Printer Friendly

Theoretical Analysis of the Effect Provoked by Bromine-Addition on the Thermolysis and Chemiexcitation of a Model Dioxetanone.

1. Introduction

Bioluminescence is a widespread natural phenomenon in which living organisms convert chemical energy into light emission via biochemical reactions [1-5]. Bioluminescence can be found in organisms as different as bacteria, dinoflagellates, fungi, crustaceans, worms, insects, and fishes. Light emission from these systems is the result of enzyme-catalyzed reactions, which can be divided into two main classes: luciferase-luciferin reactions [2, 5-8] and photoprotein systems [2, 9]. The luciferase enzyme is responsible for catalyzing the oxidation of its substrate, luciferin, which generates an electronically excited singlet state product. This product, generally termed oxyluciferin, subsequently relaxes to the ground state by photon emission. It should be noted that luciferin, luciferase, and oxyluciferin are only generic terms, showing significant structural differences between bioluminescent species. Moreover, luciferase-luciferin reactions are the most prevalent bioluminescent systems [1-3, 5-8].

Photoprotein systems have been found to be exclusive to marine organisms and are characterized by the formation of a stable enzyme-substrate complex [2]. Such complex is formed between the apoprotein and an oxygenated marine luciferin (2-hydroxyperoxycoelenterazine). Binding of calcium ions to the photoprotein surface triggers the decomposition of the stable complex, which occurs with light emission [2].

Bioluminescence can be considered a subtype of chemiluminescence, in which light emission arises from a chemical reaction [1, 10, 11]. The efficiency of light emission of both bioluminescent and chemiluminescent reactions is described in terms of quantum yield, which is controlled by three factors [1, 10, 11]: chemical yield of the ground state reaction, chemiexcitation yield of the singlet excited state product, and finally the fluorescent quantum yield of the emitter. Typically, bioluminescent systems present significantly higher quantum yields than chemiluminescent reactions, with some reactions reaching quantum yields of 45-61% [12]. Given this efficient production of electronically singlet excited state products, relative nontoxicity of luciferin compounds, and the relatively simple chemistry of these systems, among other beneficial characteristics (as sensitivity and sensibility), several chemi-/bioluminescent systems have gained numerous biomedical, pharmaceutical, and bioanalytical applications. More specifically, these systems are used in the analytical determination of ATP and other metabolites, in environmental monitoring, in bioimaging, and in biosensing, as a gene reporter, tested as alternative excitation sources in photodynamic therapy of cancer, and used in investigations of infectious diseases, among others [13-17].

[formula not reproducible]

The efficient formation of singlet excited state products, necessary for the use of these systems in the many applications referred above, is only made possible by the formation of cyclic peroxide intermediates during the different chemi- and bioluminescent reactions [18-28]. Within the large number of different chemi- and bioluminescent systems, these peroxide intermediates can take the form of dioxetanes (I), dioxetanones (II), or dioxetanedione (III) [18-28], which can be seen in Scheme 1. These cyclic peroxides are responsible for chemi- and bioluminescence as their thermolysis provides a route for a thermally activated ground state reaction to produce singlet excited state products [18-28]. This chemiexcitation process is thought to arise from crossing points between the ground state and excited state potential energy surfaces (PES) on the reaction coordinate.

It should be noted that while chemi- and bioluminescent systems are better known for their production of singlet excited states, experimental studies have shown that more structurally simple dioxetanes and dioxetanones have the ability to produce triplet excited states [1, 10, 25-27]. While no experimental results are found for more complex chemi-/bioluminescent systems, different theoretical studies have found pathways for triplet chemiexcitation in the thermolysis of dioxetanone rings in several systems [1, 11, 18, 19, 24, 28, 29]. This production of triplet excited states can be problematic for the several practical applications based on the formation of light-emitting singlet states, as triplet states are very easily quenched, and their formation will not be detected with the luminescent and fluorescent approaches typically used to detect chemi-/bioluminescence. Moreover, triplet states are more reactive and are able to produce harmful reactive species (as singlet oxygen), which can lead to some problems when using these systems in biological samples.

While the formation of triplet state (instead of singlet ones) is not desired in the typical applications of chemi-/bioluminescence, such states can have important roles in other applications. One such example is upconversion by triplet-triplet annihilation, which typically proceeds as follows [30-32]: a sensitizer molecule is photoexcited and undergoes intersystem crossing to a triplet state. Subsequently, the sensitizer transfers its energy to an emitter molecule via fast triplet-triplet energy transfer, which stores the energy in the lowest triplet state of the emitter molecules. Then, two emitters interact and triplet-triplet annihilation occurs, which brings one emitter molecule to an excited singlet state while quenching another to its ground state. The emitter then emits light via fluorescence, at a higher energy than that of the photons initially absorbed by the sensitizer. Triplet-triplet annihilation has been already applied with success in several research fields, as in luminescence bioimaging [33], photovoltaics [34, 35], and photoinduced drug release [36].

