Abstract:Our study on the unimolecular decomposition of a relatively stable 1,2-dioxetanone derivative, model compound for bioluminescence processes, indicates the existence of different reaction pathways for ground and excited state formation.
“…By its turn, for OH, the energy gap is of 4.0‐10.0 kcal mol −1 , between IRC of 0.20 and 9.94 amu 1/2 bohr. It should be noted that previous studies indicate that multireference calculations should predict even smaller gaps between S 0 and S 1 . This was ascribed to the importance of multireference correlation in these systems, which implies that S 0 and S 1 become degenerated in the biradical region.…”
Section: Resultsmentioning
confidence: 70%
“…An active space of 10‐in‐8 was chosen for the different dioxetanones (Supporting Information Figures S5 and S6). The choice of active space was made based on previous studies and correspond to OO and CC σ bonding and σ* antibonding orbitals, CO π bonding and π* antibonding orbitals, and oxygen lone pairs orbitals . The MS‐CASPT2 eliminate the method was used to compute the dynamical electron correlation .…”
Section: Computational Sectionmentioning
confidence: 99%
“…It should be noted that previous studies indicate that multireference calculations should predict even smaller gaps between S 0 and S 1 . [22][23][24][34][35][36][37][53][54][55] This was ascribed to the importance of multireference correlation in these systems, which implies that S 0 and S 1 become degenerated in the biradical region. The energetic error present in this region may result from spin contamination in the reference state introduced by a BS technology.…”
Section: Study Of Singlet Chemiexcitationmentioning
Despite decades of research, it is still not clear what is the mechanism behind the efficient chemiexcitation of dioxetanones in chemiluminescent and bioluminescent reactions. In fact, long‐standing theories (charge transfer‐initiated luminescence and chemically induced electron‐exchange luminescence) have been demonstrated to not be able to explain this phenomenon. Herein, a theoretical approach using reliable and up‐to‐date methodology was used to address this problem, by focusing on model dioxetanones. Time‐dependent (TD)‐Density functional theory (DFT) and multireference complete‐active‐space second‐order perturbation theory (CASPT2) calculations provided evidence that points to efficient intramolecular chemiexcitation being the result of the reacting molecules having access to a long zone of the Potential energy surface (PES), within the biradicalar region, where S0 and S1 are degenerate. Molecules with inefficient chemiexcitation are unable to reach this zone of degeneracy. Our main finding is that access to the region of degeneracy appears to be given due to increased interaction between the keto and CO2 moieties, as supported by the use of the activation strain model and Born‐Oppenheimer molecular dynamics, which extends the biradical region by delaying the rupture of the peroxide ring. Increased interaction derives from attractive electrostatic interactions between the moieties of dioxetanone. Thus, we hypothesize that efficient chemiexcitation results not only from electron/charge transfer and subsequent charge annihilation but is instead based on the degree of interaction between the keto and CO2 moieties, which controls the access to a region of degeneracy between the ground and excited states.
