Develop dynamic model for predicting traffic CO emissions in urban areas.

The greater the use of energy in the transportation sectors, the higher the emission of carbon monoxide (CO), and hence inevitable harm to environment and human health. In this concern, measuring and predicting of CO emission from transportation sector-especially large cities-is important as it constitute 90 % of all CO emission. Many urban cities in developing world have not properly experienced such measurements or predictions. In this paper, for the first time, field measurements of traffic characteristics data and corresponding CO concentration have been performed for developing a model for predicting CO emissions from transportation sector for New Borg El Arab (NBC), Egypt. The performance of Swiss-German Handbook Emission Factors for Road Transport (HBEFA v3.1) model has been assessed for predicting the CO concentration at roadside in the study area. Results indicated that HBEFA v3.1 underestimate emission figures. The developed CO dynamic emission model involves the traffic flow characteristics with roadside CO concentrations. Acceptable representation of measured CO concentration has been shown by the developed dynamic CO emission model which introduces R (2) = 0.77, mean biases and frictional biases of -0.27 mg m(-3) and 0.09, respectively. A comparison between predicted CO concentrations using HBEFA v3.1 and the promoted dynamic model indicate that HBEFA v3.1 estimates CO emission concentrations in the study area with a mean error and frictional biases 159.26 and 233.33 %, respectively, higher than those of the developed model.

Rotationally resolved high-resolution spectrum of the S(1)-S(0) transition of jet-cooled thioanisole.

The rotationally resolved high-resolution fluorescence excitation spectrum of the 0-0 band in the S(1)← S(0) electronic excitation of thioanisole was observed using the techniques of a collimated supersonic jet and a single-mode ultraviolet laser for the first time. High accurate rotational constants for the S(0) and the S(1) states have been determined by precisely calibrated transition energies of about 1000 assigned rotational lines. The molecular structure of thioanisole has been estimated by high-level MO calculations. The planarity of thioanisole in the S(0) and the S(1) states was also demonstrated clearly. The lifetime of the S(1) state was estimated to be 2.0 ns from the observed line width. This line shape did not change with the magnetic field of 1 Tesla, suggesting that the main radiationless process should be internal conversion to the S(0) state.

Fluorescence spectroscopy of jet-cooled o-fluoroanisole: mixing through Duschinsky effect and Fermi resonance.

Laser-induced fluorescence (LIF) excitation, UV-UV hole burning, and single vibronic level fluorescence (SVLF) spectra of jet-cooled o-fluoroanisole (o-FA) were measured. The most intense lowest-frequency band at 36 612 cm(-1) was assigned to the origin band of the most stable trans conformer. The UV-UV hole-burning spectrum demonstrated that the prominent bands in the LIF excitation spectrum were responsible for the trans conformer. The metastable non-planar conformer was not observed in the spectra. The vibrational band assignments were performed with the aid of quantum chemical calculations at the B3LYP/cc-pVTZ and CIS/6-311G(d,p) levels. The precise analysis of the SVLF spectra indicated that strong vibrational mixing through the Duschinsky effect and the Fermi resonance occurs in the S(1) state.

Excited-state dynamics of 6-aza-2-thiothymine and 2-thiothymine: highly efficient intersystem crossing and singlet oxygen photosensitization.

Significant influences of sulfur and aza substitution on excited-state dynamics in thymine analogues, 6-aza-2-thiothymine (ATT) and 2-thiothymine (2TT), were intensively studied by means of nanosecond transient absorption and time-resolved luminescence spectroscopy. Transient absorption spectral measurements gave distinct spectral features and sufficiently longer lifetimes for both molecules attributable to the T(1) (pi pi*) state under Ar-saturated condition. Additionally, another long-lived subsequent transient was also observed for ATT, which suggests hydrogen abstraction from a ground-state molecule itself takes place only for triplet ATT. Quantum yields for intersystem crossing (Phi(ISC)) were determined to be unity as well as other pyrimidine analogues we reported previously, and efficient photosensitized singlet oxygen O(2)* ((1)Delta(g)) formation was also observed in the presence of dissolved molecular oxygen with a quantum yield (Phi(Delta)) of 0.69 +/- 0.02 for ATT whereas it almost halved for 2TT. These findings have shown the combination of subtle substitutions can possibly control photophysical or photochemical properties such as O(2)* ((1)Delta(g)) formation or reactivity in excited states in addition to the substantial intersystem crossing caused by replacing oxygen O2 in thymine by sulfur (referred to S2 substitution henceforward). The experimental results were corroborated by quantum chemical calculation at the B3LYP/6-31+G(d,p)/PCM level.