Another useful application of triplet excited states is on the field of photocatalysis [37-39]. In this field, photosensitizers are used to mediate photochemical reactions by absorbing light and using that energy to activate ground state reactants toward some specific chemical reactions. One common method of photoactivation is via energy transfer from the longer-lived triplet state of the photosensitizer to the substrate [37-39]. Another photoactivation pathway involves an electron transfer from or to the photoexcited sensitizer [37, 38].

Given this, if one can shift the spin of the chemi-/bioluminescent products, from light-emitting singlet to triplet states, one can open the door for new types of applications for chemi- and bioluminescent systems, as in upconversion processes by triplet-triplet annihilation and photocatalysis. One way to facilitate intersystem crossing to triplet states is to introduce heavy atoms (as bromine and iodine) into the molecular structures, the so called "heavy atom effect" [40-42]. Thus, the objective of this work is to model theoretically the effect of bromine-substitution in a model dioxetanone (IV, Scheme 1) and, more specifically, in its thermolysis and triplet chemiexcitation steps. To our knowledge, this is the first theoretical study trying to understand the possible role of the "heavy atom effect" in the reactions of dioxetanone molecules and in what way it affects triplet chemiexcitation. To this end, a methodology combining density functional theory- (DFT-) based and multireference methods was used.

2. Theoretical Methodology

All calculations were made with the Gaussian 09 program package [43], with no solvent effects. DFT methods (particularly long-range-corrected hybrid exchange-correlation density functionals) have been gaining traction in the study of chemi-/bioluminescent reactions, given their ability to provide quite accurate qualitative pictures for these systems [18-21 ,24, 28, 44-47]. In thisstudywasusedtheCAM-B3LYP long-range-corrected density functional [44], which provides good estimates for [pi] [right arrow] [[pi].sup.*] and [pi] [right arrow] [[pi].sup.*] local excitations and charge transfer and Rydberg states [45]. Moreover, this functional was already used with success in the study of different dioxetanones [20,21].

Geometry optimizations and frequency calculations were made with the CAM-B3LYP functional, with the 6-31G(d, p) basis set being used for all atoms except bromine, for which the LanL2DZ basis set was used. The combination of 6-31G(d, p) and LanL2DZ basis set was termed Basis Set-1 (BS-1). A restricted (R) approach was used for closed-shell species, while an unrestricted (U) species was used for open-shell structures. The U approach was used with a broken-symmetry technology, which mixes the HOMO and LUMO, making an initial guess for a biradical.

The thermolysis reaction of the model dioxetanones was studied by performing intrinsic reaction coordinates (IRC) [48], at the CAM-B3LYP/BS-1 level of theory, which assessed if the obtained transition states connected the desired reactants and products. The transition states were located by using the STQN method [49]. In this work was used the QST3 variant, which requires three molecular specifications: the reactants, the products, and an initial structure for the transition state. The Cartesian coordinates of these transition state structures, used in the IRC calculations, can be found in Tables S1 and S2 of Supplementary Material available online at

The energies of the geometry optimizations, IRC, and QST3-obtained structures were reevaluated by single point calculations with the CAM-B3LYP density functional and the 6-31 + G(d, p) basis set for all atoms, except for bromine. For this atom, the LanL2DZdp basis set was used, which includes polarization and diffuse functions. The combination of 6-31 + G(d, p) and LanL2DZdp basis set was termed Basis Set-2 (BS-2). Thus, the energies of the singlet ground state ([S.sub.0]) and first triplet state ([T.sub.1]) were both calculated at the CAM-B3LYP/BS-2 level of theory.

The spin-orbit coupling between [S.sub.0] and [T.sub.1] states was calculated by using the CASSCF method [50]. The LanL2DZ basis set was used for all atoms. The active space consisted of two electrons on two orbitals. These were single point energy calculations made on the DFT-computed IRC- or QST3-obtained structures.

3. Results and Discussion

We started this work by analyzing the thermolysis reaction of unsubstituted dioxetanone IVa and monobrominated species IVb, whose energetic profiles are presented in Figures 1(a) and 1(c), respectively. In Figures 1(b) and 1(d) are presented important geometric parameters: the bond lengths of [O.sub.1] - [O.sub.4] and [C.sub.2] - [C.sub.3] (Scheme 1). It should be noted that the imino- cyclopentadienyl moiety was based on the scaffold of aza-BODIPY [40-42], which are molecules capable of producing triplet states upon photoexcitation, when they are functionalized with heavy atoms.

