Bioluminescence is a phenomenon that has fascinated mankind for centuries. Today the phenomenon and its sibling, chemiluminescence, have impacted society with a number of useful applications in fields like analytical chemistry and medicine, just to mention two. In this review, a molecular-orbital perspective is adopted to explain the chemistry behind chemiexcitation in both chemi- and bioluminescence. First, the uncatalyzed thermal dissociation of 1,2-dioxetane is presented and analyzed to explain, for example, the preference for triplet excited product states and increased yield with larger nonreactive substituents. The catalyzed fragmentation reaction and related details are then exemplified with substituted 1,2-dioxetanone species. In particular, the preference for singlet excited product states in that case is explained. The review also examines the diversity of specific solutions both in Nature and in artificial systems and the difficulties in identifying the emitting species and unraveling the color modulation process. The related subject of excited-state chemistry without light absorption is finally discussed. The content of this review should be an inspiration to human design of new molecular systems expressing unique light-emitting properties. An appendix describing the state-of-the-art experimental and theoretical methods used to study the phenomena serves as a complement.

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The hitherto unknown monomethyl derivative If and the parent 1,2-dioxetane lg have been prepared and fully characterized. The influence of the degree and pattern of methyl substitution of the complete set of 1,2-dioxetanes la-g on the activation parameters (AH*, AS*, and AG') and on the excitation yields ( and 5) have been determined. It was found that (1) the thermal stability increases with the degree of methylation, (2) the pattern of methylation does not alter appreciably thermal stability, (3) triplet n,ir* states are preferentially energized, and (4) the triplet and singlet excitation yields increase with the degree of methylation. These experimental results are compared with thermochemical estimates and rationalized in terms of the diradical hypothesis and energy surface crossings. The present findings are most consistent with the merged mechanism, in which the activated complex starts out on the ground-state diradical energy surface and crosses over to the carbonyl excited state surfaces, yielding excited carbonyl fragments.Numerous recent results1 of substituent effects in the thermolysis of 1,2-dioxetanes have been interpreted in favor of a diradical2 rather than a concerted3,4 mechanism (Scheme I). A series of ris/Zra ns-3,4-dialkyl-lc and 3,3-dialkyl-l,2-dioxetaneslf reveal that 3,3-interactions are more important than 3,4-inter-

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Although the mechanisms of many chemiluminescence (CL) reactions have been intensively studied, no general model has been suggested to rationalize the efficiency of these transformations. To contribute to this task, we report here quantum yields for some well-characterized CL reactions, concentrating on recent reports of efficient transformations. Initially, a short review on the most important general CL mechanisms is given, including unimolecular peroxide decomposition, electrogenerated CL, as well as the intermolecular and intramolecular catalyzed decomposition of peroxides. Thereafter, quantum yield values for several CL transformations are compiled, including the unimolecular decomposition of 1,2-dioxetanes and 1,2-dioxetanones, the catalyzed decomposition of appropriate peroxides and the induced decomposition of properly substituted 1,2-dioxetane derivatives. Finally, some representative examples of quantum yields for complex CL transformations, like luminol oxidation and the peroxyoxalate reaction, in different experimental conditions are given. This quantum yield compilation indicates that CL transformations involving electron transfer steps can occur with high efficiency in general only if the electron transfer is of intramolecular nature, with the intermolecular processes being commonly inefficient. A notable exception to this general rule is the peroxyoxalate reaction which, also constituting an example of an intermolecular electron transfer system, possesses very high quantum yields.

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A high-energy intermediate in the peroxyoxalate reaction can be accumulated at room temperature under specific reaction conditions and in the absence of any reducing agent in up to micromolar concentrations. Bimolecular interaction of this intermediate, accumulated in the reaction of oxalyl chloride with hydrogen peroxide, with an activator (highly fluorescent aromatic hydrocarbons with low oxidation potential) added in delay shows unequivocally that this intermediate is responsible for chemiexcitation of the activator. Activation parameters for the unimolecular decomposition of this intermediate (DeltaH(double dagger) = 11.2 kcal mol(-1); DeltaS(double dagger) = -23.2 cal mol(-1) K(-1)) and for its bimolecular reaction with 9,10-diphenylanthracene (DeltaH(double dagger) = 4.2 kcal mol(-1); DeltaS(double dagger) = -26.9 cal mol(-1) K(-1)) show that this intermediate is much less stable than typical 1,2-dioxetanes and 1,2-dioxetanones and demonstrate its highly favored interaction with the activator. Therefore, it can be inferred that structural characterization of the high-energy intermediate in the presence of an activator must be highly improbable. The observed linear free-energy correlation between the catalytic rate constants and the oxidation potentials of several activators definitely confirms the occurrence of the chemically initiated electron-exchange luminescence (CIEEL) mechanism in the chemiexcitation step of the peroxyoxalate system.