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Morphologische und zytologische Untersuchungen haben eine Korrelation der Chromosomenzahlen von Bromus benekenii (2n = 28) und B. ramosus (2n = 42) mit ihren morphologischen Merkmalen ergeben. Die eindeutige Unterscheidung ist Voraussetzung für einen vegetationskundlichen, bodenkundlichen und mikroklimatischen Vergleich an Standorten in Hessen. Danach ist B. benekenii häufiger in Wäldern (Fagetalia sylvaticae), B. ramosus dagegen in Schlagfluren (Atropetalia) und mesophilen Saum-Gesellschaften (Trifolion medii) vertreten.
Beide Arten stellen während ihrer Wachstumsphasen ähnliche, relativ hohe "Ansprüche" an den Standort (z.B. Lichtverhältnisse, Wasserhaushalt, Stickstoffgehalte und pH-Werte der Böden). Die günstigen Bedingungen sind jedoch an B. benekenii-Standorten aufgrund früh einsetzender Trockenheit oder Beschattung von kürzerer Dauer als an den Standorten von B. ramosus. B. benekenii ist hieran durch eine früher abgeschlossene Entwicklung angepasst.
Die Möglichkeit einer Bastardierung ist infolge der abweichenden Blütezeiten gering.
Ergebnisse physiologischer und anatomischer Untersuchungen von Reaktionen der Arten auf Wasserstress und abgestufte Lichtintensitäten deuten daraufhin, daß B. ramosus etwas besser an höhere Lichtintensitäten und Wasserstress angepasst ist als B. benekenii. B. ramosus besitzt dadurch einen Konkurrenzvorteil.
Die durchgeführten Untersuchungen erweisen B. benekenii und B. ramosus als zwei gut geschiedene Arten. Auf Standorten mit optimalen Wuchsbedingungen ist B. ramosus in der Wettbewerbssituation überlegen und verdrängt B. benekenii auf Standorte mit verkürzter, relevanter Wachstumszeit.
Beitrag zur Kenntnis der Wasserinsektenfauna Nordwest-Hessens : 1. Köcherfliegen (Trichoptera)
(1992)
The transverse momentum and rapidity distributions of negative hadrons and participant protons have been measured for central 32S+ 32S collisions at plab=200 GeV/c per nucleon. The proton mean rapidity shift < Delta y>~1.6 and mean transverse momentum <pT>~0.6 GeV/c are much higher than in pp or peripheral AA collisions and indicate an increase in the nuclear stopping power. All pT spectra exhibit similar source temperatures. Including previous results for K0s Lambda , and Lambda -bar, we account for all important contributions to particle production.
We present the measured correlation functions for pi+ pi-, pi- pi- and pi+ pi+ pairs in central S+Ag collisions at 200 GeV per nucleon. The Gamov function, which has been traditionally used to correct the correlation functions of charged pions for the Coulomb interaction, is found to be inconsistent with all measured correlation functions. Certain problems which have been dominating the systematic uncertainty of the correlation analysis are related to this inconsistency. It is demonstrated that a new Coulomb correction method, based exclusively on the measured correlation function for pi+ pi- pairs, may solve the problem.
Elliptic flow from nuclear collisions is a hadronic observable sensitive to the early stages of system evolution. We report first results on elliptic flow of charged particles at midrapidity in Au+Au collisions at sqrt(s_NN)=130 GeV using the STAR TPC at RHIC. The elliptic flow signal, v_2, averaged over transverse momentum, reaches values of about 6% for relatively peripheral collisions and decreases for the more central collisions. This can be interpreted as the observation of a higher degree of thermalization than at lower collision energies. Pseudorapidity and transverse momentum dependence of elliptic flow are also presented.
Two-pion correlation functions in Au+Au collisions at sqrt[sNN] = 130 GeV have been measured by the STAR (solenoidal tracker at RHIC) detector. The source size extracted by fitting the correlations grows with event multiplicity and decreases with transverse momentum. Anomalously large sizes or emission durations, which have been suggested as signals of quark-gluon plasma formation and rehadronization, are not observed. The Hanbury Brown-Twiss parameters display a weak energy dependence over a broad range in sqrt[sNN].
The first measurements of light antinucleus production in Au+Au collisions at the Relativistic Heavy-Ion Collider are reported. The observed production rates for d-bar and 3He-bar are much larger than in lower energy nucleus-nucleus collisions. A coalescence model analysis of the yields indicates that there is little or no increase in the antinucleon freeze-out volume compared to collisions at CERN SPS energy. These analyses also indicate that the 3He-bar freeze-out volume is smaller than the d-bar freeze-out volume.
Elliptic flow from nuclear collisions is a hadronic observable sensitive to the early stages of system evolution. We report first results on elliptic flow of charged particles at midrapidity in Au+Au collisions at sqrt[sNN] = 130 GeV using the STAR Time Projection Chamber at the Relativistic Heavy Ion Collider. The elliptic flow signal, v2, averaged over transverse momentum, reaches values of about 6% for relatively peripheral collisions and decreases for the more central collisions. This can be interpreted as the observation of a higher degree of thermalization than at lower collision energies. Pseudorapidity and transverse momentum dependence of elliptic flow are also presented.
The minimum-bias multiplicity distribution and the transverse momentum and pseudorapidity distributions for central collisions have been measured for negative hadrons ( h-) in Au+Au interactions at sqrt[sNN] = 130 GeV. The multiplicity density at midrapidity for the 5% most central interactions is dNh-/d eta | eta = 0 = 280±1(stat)±20(syst), an increase per participant of 38% relative to pp-bar collisions at the same energy. The mean transverse momentum is 0.508±0.012 GeV/c and is larger than in central Pb+Pb collisions at lower energies. The scaling of the h- yield per participant is a strong function of pperp. The pseudorapidity distribution is almost constant within | eta |<1.
We report the first measurement of inclusive antiproton production at midrapidity in Au+Au collisions at sqrt[sNN] = 130 GeV by the STAR experiment at RHIC. The antiproton transverse mass distributions in the measured transverse momentum range of 0.25<pperp<0.95 GeV/c are found to fall less steeply for more central collisions. The extrapolated antiproton rapidity density is found to scale approximately with the negative hadron multiplicity density.