Analysis of the geometric parameters shows that the thermolysis of both species occurs via a stepwise mechanism. The reaction begins by [O.sub.1] - [O.sub.4] bond breaking, while the length of [C.sub.2] - [C.sub.3] remains constant. Only after [O.sub.1] - [O.sub.4], does the length of [C.sub.2] - [C.sub.3] increases, subsequently leading to its cleavage. Analysis of the ([S.sup.2]) value for the transition state of both IVb (~0.57) and IVa (~0.55) showed that these structures have a biradical character. Given this, we can ascribe a stepwise-biradical mechanism for the thermolysis of both dioxetanone species, which is in line with previous theoretical studies of such molecules [18, 20, 21, 24, 28, 29].

While a stepwise-biradical mechanism is usually found in the decomposition of these cyclic peroxides, it can be further subdivided: the biradical is formed due to an electron transfer from an electron-rich moiety to the dioxetanone, thereby forming a radical cation and a radical anion, respectively; the biradical is formed due to the homolytic cleavage of the [O.sub.1] - [O.sub.4] bond. In this case, both molecules appear to undergo thermolysis via homolysis, as the electron spin density of the transition state resides only on the [O.sub.1] and [O.sub.4] heteroatoms (Figures 2(c) and 2(d)). This finding is in line with the limited charge transfer found between the dioxetanone and imino-cyclopentadiene moieties, as demonstrated in Figures 2(a) and 2(b). The atomic charges were measured within the Natural Population Analysis (NPA) scheme. The finding that these molecules undergo a homolysis-based stepwise-biradical thermolysis can be attributed to the absence of an ionizable group, as seen before in the theoretical analysis of such molecules [18, 20, 21, 24, 28, 29].

Both species have similar activation energies of 24.7 kcal [mol.sup.-1] for IVa and 24.5 kcal [mol.sup.-1] for IVb. These energies were calculated at the CAM-B3LYP/BS-2 level of theory, with thermal corrections calculated at the CAM-B3LYP/BS-1 level of theory. Considering that no solvents effects were considered and that these species are only model dioxetanones, the obtained activation parameters compare well with the experimentally obtained ones for several cyclic peroxides (within ~20.0 kcal [mol.sup.-1]) [51-53].

So far, the main conclusion is that the addition of a bromine atom affects slightly the decomposition of the model dioxetanone, as there are only very minor differences between the thermolysis of species IVa and IVb. In fact, both species present the same characteristics as other dioxetanone without an ionized group [18-21, 24, 28, 29].

In the same vein, we have found a pathway for triplet chemiexcitation for species IVa and IVb (Figures 1(a) and 1(c), resp.), in line with other theoretical works on different dioxetanones, dioxetanes, and dioxetanedione [11, 18, 19, 24, 28, 29]. Upon starting the reaction, the energetic difference between [S.sub.0] and [T.sub.1] states was large for both molecules (about 48 kcal [mol.sup.-1]). However, from the reactant onward, the energy of the [T.sub.1] state decreased significantly to a point in both species where the [S.sub.0] - [T.sub.1] energy gap is low enough to allow chemiexcitation: 2.5 kcal [mol.sup.-1] (at 0.32 [amu.sup.1/2] bohr) for IVa and 2.6 kcal [mol.sup.-1] (at 0.32 [amu.sup.1/2] bohr) for IVb. In conclusion, by analyzing the [S.sub.0] and [T.sub.1] energetic profiles, our results indicate that both IVa and IVb species are capable of triplet chemiexcitation. Moreover, the very similar [S.sub.0] - [T.sub.1] energy gap suggests a triplet chemiexcitation of similar magnitude, thereby indicating a small effect provoked by the addition of a bromine heavy atom.

It should be noted, however, that intersystem crossing is a process formally forbidden in nonrelativistic quantum theory, and, so, inferring singlet-triplet transition probabilities from energy gaps is not sufficiently accurate [40, 54]. So, to assess the efficiency of intersystem crossing, we must take into account the spin-orbit coupling (SOC) between [S.sub.0] and [T.sub.1] [40, 54]. These were computed at the multireference CASSCF level of theory, and the SOC values for IVa and IVb are presented in Table 1. The CASSCF-computed [S.sub.0] - [T.sub.1] energy gaps (3.1 kcal [mol.sup.-1] for IVb and 2.9 kcal [mol.sup.-1] for IVa) are in line with the DFT-computed ones gap (2.5 kcal [mol.sup.-1] for IVb and 2.6 kcal [mol.sup.-1] for IVa). Once again, it appears that the addition of a bromine heavy atom has little effect, as the SOC values for IVa (5.3 [cm.sup.-1]) and IVb (6.1 [cm.sup.-1]) are very similar, despite the SOC being higher for the monobrominated species.

