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Vibrational energy relaxation of azulene studied by the transient grating method. II. Liquid solvents.

The vibrational energy dissipation process of the ground-state azulene in various liquids has been studied by the transient grating spectroscopy. The acoustic signal produced by the temperature rise of the solvent due to the vibrational energy relaxation of azulene was monitored. The temperature rise-time constant of the solvent has been determined both by the fitting of the acoustic signal to a theoretical model equation and by the analysis of the acoustic peak shift. We found that the temperature rise-time constants determined by the transient grating method in various solvents are larger than the vibrational energy relaxation time constants determined by the transient absorption measurement [D. Schwarzer, J. Troe, M. Votsmeier, and M. Zerezke, J. Chem. Phys. 105, 3121 (1996)]. The difference is explained by different energy dissipation pathways from azulene to solvent; vibrational-vibrational (V-V) energy transfer and vibrational-translational (V-T) energy transfer. The contribution of the V-V energy transfer is estimated in various liquid solvents from the difference between the temperature rise time and vibrational energy relaxation time, and the solvent V-T relaxation time.

Journal Article↗

Reaction coordinate analysis of the S1-S0 internal conversion of azulene.

The reaction coordinate of the S(1)-S(0) internal conversion of azulene has been analyzed using ab initio complete active space self-consistent field method. The stable geometry in S(0) (S(0) geometry) takes a bond-equalized structure where all the peripheral skeletal bond distances are similar to an aromatic CC bond distance. The transannular bond is similar to a normal C-C single bond. The first event upon electronic excitation into S(1) at S(0) geometry is characterized by the following two simultaneous changes in the skeletal bonds; the transannular bond in S(1) increases its double bond character and the aromaticity of the peripheral bonds disappears. In consequence, the most stable azulene in S(1) (S(1) geometry) has a biradical character. To reach the conical intersection between S(1) and S(0) (S(1)S(0)-CIX) where radiationless relaxation takes place, the seven-membered ring greatly deviates from a planar structure. After a transition into S(0) at S(1)S(0)-CIX, the bond-equalized structure is recovered immediately and then the nonplanarity decreases so that azulene again takes the stable planar S(0) geometry. In order to deepen the understanding of the S(1)-S(0) internal conversion, the dipole moments along the reaction coordinate have been analyzed.

Journal Article↗

Substituent constants of azulene.

The ionization constants in water for six 3-substituted azuloic acids were determined spectrophotometrically. Conversion of these physical constants to their pKa values allowed a set of Hammett-type sigma values for the substituents on these acids to be calculated. Determination of partition coefficients for nine 1-substituted azulenes allowed Hansch-type pi values to be determined, using azulene as the model compound.

Azulenes↗

Van der Waals complexes of polar aromatic molecules: unexpected structures for dimers of azulene.

Full geometry optimizations at the dispersion corrected DFT-BLYP/TZV2P level of theory have been performed for dimers of azulene that may serve as a model system for the van der Waals complexes of polar pi systems. The structures and binding energies for 11 dimers are investigated in detail. The DFT-D interaction energies have been successfully checked against results from the accurate SCS-MP2/aug-cc-pVTZ approach. Out of the nine investigated stacked complexes, eight have binding energies larger than 7.4 kcal/mol (SCS-MP2) that exceed the value of 7.1 kcal/mol for the best naphthalene dimer. T-shaped arrangements (CH...pi) are significantly less stable. Two out of the three best structures have an antiparallel alignment of the monomer dipole moments in the complex, although the best ones with a parallel orientation are only about 0.5 kcal/mol less strongly bound which points to a minor importance of dipole-dipole interactions to binding. Quite surprisingly, the energetically lowest structure (DeltaE = -9.2 kcal/mol) corresponds to a situation where the two seven-membered rings are located almost on top of each other (7-7) and the long molecular axes are rotated against each other by 130 degrees. The 7-7 structural motif is found also in other energetically low-lying structures, and the expected 5-7 (two-side) arrangement is less strongly bound by about 2 kcal/mol. This can be explained by the electrostatic potential of azulene that only partially reflects the charge separation according to the common 4n + 2 pi electron rule. General rules for predicting stable van der Waals complexes of polar pi systems are discussed.