Triplet formation of 6-azauridine and singlet oxygen sensitization with UV light irradiation.

Excited state characteristics of 6-azauridine (6AUd), which is known as a medicine against psoriasis and neoplastic, were investigated with laser plash photolysis, time-resolved thermal lensing, and near IR single photon counting method. The triplet-triplet absorption spectrum of 6AUd was observed for the first time. The formation quantum yield of excited triplet 6AUd (Phi(ISC)) was estimated by acetone triplet sensitization and actinometry with benzophenone to be 1.00 +/- 0.07 (248 nm excitation) and 0.78 +/- 0.05 (308 nm excitation). This excitation wavelength effect could be explained by intersystem crossing (ISC) to the excited triplet manifolds occurring during the relaxation on the potential energy surface (PES) of the S(1)(npi*) state and be in competition with internal conversion to the S(0) state after the relaxation to the minimum of the S(1)(npi*) state. 6AUd had a lower Phi(ISC) value than 6-azauracil (6AU) with the 308 nm excitation (Phi(ISC) = 0.93 +/- 0.04 for 6AU). The nucleoside has more vibrational modes than 6AU, and therefore the ribose would accelerate intramolecular vibrational energy redistribution and the relaxation to the minimum of the PES of the S(1)(npi*) state. Sensitized singlet oxygen formation of 6AUd was also detected in the O(2)-saturated condition with quantum yields of 0.49 +/- 0.01 with the 248 nm excitation, indicating the high phototoxicity of 6AUd.

Intersystem crossing to excited triplet state of aza analogues of nucleic acid bases in acetonitrile.

Excited state characteristics of aza analogues of nucleic acid bases, 8-azaadenine (8AA), 5-azacytosine (5AC), 8-azaguanine (8AG), and 6-azauracil (6AU), in acetonitrile solution were comprehensively investigated with steady state absorption and emission spectra, transient absorption measurements, emission measurements for the singlet oxygen molecule, and time-dependent density functional theory (TD-DFT) calculations. The triplet-triplet absorption spectrum of 8AA whose peak was 455 nm was observed for the first time. Sensitized singlet oxygen formation of 8AA was also observed in O(2)-saturated acetonitrile with quantum yields of 0.15 +/- 0.02. It was concluded that there were two kinds of aza analogues of nucleic acid bases: type A had substantial quantum yield for the intersystem crossing and potential of O2 (1Delta(g)) formation (8AA and 6AU), and type B did not (5AC and 8AG). TD-DFT calculations indicated that type A molecules had a dark 1npi* state below the first allowed 1pipi* state, while both S1 and S2 states for type B molecules had a pipi* character. It strongly suggested that the dark 1npi* state below the 1pipi* state would play an important role in the ISC process of aza analogues of nucleic acid bases.

Excited state characteristics of 6-azauracil in acetonitrile: drastically different relaxation mechanism from uracil.

Excited-state dynamics of 6-azauracil (6-AU) and sensitized singlet oxygen formation in acetonitrile solution with UV irradiation were investigated for the first time. In the transient absorption measurement, the 248 nm laser photolysis gave a relatively intense absorption band at 320 nm (= 1100 +/- 100 dm(3) mol(-1) cm(-1)) and a broadband in the 500-700 nm region due to triplet 6-AU. The triplet 6-AU, decaying with the rate constant of (5.3 +/- 0.2) x 10(6) s(-1) in Ar saturated acetonitrile, was quenched by molecular oxygen with the rate constant of (2.5 +/- 0.1) x 10(9) dm(3) mol(-1) s(-1). The formation quantum yield of excited triplet 6-AU was estimated to be unity by acetone triplet sensitization and actinometry with benzophenone. The time-resolved thermal lensing signal of 6-AU was also observed by 248 nm laser excitation. In the presence of molecular oxygen, the sensitization from triplet 6-AU gave rise to formation of singlet oxygen O(2) ((1)Delta(g)) with a quantum yield of 0.63 +/- 0.03. Drastically different excited-state dynamics of aza-substituted uracil from normal uracil were clarified, and the mechanism for the enhancement of intersystem crossing by aza-substitution is discussed.