So far, it does appear that the addition of a bromine atom has only a limited effect on the triplet chemiexcitation of model dioxetanone IV. However, it might be possible that this lack of effect is due to the position of bromine-substitution in the cyclopentadiene moiety and not due to a general absence of the "heavy atom effect" in this molecule. To test this hypothesis, we have calculated transition state structures (with the QST3 method, at the CAM-B3LYP/SD-1 level of theory) for species IVb, IVc, and IVd. The Cartesian coordinates of these structures can be found in Tables S3-S5 of Supplementary Material. At those DFT-computed structures, CASSCF single point energy calculations were made to obtain the SOC values (Table 1). The CASSCF-computed [S.sub.0] - [T.sub.1] energy gaps are similar to all species (between 10.8 and 11.4 kcal [mol.sup.-1]), further indicating that the position of the bromine atom has little effect on the value of the [S.sub.0] - [T.sub.1] energy gap. However, this is not true for the SOC values. These increased more significantly, from 7.5 to 11.5 [cm.sup.-1], with IVd presenting SOC values more than double the ones presented previously by IVa. Thus, these results indicate that the addition of heavy atoms can indeed increase the efficiency of intersystem crossing and, so, the formation of triplet state products, but this effect is controlled by the position in which the heavy atom is inserted.

Having analyzed the effect of monobromination on the thermolysis and triplet chemiexcitation of model dioxetanone IV, we have studied some properties of the [T.sub.1] reaction product (species Va-d, Scheme 1). The Cartesian coordinates of these structures can be found on Tables S6-S9 of Supplementary Material. These properties are the electron affinity (EA), ionization energies (IE), and [T.sub.1] - [S.sub.0] energy gaps (present in Table 2). The EA and IE were computed vertically, with single point energy calculations on the [T.sub.1] structure, with [T.sub.1] as the reference state. All V species present very high IEs, with a limited effect provoked by monobromination, which limits the use of these species as electron donors in photocatalysis. On the contrary, the EA values are more suitable for the use of these species as electron acceptors. Moreover, the addition of bromine atoms can significantly improve the EA of V up to 8.8 kcal [mol.sup.-1], depending on the location of the substitution on the cyclopentadiene ring. As for [T.sub.1] - [S.sub.0] energy gaps, these were computed adiabatically. Our calculations have indicated that monobromination has a limited effect on the [T.sub.1] - [S.sub.0] energy gaps, except for species Vc, which decreased the gap by 3.5 kcal [mol.sup.-1].

4. Conclusion

Chemi- and bioluminescence are phenomena in which chemical energy is converted into light emission, via chemical and biochemical reactions. Given this feature, coupled to high quantum yields, relative nontoxicity of the reaction substrates, and the relatively simple chemistry, among other beneficial characteristics (as sensitivity and sensibility), several chemi-/bioluminescent systems have gained numerous biomedical, pharmaceutical, and bioanalytical applications.

The efficient formation of light-emitting singlet excited states, needed for the applications referred above, is made possible by the formation of cyclic peroxides (as dioxetanes or dioxetanones). Their thermolysis provides a route for a thermally activated ground state reaction to produce singlet excited state products. However, both experimental and theoretical studies have demonstrated that the thermolysis of these species is also able to produce triplet states. While the formation of such states is not desired in the typical applications of chemi-/bioluminescence, efficient production of triplet states might open the door for the use of chemi-/bioluminescent systems as sensitizers in the fields of photocatalysis and upconversion processes by triplet-triplet annihilation, among others.

Given this, the objective of this theoretical study was to assess the effect induced by heavy atom substitution (in this case, bromine) on the thermolysis and triplet chemiexcitation of a model dioxetanone. Our calculations indicated that monobromination has little effect on the [S.sub.0] thermolysis reaction, with little effect on the energetics of the reaction and on the variation of other parameters (as selected bond lengths and electron spin and charge density). However, the addition of bromine atoms can increase the spin-orbit coupling of the [S.sub.0] and [T.sub.1], thereby increasing the efficiency of intersystem crossing. Nevertheless, this effect is dependent on the position of the bromine-substitution. Study of the [T.sub.1] reaction product showed a general limited effect provoked by monobromination on the ionization energies and [S.sub.0] - [T.sub.1] gaps. On the contrary, monobromination improves the electron affinity of the [T.sub.1] product, with the degree of improvement being controlled by the position of monobromination. 10.1155/2017/1903981

Conflicts of Interest

The authors declare that they have no conflicts of interest.