“…By its turn, for OH, the energy gap is of 4.0‐10.0 kcal mol −1 , between IRC of 0.20 and 9.94 amu 1/2 bohr. It should be noted that previous studies indicate that multireference calculations should predict even smaller gaps between S 0 and S 1 . This was ascribed to the importance of multireference correlation in these systems, which implies that S 0 and S 1 become degenerated in the biradical region.…”
Section: Resultsmentioning
confidence: 70%
“…An active space of 10‐in‐8 was chosen for the different dioxetanones (Supporting Information Figures S5 and S6). The choice of active space was made based on previous studies and correspond to OO and CC σ bonding and σ* antibonding orbitals, CO π bonding and π* antibonding orbitals, and oxygen lone pairs orbitals . The MS‐CASPT2 eliminate the method was used to compute the dynamical electron correlation .…”
Section: Computational Sectionmentioning
confidence: 99%
“…It should be noted that previous studies indicate that multireference calculations should predict even smaller gaps between S 0 and S 1 . [22][23][24][34][35][36][37][53][54][55] This was ascribed to the importance of multireference correlation in these systems, which implies that S 0 and S 1 become degenerated in the biradical region. The energetic error present in this region may result from spin contamination in the reference state introduced by a BS technology.…”
Section: Study Of Singlet Chemiexcitationmentioning
Despite decades of research, it is still not clear what is the mechanism behind the efficient chemiexcitation of dioxetanones in chemiluminescent and bioluminescent reactions. In fact, long‐standing theories (charge transfer‐initiated luminescence and chemically induced electron‐exchange luminescence) have been demonstrated to not be able to explain this phenomenon. Herein, a theoretical approach using reliable and up‐to‐date methodology was used to address this problem, by focusing on model dioxetanones. Time‐dependent (TD)‐Density functional theory (DFT) and multireference complete‐active‐space second‐order perturbation theory (CASPT2) calculations provided evidence that points to efficient intramolecular chemiexcitation being the result of the reacting molecules having access to a long zone of the Potential energy surface (PES), within the biradicalar region, where S0 and S1 are degenerate. Molecules with inefficient chemiexcitation are unable to reach this zone of degeneracy. Our main finding is that access to the region of degeneracy appears to be given due to increased interaction between the keto and CO2 moieties, as supported by the use of the activation strain model and Born‐Oppenheimer molecular dynamics, which extends the biradical region by delaying the rupture of the peroxide ring. Increased interaction derives from attractive electrostatic interactions between the moieties of dioxetanone. Thus, we hypothesize that efficient chemiexcitation results not only from electron/charge transfer and subsequent charge annihilation but is instead based on the degree of interaction between the keto and CO2 moieties, which controls the access to a region of degeneracy between the ground and excited states.
“…Proper description of bioluminescence and chemiluminescence at the molecular level requires methods able to locate conical intersections and singlet‐triplet crossings along the potential energy surface of chemical reactions involving species with energy‐degenerate open‐shell electronic configurations . Although the use of excited‐state multiconfigurational methods are the state‐of‐the‐art approach for such studies, important insight on the mechanisms of bioluminescent and chemiluminescent transformations came also from simpler approaches, including density functional studies or even from semiempirical calculations (Scheme ).…”
Section: The (Bio)chemistry Of Four‐membered Ring Peroxidesmentioning
confidence: 99%
“…The unimolecular decomposition of 1,2‐dioxetanones produces carbon dioxide in the ground state and an excited‐state carbonyl compound (Φ T up to 10% and Φ S < 0.1%) . In contrast with the indirect chemiluminescence of 1,2‐dioxetanes substituted with simple alkyl or aryl groups, attempts to enhance the chemiluminescence of 1,2‐dioxetanones with fluorescent energy acceptors resulted in an increase of the rate of peroxide decomposition that depends on the oxidation potential of the fluorophore.…”
Section: The (Bio)chemistry Of Four‐membered Ring Peroxidesmentioning
Four-membered cyclic peroxides are high-energy compounds often associated to cold light emission, but whose chemical and biological roles are still matters of debate. The often-dangerous synthesis of 1,2-dioxetanes, achieved around 50 years ago, has been mastered over the years to a point where some derivatives are commercially available. This fact does not imply that 1,2-dioxetanes can be conveniently prepared in the gram scale or that the synthesis of analogous 1,2-dioxetanones and the elusive 1,2-dioxetanedione are simple. Important questions on the mechanism of chemiluminescence and bioluminescence reactions are under experimental and theoretical scrutiny. The available data have contributed to relate structural and medium effects to the quantum efficiency of these compounds to produce excited states. Consequently, such peroxides have been suggested to produce biologically relevant electronically excited species in vivo in the absence of light. The connection of this hypothesis with melanin-mediated photodamage in the dark has renewed the interest in such cyclic peroxides. This review gives some insight on the synthesis, chemiluminescence mechanism, and biological relevance of 1,2-dioxetanes, 1,2-dioxetanones, and 1,2-dioxetanedione and provides practical protocols for those interested in engaging this field.
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