Reaction dynamics of excited 2-(3-benzoylphenyl)propionic acid (ketoprofen) with histidine.

Photoreaction dynamics of 2-(3-benzoylphenyl)propionic acid (ketoprofen, KP), one of nonsteroidal anti-inflammatory drugs, with histidine in a phosphate buffer solution (pH 7.4) was investigated with the laser flash photolysis. The deprotonated form of KP (KP(-)) was decarboxylated via UV laser excitation to form a carbanion. It was found that histidine accelerates the protonation reaction of the carbanion to 3-ethylbenzophenone ketyl biradical (3-EBPH) for the first time. The experimental results of the photoreaction of KP with alanine as well as the photoreaction of KP with 4-methylimidazole (a part of the side chain of histidine) in methanol, clearly showed that the protonated form of histidine is a key species for the protonation reaction of the carbanion. These series of the initial reactions should result in the occurrence of photosensitization in vivo. The reaction mechanism was discussed in detail.

Conformations of 2-aminoindan in a supersonic jet: the role of intramolecular N-H...pi hydrogen bonding.

Laser-induced fluorescence (LIF), dispersed fluorescence (DF), mass-resolved one-color resonance enhanced two-photon ionization (RE2PI) and UV-UV hole-burning spectra of 2-aminoindan (2-AI) were measured in a supersonic jet. The hole-burning spectra demonstrated that the congested vibronic structures observed in the LIF excitation spectrum were responsible for three conformers of 2-AI. The origins of the conformers were observed at 36931, 36934, and 36955 cm(-1). The DF spectra obtained by exciting the band origins of the three conformers showed quite similar vibrational structures, with the exception of the bands around 600-900 cm(-1). The molecular structures of the three conformers were assigned with the aid of ab initio calculations at the MP2/6-311+G(d,p) level. An amino hydrogen of the most stable conformer points toward the benzene ring. The stability of the most stable conformer was attributed to an intramolecular N-H...pi hydrogen bonding between the hydrogen atom and the pi-electron of the benzene ring. The other two conformers, devoid of intramolecular hydrogen bonding, were also identified for 2-AI. This suggests weak hydrogen bonding in the most stable conformer. The intramolecular N-H...pi hydrogen bonding in 2-AI was discussed in comparison with other weak hydrogen-bonding systems.

Low-frequency vibrations specific for conformers of 1-aminoindan studied by UV-UV hole-burning spectroscopy.

The UV-UV hole-burning spectra of the jet-cooled 1-aminoindan were measured for the first time. Complicated spectral features observed in the laser-induced fluorescence excitation spectrum due to two conformers, R and B, were firmly separated. On the basis of fluorescence measurements and B3LYP/cc-pVTZ calculations, low-frequency ring twisting and ring puckering modes were assigned. These modes are coupled in the S1 state due to the Duschinsky rotation. The Duschinsky matrix was calculated from the normal modes predicted by quantum chemical calculations. The coupling between the twisting and puckering modes for conformer B is stronger than that for conformer R. The twisting mode was observed at 0+99 cm(-1) in the S1 state for conformer B, while not for conformer R. The Franck-Condon activity of the twisting mode substantially differs between the two conformers. The transition to the twisting level for conformer B would be allowed by the Duschinsky rotation. The fluorescence lifetime of conformer vibronic levels was also measured and differed for each conformer.

Triplet formation of 4-thiothymidine and its photosensitization to oxygen studied by time-resolved thermal lensing technique.