Azulenes↗

Ab initio and RRKM study of photodissociation of azulene cation.

The ab initio/Rice-Ramsperger-Kassel-Marcus (RRKM) approach has been applied to investigate the photodissociation mechanism of the azulene cation at different values of the photon energy. Reaction pathways leading to various decomposition products have been mapped out at the G3(MP2,CC)//B3LYP level and then the RRKM and microcanonical variational transition state theories have been applied to compute rate constants for individual reaction steps. Relative product yields (branching ratios) for the dissociation products have been calculated using the steady-state approach. The results show that a photoexcited azulene cation can readily isomerize to a naphthalene cation. The major dissociation channels are elimination of atomic hydrogen, an H2 molecule, and acetylene. The branching ratio of the H elimination channel decreases with an increase of the photon energy. The branching ratio of the acetylene elimination as well as that of the H2 elimination rise as the photon energy increases. The main C8H6+ fragment at all photon energies considered is a pentalene cation, and its yield decreases slightly with increasing excitation energy, whereas the branching ratios of the other C8H6+ fragments, phenylacetylene and benzocyclobutadiene cations, grow.

Azulenes↗

Cytotoxic activity of azulenes against human oral tumor cell lines.

We investigated 27 azulene derivatives for their relative cytotoxicity against three human normal cells and three human oral tumor cell lines. 2-Acetylaminoazulene [4], diethyl 2-chlorozulene-1,3-dicarboxylate [9] and methyl 7-isopropyl-2-methoxyazulene-1-carboxylate [24] showed higher tumor-specific cytotoxicity than azulene [1] and guaiazulene [2]. Four 1- and 3-halogenated compounds showed lower tumor specificity. The tumor-specific cytotoxic activity seems not to be related to the position of functional groups. All compounds showed no anti-HIV activity. Methyl 7-isopropyl-2-methoxyazulene-1-carboxylate [24] induced apoptotic cell death (characterized by internucleosomal DNA fragmentation and caspase 3 activation) in HL-60 cells. ESR spectroscopy showed that methyl 7-isopropyl-2-methoxyazulene-1-carboxylate [24] did not produce radical and less efficiently scavenged O2- (generated by HX-XOD reaction) and NO (generated from NOC-7). These data suggest that a radical-mediated oxidation mechanism may not be involved in the apoptosis induction by methyl 7-isopropyl-2-methoxyazulene-1-carboxylate [24].

Anti-Inflammatory Agents, Non-Steroidal↗

HNS-32, a novel azulene-1-carboxamidine derivative, inhibits nifedipine-sensitive and -insensitive contraction of the isolated rabbit aorta.

The vasorelaxant profile of a novel azulene-1-carboxamidine derivative, HNS-32 [N1,N1-dimethyl-N2-(2-pyridylmethyl)-5-isopropyl-3,8-dimethyl-azulene-1-carboxamidine, CAS 186086-10-2], was investigated in the isolated rabbit aorta precontracted with high KCl, noradrenaline (NA) or phorbol 12, 13-dibutyrate (PDBu) and compared with those of nifedipine and nitroglycerin. In preparations without endothelium, HNS-32 elicited concentration-dependent, full inhibition of contractions elicited by high KCI (80 mM), NA (3x10(-6) M) or PDBu (10(-6) M). In contrast, nifedipine inhibited only the contraction elicited by membrane depolarization with high KCl. Nitroglycerin also attenuated high-KCl-, NA- and PDBu-elicited contractions effectively, although full suppression was obtained only for NA-elicited contraction. Whilst the relaxant effect of HNS-32 was not affected by the presence of endothelium, the relaxant response to acetylcholine was endothelium dependent. Addition of excess Ca2+ restored both the HNS-32-reduced tension in muscle precontracted with high KCI and the nifedipine-mediated tension decrease. Relaxation elicited by HNS-32 was not affected by the adenylate cyclase inhibitor, 9-(tetrahydro-2'-furyl)adenine (SQ 22,536, 10(-4) M), the soluble guanylate cyclase inhibitor, 1H-(1,2,4)-oxadiazolo-(4,3-a)-quinoxalin-1-one (ODQ, 10(-5) M) or a cocktail of K+ channel blockers (glybenclamide 10(-6) M, tetraethylammonium 2x10(-3) M, apamin 10(-7) M, 4-aminopyridine 10(-4) M and Ba2+ 10(-5) M). These findings indicate that HNS-32 inhibits both L-type Ca2+ channel-dependent and -independent vascular contraction. Blockade of Ca2+ entry through L-type Ca2+ channels may be involved in the inhibitory effect of HNS-32 on the contraction due to membrane depolarization with high KCl. On the other hand, HNS-32 seems to inhibit Ca2+ channel-independent contraction via mechanism(s) other than elevation of cyclic nucleotides (cAMP and cGMP) and opening of K+ channels.

