auf Empfehlung der Regierungskommission Corporate Governance eingesetzte Kodex-Kommission den Deutschen Corporate Governance Kodex (im folgenden: DCG-Kodex/Kodex) vorgelegt. Mit Inkrafttreten des Transparenz- und Publizitätsgesetzes4, voraussichtlich im August 2002, werden Vorstand und Aufsichtsrat börsennotierter Aktiengesellschaften künftig jährlich zu erklären haben, ob sie den Empfehlungen des Kodex folgen, und, soweit dies nicht der Fall ist, Abweichungen offen zu legen haben. Im folgenden ist zunächst das Kodex-Konzept, das dem angelsächsischen Rechtskreis entstammt, zu erläutern und die mit dem DCG-Kodex verfolgte Zielsetzung vorzustellen (dazu B.). Dem schließt sich ein Überblick über Regelungstechnik und Inhalt des DCG-Kodex sowie dessen gesetzliche „Flankierung“ durch das TransPuG an (dazu C.). Sodann werden die Entsprechens-Erklärung (dazu D.) sowie Haftungsfragen im Zusammenhang mit dem DCG-Kodex (dazu E.) behandelt.
Ratios of hadronic abundances are analyzed for pp and nucleus-nucleus collisions at sqrt(s)=20 GeV using the microscopic transport model UrQMD. Secondary interactions significantly change the primordial hadronic cocktail of the system. A comparison to data shows a strong dependence on rapidity. Without assuming thermal and chemical equilibrium, predicted hadron yields and ratios agree with many of the data, the few observed discrepancies are discussed.
Quantum Molecular Dynamics (QMD) calculations of central collisions between heavy nuclei are used to study fragment production and the creation of collective flow. It is shown that the final phase space distributions are compatible with the expectations from a thermally equilibrated source, which in addition exhibits a collective transverse expansion. However, the microscopic analyses of the transient states in the intermediate reaction stages show that the event shapes are more complex and that equilibrium is reached only in very special cases but not in event samples which cover a wide range of impact parameters as it is the case in experiments. The basic features of a new molecular dynamics model (UQMD) for heavy ion collisions from the Fermi energy regime up to the highest presently available energies are outlined.
The equilibration of hot and dense nuclear matter produced in the central cell of central Au+Au collisions at RHIC (sqrt s = 200 A GeV) energies is studied within a microscopic transport model. The pressure in the cell becomes isotropic at t approx 5 fm/c after beginning of the collision. Within the next 15 fm/c the expansion of matter in the cell proceeds almost isentropically with the entropy per baryon ratio S/A approx 150, and the equation of state in the (P,epsilon) plane has a very simple form, P=0.15 epsilon. Comparison with the statistical model of an ideal hadron gas indicates that the time t approx 20 fm/c may be too short to reach the fully equilibrated state. Particularly, the creation of long-lived resonance-rich matter in the cell decelerates the relaxation to chemical equilibrium. This resonance-abundant state can be detected experimentally after the thermal freeze-out of particles.
Equilibrium properties of infinite relativistic hadron matter are investigated using the Ultrarelativistic Quantum Molecular Dynamics (UrQMD) model. The simulations are performed in a box with periodic boundary conditions. Equilibration times depend critically on energy and baryon densities. Energy spectra of various hadronic species are shown to be isotropic and consistent with a single temperature in equilibrium. The variation of energy density versus temperature shows a Hagedorn-like behavior with a limiting temperature of 130 +/- 10 MeV. Comparison of abundances of different particle species to ideal hadron gas model predictions show good agreement only if detailed balance is implemented for all channels. At low energy densities, high mass resonances are not relevant; however, their importance raises with increasing energy density. The relevance of these different conceptual frameworks for any interpretation of experimental data is questioned.
The hypothesis of local equilibrium (LE) in relativistic heavy ion collisions at energies from AGS to RHIC is checked in the microscopic transport model. We find that kinetic, thermal, and chemical equilibration of the expanding hadronic matter is nearly reached in central collisions at AGS energy for t >_ fm/c in a central cell. At these times the equation of state may be approximated by a simple dependence P ~= (0.12-0.15) epsilon. Increasing deviations of the yields and the energy spectra of hadrons from statistical model values are observed for increasing bombarding energies. The origin of these deviations is traced to the irreversible multiparticle decays of strings and many-body (N >_ 3) decays of resonances. The violations of LE indicate that the matter in the cell reaches a steady state instead of idealized equilibrium. The entropy density in the cell is only about 6% smaller than that of the equilibrium state.
Abstract: Local thermal and chemical equilibration is studied for central AqA collisions at 10.7 160 AGeV in the Ultrarelativis- . tic Quantum Molecular Dynamics model UrQMD . The UrQMD model exhibits strong deviations from local equilibrium at the high density hadron string phase formed during the early stage of the collision. Equilibration of the hadron resonance matter is established in the central cell of volume Vs125 fm3 at later stages, tG10 fmrc, of the resulting quasi-isentropic expansion. The thermodynamical functions in the cell and their time evolution are presented. Deviations of the UrQMD quasi-equilibrium state from the statistical mechanics equilibrium are found. They increase with energy per baryon and lead to a strong enhancement of the pion number density as compared to statistical mechanics estimates at SPS energies. PACS: 25.75.-q; 24.10.Lx; 24.10.Pa; 64.30.qt
We study the thermodynamic properties of infinite nuclear matter with the Ultrarelativistic Quantum Molecular Dynamics (URQMD), a semiclassical transport model, running in a box with periodic boundary conditions. It appears that the energy density rises faster than T4 at high temperatures of T approx. 200 - 300 MeV. This indicates an increase in the number of degrees of freedom. Moreover, We have calculated direct photon production in Pb+Pb collisions at 160 GeV/u within this model. The direct photon slope from the microscopic calculation equals that from a hydrodynamical calculation without a phase transition in the equation of state of the photon source.