This work was made in the framework of Project PTDC/QEQ-QFI/0289/2014, which is funded with national funds by FCT/MEC (PIDDAC). The project is also cofunded by "Fundo Europeu de Desenvolvimento Regional" (FEDER), through "COMPETE-Programa Operacional Fatores de Competitividade" (COMPETE-POFC). This work was also made in the framework of the Project Sustainable Advanced Materials (NORTE-01-00145-FEDER-000028), funded by "Fundo Europeu de Desenvolvimento Regional (FEDER)," through "Programa Operacional do Norte" (NORTE2020). Acknowledgment to Project POCI-01-0145FEDER-006980, funded by FEDER through COMPETE2020, is also made. The Laboratory for Computational Modeling of Environmental Pollutants-Human Interactions (LACOMEPHI) is acknowledged. Luis Pinto da Silva also acknowledges a postdoctoral grant funded by Project Sustainable Advanced Materials (NORTE-01-00145-FEDER-000028).


[1] L. Pinto Da Silva and J. C. G. Esteves Da Silva, "Firefly chemiluminescence and bioluminescence: efficient generation of excited states," ChemPhysChem, vol. 13, no. 9, pp. 2257-2262, 2012.

[2] A. S. Tsarkova, Z. M. Kaskova, and I. V. Yampolsky, "A tale of two luciferins: fungal and earthworm new bioluminescent systems," Accounts of Chemical Research, vol. 49, no. 11, pp. 2372-2380, 2016.

[3] J. Vieira, L. P. Da Silva, and J. C. G. E. Da Silva, "Advances in the knowledge of light emission by firefly luciferin and oxyluciferin," Journal of Photochemistry and Photobiology B: Biology, vol. 117, pp. 33-39, 2012.

[4] E. P. Coutant and Y. L. Janin, "Synthetic routes to coelenterazine and other imidazo [1, 2-a] pyrazin-3-one luciferins: essential tools for bioluminescence-based investigations," Chemistry, vol. 21, pp. 17158-17171, 2015.

[5] S. V. Markova and E. S. Vysotski, "Coelenterazine-dependent luciferases," Biochemistry (Moscow), vol. 80, no. 6, pp. 714-732, 2015.

[6] S. M. Marques and J. C. G. Esteves Da Silva, "Firefly bioluminescence: a mechanistic approach of luciferase catalyzed reactions," IUBMB Life, vol. 61, no. 1, pp. 6-17, 2009.

[7] S. Tu and H. I. X. Mager, "Biochemistry of bacterial bioluminescence," Photochemistry and Photobiology, vol. 62, no. 4, pp. 615-624, 1995.

[8] D. E. Desjardin, A. G. Oliveira, and C. V Stevani, "Fungi bioluminescence revisited," Photochemical & Photobiological Sciences, vol. 7, pp. 170-182, 2008.

[9] O. Shimomura and F. H. Johnson, "Peroxidized coelenterazine, the active group in the photoprotein aequorin," Proceedings of the National Academy of Sciences of the United States of America, vol. 75, pp. 2611-2615, 1978.

[10] M. Matsumoto, "Advanced chemistry of dioxetane-based chemiluminescent substrates originating from bioluminescence," Journal of Photochemistry and Photobiology C: Photochemistry Reviews, vol. 5, no. 1, pp. 27-53, 2004.

[11] I. Navizet, Y. J. Liu, N. Ferre, D. Roca-Sanjuan, and R. Lindh, "The chemistry of bioluminescence: an analysis of chemical functionalities," ChemPhysChem, vol. 12, pp. 3064-3076, 2011.

[12] K. Niwa, Y. Ichino, S. Kumata et al., "Quantum yields and kinetics of the firefly bioluminescence reaction of beetle luciferases," Photochemistry and Photobiology, vol. 86, no. 5, pp. 1046-1049, 2010.

[13] A. Roda, M. Guardigli, E. Michelini, and M. Mirasoli, "Bioluminescence in analytical chemistry and in vivo imaging," TrAC Trends in Analytical Chemistry, vol. 28, no. 3, pp. 307-322, 2009.

[14] M. B. Gu, R. J. Mitchell, and B. C. Kim, "Whole-cell-based biosensors for environmental biomonitoring and application," Advances in Biochemical Engineering/Biotechnology, vol. 87, pp. 269-305, 2004.

[15] C. M. Magalhaes, J. C. G. Esteves da Silva, and L. Pinto da Silva, "Chemiluminescence and Bioluminescence as an excitation source in the photodynamic therapy of cancer: a critical review," ChemPhysChem, vol. 17, pp. 2286-2294, 2016.

[16] K. E. Luker and G. D. Luker, "Bioluminescence imaging of reporter mice for studies of infection and inflammation," Antiviral Research, vol. 86, no. 1, pp. 93-100, 2010.

[17] L. Cevenini, M. M. Calabretta, A. Lopreside et al., "Exploiting nanoluc luciferase for smartphone-based bioluminescence cell biosensor for (anti)-inflammatory activity and toxicity," Analytical and Bioanalytical Chemistry, vol. 408, pp. 8859-8868, 2016.