Excited-state dynamics of 4-thiothymidine (S4-TdR) and its photosensitization to molecular oxygen in solution with UVA irradiation were investigated. Absorption and emission spectra measurements revealed that UVA photolysis of S4-TdR gives rise to a population of T1(pipi*), following S2(pipi*) --> S1(npi*) internal conversion. In transient absorption measurement, the 355 nm laser photolysis gave broad absorption (380-600 nm) bands of triplet S4-TdR. The time-resolved thermal lensing (TRTL) signal of S4-TdR containing the thermal component due to decay of triplet S4-TdR was clearly observed by the 355 nm laser excitation. The quantum yield for S1 --> T1 intersystem crossing was estimated to be unity by a triplet quenching experiment with potassium iodide. In the presence of molecular oxygen, the photosensitization from triplet S4-TdR gave rise to singlet oxygen O2 (1Deltag) with a quantum yield of 0.50. Therapeutic implications of such singlet oxygen formation are discussed.

Reaction dynamics of excited ketoprofen with triethylamine.

The reaction dynamics of ketoprofen (KP) with and without triethylamine (TEA) in methanol both in the ground and the excited states was studied by laser flash photolysis and the pump-probe emission spectroscopy. After the excitation, triplet KP abstracted a hydrogen atom from methanol to form KP ketyl radical (KPH). In the presence of TEA, the acid-base equilibrium state was found to be KP + TEA right arrow over left arrow KP- + TEAH+ in the ground state. The equilibrium constant was determined to be 32 +/- 7. Excited KP- rapidly underwent decarboxylation to form a carbanion resonant with the 3-ethylbenzophenone ketyl biradical anion (3-EBP-), followed by a proton-transfer reaction with TEAH+ to produce the 3-ethylbenzophenone ketyl biradical (3-EBPH). Furthermore, 3-EBPH was found to make a complex with TEA, whose equilibrium constant was obtained to be 18 +/- 2 M(-1). The complex formation ability of 3-EBPH was discussed compared with benzophenone ketyl radical (BPH).

Internal rotational motion of the chloromethyl group of the jet-cooled benzyl chloride molecule.

The mass-resolved resonance enhanced two-photon ionization spectra of jet-cooled benzyl chloride were measured. Some low-frequency vibronic bands around the S1-S0 origin band were assigned to transitions of the internal rotational mode of the chloromethyl group. The internal rotational motion was analyzed by using the one-dimensional free rotor approximation. The conformation in the S1 state was found to be that in which the C-Cl bond lies in orthogonal to the benzene plane. For the species with m/e 126, the transition energy of the internal rotational bands corresponded well to the potential energy values of V2 = 1900 cm(-1) and V4 = 30 cm(-1) in the S1 state and the reduced rotational constant B values 0.50 and 0.47 cm(-1) in the S0 and S1 states, respectively. The B values obtained for the chlorine isotopomer (m/e 128) were slightly different. The S1 potential barrier height was found to be about 3 times larger than that for the S0 state. Molecular orbital calculations suggest that the difference between energies of the HOMO and LUMO with respect to the rotation of the chloromethyl group correspond approximately to the potential energy curve obtained for the S1 state.

Production and excited state dynamics of the photorearranged isomer of benzyl chloride and its methyl derivatives studied by stepwise two-color laser excitation transient absorption and time-resolved thermal lensing techniques.

Production and photoexcited dynamics of reaction intermediates with photolyses of benzyl chloride (BzCl) and methyl-substituted benzyl chlorides (MeBzCls) were studied by using stepwise two-color laser excitation transient absorption (TC-TA) and two-color laser excitation time-resolved thermal lensing (TC-TRTL) measurements. With photoexcitation of BzCl the formation of transient photorearranged isomer was suggested in the previous paper [Res. Chem. Intermed. 2001, 27, 137]. Such an isomer formation for MeBzCls was also observed in a 248 nm excitation. It was found that further photoexcitation of the isomers with the 308 nm light caused photodissociation to yield the corresponding benzyl radicals. The reaction quantum yield and the molar absorptivity of the photorearranged isomer of BzCl were estimated. The heat of reaction for the photodissociation of the isomer was successfully determined with the TC-TRTL measurement. These experimental results were consistent with MO calculations.