Vibrational-state populations and velocity distributions of H, , HD, and D, desorbing from Pd( 100) are measured with rotational state selectivity over a wide temperature range from T, = 325 to 825 K. At all surface temperatures the vibrational populations, increasing exponentially with T,, are found to be significantly higher than those expected for thermally equilibrated molecules. The slopes of Boltzmann plots are considerably lower than expected for a thermal excitation mechanism of the vibrational states at the corresponding gas-phase energies. They also show a non-trivial isotope effect. The velocity distributions from clean Pd(100) are found to be Maxwell-Boltzmann-like. The translational energies of H, molecules are accommodated at the surface temperatures, whereas those of D, are higher than kT, by ca. 10-30 meV. Both the vibrational excitation and the isotope effect in translation can be understood with a quantum-mechanical model calculation on a two-dimensional potential-energy surface. The vibrational-state selective angular distributions for desorption from Cu( 100) display a different behaviour for ground and excited states. The distributions for the vibrationally excited states are broader than that of ground-state molecules. They also show an isotope effect.
Der Wasserhaushalt dieses Stagnogleys ist bestimmt durch das perhumide und kühle Klima, die Verdichtung des Unterbodens und den massigen anstehenden Granit sowie durch die Lage am flachen Unterhang des Bärhaldekammes. Da die Wegfuhr des Sickerwassers gehemmt ist, tritt ein permanenter Hangwasserspiegel in ca. 55 cm Tiefe auf. Hang‐ und Sickerwassermenge verhalten sich wie 150:1. Trotz der hohen Zufuhren mit dem Hangwasser aus dem oberhalb gelegenen Podsolgebiet treten bei den meisten Hauptelementen große Verluste auf. Bei anderen Elementen (Al, Be, Si) werden Verluste des Oberbodens durch Zufuhren mit dem Hangwasser im Unterboden ausgeglichen oder übertroffen. Einzelne Spurenelemente (Pb, Zn) wurden von jeher akkumuliert, andere erst seit dem Anstieg der Immissionen (Cd, Co, Cu). Bei allen Elementen übertrifft der laterale den vertikalen Elementtransport um das 30‐ bis 400‐fache.
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