[18] L. Pinto da, C. M. Silva, and J. C. G. Esteves da Silva, "Interstate crossing-induced chemiexcitation mechanism as the basis for imidazopyrazinone bioluminescence," ChemistrySelect, vol. 1, pp. 3343-3356, 2016.

[19] L. P. Da Silva and J. C. G. E. Da Silva, "Interstate crossing-induced chemiexcitation as the reason for the chemiluminescence of dioxetanones," ChemPhysChem, vol. 14, no. 5, pp. 1071-1079, 2013.

[20] B.-W. Ding, P. Naumov, and Y.-J. Liu, "Mechanistic insight into marine bioluminescence: photochemistry of the chemiexcited cypridina (sea firefly) lumophore," Journal of Chemical Theory and Computation, vol. 11, no. 2, pp. 591-599, 2015.

[21] B. W. Ding and Y. J. Liu, "Bioluminescence of firefly squid via mechanism of single electron-transfer oxygenation and charge-transfer-induced luminescence," Journal of the American Chemical Society, vol. 139, pp. 1106-1119, 2017.

[22] L. F. M. L. Ciscato, F. H. Bartoloni, A. S. Colavite, D. Weiss, R. Beckert, and S. Schramm, "Evidence supporting a 1, 2-dioxetanone as an intermediate in the benzofuran-2(3H)one chemiluminescence," Photochemical and Photobiological Sciences, vol. 13, no. 1, pp. 32-37, 2014.

[23] S. Schramm, I. Navizet, P. Naumov et al., "The light emitter of the 2-coumar-anone chemiluminescence: theoretical and experimental elucidation of a possible model for bioluminescent systems," European Journal of Organic Chemistry, vol. 4, 2016.

[24] L. Pinto Da Silva and J. C. G. Esteves Da Silva, "Mechanistic study of the unimolecular decomposition of 1, 2-dioxetanedione," Journal of Physical Organic Chemistry, vol. 26, no. 8, pp. 659-663, 2013.

[25] W. Adam and W. J. Baader, "Effects of methylation on the thermal stability and chemiluminescence properties of 1, 2-dioxetanes," Journal of the American Chemical Society, vol. 107, no. 2, pp. 410-416, 1985.

[26] S. P. Schmidt and G. B. Schuster, "Kinetics of unimolecular dioxetanone chemiluminescence. Competitive parallel reaction paths," Journal of the American Chemical Society, vol. 100, no. 17, pp. 5559-5561, 1978.

[27] W. Adam, "Thermal generation of electronic excitation with hyperenergetic molecules," Pure and Applied Chemistry, vol. 52, no. 12, pp. 2591-2608, 1980.

[28] H. Isobe, S. Yamanaka, S. Kuramitsu, and K. Yamaguchi, "Regulation mechanism of spin-orbit coupling in charge-transfer-induced luminescence of imidazopyrazinone derivatives," Journal of the American Chemical Society, vol. 130, no. 1, pp. 132-149, 2008.

[29] L. Yue, Y.-J. Liu, and W.-H. Fang, "Mechanistic insight into the chemiluminescent decomposition of firefly dioxetanone," Journal of the American Chemical Society, vol. 134, no. 28, pp. 11632-11639, 2012.

[30] T. F. Schulze and T. W. Schmidt, "Photochemical upconversion: present status and prospects for its application to solar energy conversion," Energy & Environmental Science, vol. 8, pp. 103-125, 2015.

[31] X. Cui, J. Zhao, Y. Zhou, J. Ma, and Y. Zhao, "Reversible photoswitching of triplet-triplet annihilation upconversion using dithienylethene photochromic switches," Journal of the American Chemical Society, vol. 136, no. 26, pp. 9256-9259, 2014.

[32] K. Xu, J. Zhao, D. Escudero, Z. Mahmood, and D. Jacquemin, "Controlling triplet-triplet annihilation upconversion by tuning the PET in aminomethyleneanthracene derivatives," Journal of Physical Chemistry C, vol. 119, no. 42, pp. 23801-23812, 2015.

[33] Q. Liu, T. Yang, W. Feng, and F. Li, "Blue-emissive upconversion nanoparticles for low-power-excited bioimaging in vivo," Journal of the American Chemical Society, vol. 134, no. 11, pp. 5390-5397, 2012.

[34] J. S. Lissau, J. M. Gardner, and A. Morandeira, "Photon upconversion on dye-sensitized nanostructured ZrO2 films," Journal of Physical Chemistry C, vol. 115, no. 46, pp. 23226-23232, 2011.

[35] A. Monguzzi, D. Braga, M. Gandini et al., "Broadband upconversion at subsolar irradiance: triplet-triplet annihilation boosted by fluorescent semiconductor nanocrystals," Nano Letters, vol. 14, no. 11, pp. 6644-6650, 2014.

