Titlebook: Jahrbuch der Preußischen Forst- und Jagdgesetzgebung und Verwaltung; Dreiundzwanzigster B Bernhard Danckelmann (Rönigl. Preuß. Oberforstmei

canonical

Bernhard Danckelmanne kinetics as the value of the binding energy is in a reasonable agreement with the theory..It is probable that biexcitons can be formed also in other substances. Some strong arguments seem to exist in the case of CdS, CdSe and also in Ge and Si. However, in these cases some important shortcomings a

机警

Bernhard Danckelmannense light beams and optical gain measurements on highly excited CuCl. We find that the reflectivity spectra are modified when a high intensity probe is used, and that this modification can be phenomenologically explained in terms of an exciton damping parameter which varies linearly with incident l

FORGO

Bernhard Danckelmanne kinetics as the value of the binding energy is in a reasonable agreement with the theory..It is probable that biexcitons can be formed also in other substances. Some strong arguments seem to exist in the case of CdS, CdSe and also in Ge and Si. However, in these cases some important shortcomings a

烧烤

Bernhard Danckelmanne kinetics as the value of the binding energy is in a reasonable agreement with the theory..It is probable that biexcitons can be formed also in other substances. Some strong arguments seem to exist in the case of CdS, CdSe and also in Ge and Si. However, in these cases some important shortcomings a

invert

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Morsel

Bernhard Danckelmanne kinetics as the value of the binding energy is in a reasonable agreement with the theory..It is probable that biexcitons can be formed also in other substances. Some strong arguments seem to exist in the case of CdS, CdSe and also in Ge and Si. However, in these cases some important shortcomings a

Facet-Joints

Bernhard Danckelmannense light beams and optical gain measurements on highly excited CuCl. We find that the reflectivity spectra are modified when a high intensity probe is used, and that this modification can be phenomenologically explained in terms of an exciton damping parameter which varies linearly with incident l

Cupping