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Atomic excitations are used to obtain information on the course of a nuclear reaction. Employing a semiclassical picture we calculate the emission of δ electrons and positrons in deep inelastic nuclear reactions for the example of U+U collisions incorporating nuclear trajectories resulting from two different nuclear friction models. The emission spectra exhibit characteristic deviations from those expected for elastic Coulomb scattering. The theoretical probabilities are compared with recent experimental data by Backe et al. A simple model is used to estimate the influence of a threebody breakup of the compound system upon atomic excitations.
Positron creation in crossed-beam collisions of high-energy, fully stripped heavy ions is investigated within the coupled-channel formalism. In comparison with fixed-target collisions of highly stripped heavy-ion projectiles positron production probabilities are enhanced by more than one order of magnitude. The increase results from the possibility to excite electrons from the negative energy continuum into all bound states. The positron spectrum is shifted towards higher energies because of the absence of electron screening. Rutherford scattering as well as nuclear collisions with time delay are investigated. We also discuss the filling of empty bound states by electrons from pair-production processes.
Der Kernbereich der Verbreitung des Cardamino trifoliae-Fagetum, als dessen Kennarten Cardamine trifolia und Dentaria enneaphyllos anzusehen sind, liegt am Nord- und Ostrand der österreichischen Alpen; die Assoziation kann bis in die Steiermark verfolgt werden und wird dann von dem Anemono trifoliae-Fagetum abgelöst. Im östlichen Oberbayern klingt das Cardamino trifoliae-Fagetum nach Westen hin aus und verarmt an Arten. Zusätzlich tritt hier als Trennart einer Vikarianten Aposeris foetida auf. Weiter nach Westen, nach der Verbreitungsgrenze von Dentaria enneaphyllos und Cardamine trifolia, folgt das für den mittleren Alpennordrand bezeichnende Lonicero alpigenae-Fagetum, hier z.T. ebenfalls in einer Vikarianten mit Aposeris foetida. Insofern gehören in Tabelle 2 bei SEIBERT die lfd. Nummern 11, 9,1, 8, 10, 2, 3, 4, 6, 7 und 12 zum Cardamino trifoliae-Fagetum, die lfd. Nummern 13, 14 und 15 zum Lonicero alpigenae-Fagetum, die lfd. Nummer 5 zum Galio-Abietetum (diese Aufnahmen wurden weder von OBERDORFER & MÜLLER 1984 noch von MÜLLER in OBERDORFER 1992 für die Beschreibung des Cardamino trifoliae-Fagetum verwendet).
Erich Oberdorfer (1905-2002)
(2003)
Am 23. September 2002 verstarb nach einem erfüllten Leben Prof. Dr. Dr. h.c. Erich Oberdorfer im Alter von 97 Jahren. Es war ihm vergönnt, im Kreise seiner Familie ruhig einzuschlafen in seinem Haus in Freiburg-St. Georgen. Er konnte noch bis kurz vor seinem Tode geistig rege die Geschicke der Pflanzensoziologie und der Taxonomie der Pflanzen verfolgen. Mit ihm verließ uns einer der letzten Universal-Pflanzensoziologen, der meisterhaft pflanzensoziologisch-pflanzengeographische und floristisch-taxonomische Erkenntnisse zu verbinden wusste.
Long-range angular correlations on the near and away side in p–Pb collisions at √sNN=5.02 TeV
(2013)
Angular correlations between charged trigger and associated particles are measured by the ALICE detector in p–Pb collisions at a nucleon–nucleon centre-of-mass energy of 5.02 TeV for transverse momentum ranges within 0.5<pT,assoc<pT,trig<4 GeV/c. The correlations are measured over two units of pseudorapidity and full azimuthal angle in different intervals of event multiplicity, and expressed as associated yield per trigger particle. Two long-range ridge-like structures, one on the near side and one on the away side, are observed when the per-trigger yield obtained in low-multiplicity events is subtracted from the one in high-multiplicity events. The excess on the near-side is qualitatively similar to that recently reported by the CMS Collaboration, while the excess on the away-side is reported for the first time. The two-ridge structure projected onto azimuthal angle is quantified with the second and third Fourier coefficients as well as by near-side and away-side yields and widths. The yields on the near side and on the away side are equal within the uncertainties for all studied event multiplicity and pT bins, and the widths show no significant evolution with event multiplicity or pT. These findings suggest that the near-side ridge is accompanied by an essentially identical away-side ridge.
We present the first wide-range measurement of the charged-particle pseudorapidity density distribution, for different centralities (the 0-5%, 5-10%, 10-20%, and 20-30% most central events) in Pb-Pb collisions at sNN−−−√=2.76 TeV at the LHC. The measurement is performed using the full coverage of the ALICE detectors, −5.0<η<5.5, and employing a special analysis technique based on collisions arising from LHC "satellite" bunches. We present the pseudorapidity density as a function of the number of participating nucleons as well as an extrapolation to the total number of produced charged particles (Nch=17165±772 for the 0-5% most central collisions). From the measured dNch/dη distribution we derive the rapidity density distribution, dNch/dy, under simple assumptions. The rapidity density distribution is found to be significantly wider than the predictions of the Landau model. We assess the validity of longitudinal scaling by comparing to lower energy results from RHIC. Finally the mechanisms of the underlying particle production are discussed based on a comparison with various theoretical models.
n this paper measurements are presented of π+, π−, K+, K−, p and p¯¯¯ production at mid-rapidity < 0.5, in Pb-Pb collisions at sNN−−−√=2.76 TeV as a function of centrality. The measurement covers the transverse momentum (pT) range from 100, 200, 300 MeV/c up to 3, 3, 4.6 GeV/c, for π, K, and p respectively. The measured pT distributions and yields are compared to expectations based on hydrodynamic, thermal and recombination models. The spectral shapes of central collisions show a stronger radial flow than measured at lower energies, which can be described in hydrodynamic models. In peripheral collisions, the pT distributions are not well reproduced by hydrodynamic models. Ratios of integrated particle yields are found to be nearly independent of centrality. The yield of protons normalized to pions is a factor ~1.5 lower than the expectation from thermal models.
In high-energy heavy-ion collisions, the correlations between the emitted particles can be used as a probe to gain insight into the charge creation mechanisms. In this article, we report the first results of such studies using the electric charge balance function in the relative pseudorapidity \Delta\eta and azimuthal angle \Delta\phi in Pb-Pb collisions at sqrt{s_{NN}} = 2.76 TeV with the ALICE detector at the Large Hadron Collider. The width of the balance function decreases with growing centrality (i.e. for more central collisions) in both projections. This centrality dependence is not reproduced by HIJING, while AMPT, a model which incorporates strings and parton rescattering, exhibits qualitative agreement with the measured correlations in \Delta\phi but fails to describe the correlations in \Delta\eta. A thermal blast wave model incorporating local charge conservation and tuned to describe the p_T spectra and v_2 measurements reported by ALICE, is used to fit the centrality dependence of the width of the balance function and to extract the average separation of balancing charges at freeze-out. The comparison of our results with measurements at lower energies reveals an ordering with sqrt{s_{NN}}: the balance functions become narrower with increasing energy for all centralities. This is consistent with the effect of larger radial flow at the LHC energies but also with the late stage creation scenario of balancing charges. However, the relative decrease of the balance function widths in \Delta\eta and \Delta\phi with centrality from the highest SPS to the LHC energy exhibits only small differences. This observation cannot be interpreted solely within the framework where the majority of the charge is produced at a later stage in the evolution of the heavy-ion collision.