[36] S. H. C. Askes, A. Bahreman, and S. Bonnet, "Activation of a photodissociative ruthenium complex by triplettriplet annihilation upconversion in liposomes," Angewandte Chemie--International Edition, vol. 53, pp. 1029-1033, 2014.

[37] M. H. Shaw, J. Twilton, and D. W. C. MacMillan, "Photoredox catalysis in organic chemistry," Journal of Organic Chemistry, vol. 81, no. 16, pp. 6898-6926, 2016.

[38] M. Kozlowski and T. Yoon, "Editorial for the Special Issue on Photocatalysis," Journal of Organic Chemistry, vol. 81, no. 16, pp. 6895-6897, 2016.

[39] A. Iyer, S. Jockusch, and J. Sivaguru, "A photo-auxiliary approach--enabling excited state classical phototransformations with metal free visible light irradiation," Chemical Communications, vol. 53, no. 10, 2017.

[40] B. C. De Simone, G. Mazzone, J. Pirillo, N. Russo, and E. Sicilia, "Halogen atom effect on the photophysical properties of substituted aza-BODIPY derivatives," Physical Chemistry Chemical Physics, vol. 19, pp. 2530-2536, 2017.

[41] N. Adarsh, M. Shanmugasundaram, R. R. Avirah, and D. Ramaiah, "Aza-BODIPY derivatives: enhanced quantum yields of triplet excited states and the generation of singlet oxygen and their role as facile sustainable photooxygenation catalysts," Chemistry, vol. 18, no. 40, pp. 12655-12662, 2012.

[42] B. Kucukoz, G. Sevinc, E. Yildiz et al., "Enhancement of two photon absorption properties and intersystem crossing by charge transfer in pentaarylboron-dipyrromethene (BODIPY) derivatives," Physical Chemistry Chemical Physics, vol. 18, pp. 13546-13553, 2016.

[43] M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman et al., Gaussian 09, Revision A.02, Gaussian, Wallingford, Connecticut, USA, 2009.

[44] T. Yanai, D. P. Tew, and N. C. Handy, "A new hybrid exchange-correlation functional using the Coulomb-attenuating method (CAM-B3LYP)," Chemical Physics Letters, vol. 393, no. 1-3, pp. 51-57, 2004.

[45] C. Adamo and D. Jacquemin, "The calculations of excited-state properties with time-dependent density functional theory," Chemical Society Reviews, vol. 42, no. 3, pp. 845-856, 2013.

[46] C. G. Min, L. Pinto da Silva, X. K. Esteves da Silva et al., "A computational investigation of the equilibrium constants for the fluorescent and chemiluminescent states of coelenteramide," ChemPhysChem, vol. 1, pp. 117-123, 2017.

[47] L. Pinto da Silva, C. M. Magalhaes, D. M. A. Crista, and Esteves da Silva J. C. G., "Theoretical modulation of singlet/triplet chemiexcitation of chemiluminescent imidazopyrazinone dioxetanone via C8-substitution," Photochemical & Photobiological Sciencies, 2017.

[48] K. Fukui, "The path of chemical reactions--the IRC approach," Accounts of Chemical Research, vol. 14, no. 12, pp. 363-368, 1981.

[49] C. Peng, P. Y. Ayala, H. B. Schlegel, and M. J. Frisch, "Using redundant internal coordinates to optimize equilibrium geometries and transition states," Journal of Computational Chemistry, vol. 17, no. 1, pp. 49-56, 1996.

[50] M. Klene, M. A. Robb, M. J. Frisch, and P. Celani, "Parallel implementation of the CI-vector evaluation in full CI/CASSCF," Journal of Chemical Physics, vol. 113, no. 14, pp. 5653-5665, 2000.

[51] F. A. Augusto, G. A. De Souza, S. P. De Souza Jr., M. Khalid, and W. J. Baader, "Efficiency of electron transfer initiated chemiluminescence," Photochemistry and Photobiology, vol. 89, no. 6, pp. 1299-1317, 2013.

[52] M. Matsumoto, Y. Ito, M. Murakami, and N. Watanabe, "Synthesis of 5-tert-butyl-1-(3-tert-butyldimethylsiloxy)phenyl-4, 4dimethyl-2, 6, 7-trioxabicyclo[3.2.0]heptanes and their fluoride-induced chemiluminescent decomposition: Effect ofa phenolic electron donor on the CIEEL decay rate in aprotic polar solvent," Luminescence, vol. 17, no. 5, pp. 305-312, 2002.

[53] M. Tanimura, N. Watanabe, H. K. Ijuin, and M. Matsumoto, "Intramolecular Charge-transfer-induced decomposition promoted by an aprotic polar solvent for bicyclic dioxetanes bearing a 4-(benzothiazol-2-yl)-3- hydroxyphenyl moiety," Journal of Organic Chemistry, vol. 76, no. 3, pp. 902-908, 2011.

