Excited-State Equilibration and the Fluorescence-Absorption Ratio |

R.S. KnoxDepartment of Physics and Astronomy and Rochester Theory Center for Optical Sciences and Engineering, University of Rochester, Rochester, NY 14627-0171 USA |

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In any complex system at temperature T the absorption cross-section and fluorescent power at a given photon energy are connected by a simple relation if the system is in thermal equilibrium while occupying one particular electronic excited state. Although this situation is impossible in principle because of finite excited-state lifetimes, it is often approximated to the extent that the simple relation, which is expressed as a linear function of energy with slope -1/k_{B}T, holds in a variety of cases. (The usual symbols for Boltzmann's constant and absolute temperature are used.) Observed deviations are of two principal kinds: a slope characteristic of some temperature T* other than ambient, and departures from a single pure straight line. The latter may include seemingly random variations and in some cases multiple regions of straight-line behavior. We have recently introduced an effective temperature T*(E), derived from the actual local slope of the putative straight line at energy E, which turns out to be a very sensitive detector of deviations from the ideal and, we believe, from equilibrium in the excited state. Plots of T*(E) display a variety of features. An anomaly in the T*(E) spectrum of chlorophyll a can be analyzed on this model, indicating a second weakly fluorescent state about 70 meV below the well-known Q band. The cases of chlorophyll and many others are included in a selective review of applications of the universal relation to fluorescent systems._{y} |

DOI: 10.12693/APhysPolA.95.85 Erratum DOI: 10.12693/APhysPolA.95.1013 PACS numbers: 42.50.Md, 33.70.Jg, 32.50.+d, 31.70.Hq |