[54] C. M. Marian, "Spin-orbit coupling and intersystem crossing in molecules," Wiley Interdisciplinary Reviews: Computational Molecular Science, vol. 2, no. 2, pp. 187-203, 2012.

Luis Pinto da Silva, (1, 2) Rui F. J. Pereira, (1) and Joaquim C. G. Esteves da Silva (1, 2, 3)

(1) Chemistry Research Unit (CIQUP), Departamento de Quimica e Bioquimica, Faculdade de Ciencias da Universidade do Porto, R. Campo Alegre 687, 4169-007Porto, Portugal

(2) LACOMEPHI, Departamento de Geociencias, Ambiente e Ordenamento do Territorio, Faculdade de Ciencias da Universidade do Porto, R. Campo Alegre 687, 4169-007 Porto, Portugal

(3) Chemistry Research Unit (CIQUP), Departamento de Geociencias, Ambiente e Ordenamento do Territorio, Faculdade de Ciencias da Universidade do Porto, R. Campo Alegre 687, 4169-007 Porto, Portugal

Correspondence should be addressed to Luis Pinto da Silva;

Received 9 February 2017; Accepted 12 April 2017; Published 26 April 2017

Academic Editor: Teik-Cheng Lim

Caption: FIGURE 1: Energy profiles of the [S.sub.0] and [T.sub.1] states, determined in the [S.sub.0]-computed IRC path, for species IVa (a) and IVb (c). [O.sub.1] - [O.sub.4] and [C.sub.2] - [C.sub.3] bond length variations recorded during the IRC calculations for IVa (b) and IVb (d).

Caption: FIGURE 2: NPA charge density distribution between the dioxetanone and imino-cyclopentadiene moieties, for species IVa (a) and IVb (b). Electron spin density for the transition state structure of the thermolysis of IVa (c) and IVb (d).
TABLE 1: [S.sub.0] - [T.sub.1] energy gaps ([DELTA]E([S.sub.0] -
[T.sub.1]), in kcal [mol.sup.-1]) and respective SOC values
(SOC, in [cm.sup.-1]),  obtained with CASSCF(2, 2)/LanL2DZ single
point energy calculations on CAM-B3LYP/BS-1 structures.

                                   Iva (a)   IVb (a)   IVb (b)

([DELTA]E([S.sub.0] - [T.sub.1])     2.9       3.2      11.4
SOC                                  5.3       6.1       7.5

                                    IVc (b)     IVd (b)

([DELTA]E([S.sub.0] - [T.sub.1])     11.4        10.8
SOC                                   8.6        11.5

(a) Structures obtained during the IRC calculations, corresponding
to points of lower ([S.sub.0]-[T.sub.1]) energy gaps: 2.5 kcal
[mol.sup.-1] (at 0.32 [amu.sup.12] bohr) for IVa and 2.6 kcal
[mol.sup.-1] (at 0.32 [amu.sup.1/2] bohr) for IVb.

(b) Transition state structures obtained with the QST3 method.

TABLE 2: Adiabatic [S.sub.0]-[T.sub.1] energy gaps
([DELTA]E([S.sub.0]-[T.sub.1]), in kcal [mol.sup.-1]) and vertical
ionization energies (IE, in kcal [mol.sup.-1]) and electron affinity
(EA, in kcal [mol.sup.-1]) for the [T.sub.1] state of species Va-d,
obtained at the CAM-B3LYP/BS-2//CAM-B3LYP/BS-1 level of theory.

                                     Va      Vb      Vc      Vd

([DELTA]E([S.sub.0] - [T.sub.1])    25.3    26.0    21.8    24.4
IE                                 190.5   191.1   188.9   187.2
EA                                 -59.1   -67.9   -63.9   -62.2
COPYRIGHT 2017 Hindawi Limited
No portion of this article can be reproduced without the express written permission from the copyright holder.
Copyright 2017 Gale, Cengage Learning. All rights reserved.

Article Details
Printer friendly Cite/link Email Feedback
Title Annotation:Research Article
Author:da Silva, Luis Pinto; Pereira, Rui F.J.; da Silva, Joaquim C.G. Esteves
Publication:Journal of Chemistry
Article Type:Report
Date:Jan 1, 2017
Previous Article:Correlation between Formic Acid Oxidation and Oxide Species on Pt(Bi)/GC and Pt/GC Electrode through the Effect of Forward Potential Scan Limit.
Next Article:Hydrogen Reduction of Hematite Ore Fines to Magnetite Ore Fines at Low Temperatures.

Terms of use | Privacy policy | Copyright © 2022 Farlex, Inc. | Feedback | For webmasters |