Animals↗

Fulvenes, fulvalenes, and azulene: are they aromatic chameleons?

On the basis of the theory of Baird on reversal of Hückel's rule for aromaticity and antiaromaticity of annulenes when going from the electronic ground state (S0) to the lowest pipi* triplet state (T1) (J. Am. Chem. Soc. 1972, 94, 4941), we argue that fulvenes, fulvalenes, and azulene are "aromatic chameleons". The dipole moments of fulvenes in T1 should be of comparable magnitude to those of S0, but due to the reversal of Hückel's aromaticity rule in T1, their dipole should be in the opposite direction. Thereby, they are capable of adopting some aromaticity in both the T1 and S0 states as they adapt their dipolar resonance structures. The same applies to fulvalenes and azulene in their lowest quintet states (Q1) when compared to S0. Our hypothesis on chameleon behavior is supported by quantum chemical OLYP, CASSCF, and CASPT2 calculations of dipole moments, pi-orbital populations, and energies.

Journal Article↗

Calix[4]azulene.

Azulene reacts with paraformaldehyde in the presence of florisil to give excellent yields of calix[4]azulene.

Journal Article↗

Photodissociation of azulene at 193 nm: ab initio and RRKM study.

The ab initio/Rice-Ramsperger-Kassel-Marcus (RRKM) approach has been applied to investigate the photodissociation mechanism of azulene at 6.4 eV (the laser wavelength of 193 nm) upon absorption of one UV photon followed by internal conversion into the ground electronic state. Reaction pathways leading to various decomposition products have been mapped out at the G3(MP2,CC)//B3LYP level and then the RRKM and microcanonical variational transition state theories have been applied to compute rate constants for individual reaction steps. Relative product yields (branching ratios) for the dissociation products have been calculated using the steady-state approach. The results show that photoexcited azulene can readily isomerize to naphthalene and the major dissociation channel is elimination of an H-atom from naphthalene. The branching ratio of this channel decreases with an increase of the photon energy. Acetylene elimination is the second probable reaction channel and its branching ratio rises as the photon energy increases. The main C8H6 fragments at 193 nm are phenylacetylene and pentalene and the yield of the latter grows fast with the increasing excitation energy.

Journal Article↗

Energy transfer between polyatomic molecules II: Energy transfer quantities and probability density functions in benzene, toluene, p-xylene, and azulene collisions.

Collisional energy transfer, CET, is of major importance in chemical, photochemical, and photophysical processes in the gas phase. In Paper I of this series (J. Phys. Chem. B 2005, 109, 8310) we have reported on the mechanism and quantities of CET between an excited benzene and cold benzene and Ar bath. In the present work, we report on CET between excited toluene, p-xylene, and azulene with cold benzene and Ar and on CET of excited benzene with cold toluene, p-xylene, and azulene. We compare our results with those of Paper I and report average vibrational, rotational, and translational energy quantities, , transferred in a single collision. We discuss the effect of internal rotation on CET and the identity of the gateway modes in CET and the relative role of vibrational, rotational, and translational energies in the CET process, all that as a function of temperature and excitation energy. Energy transfer probability density functions, P(E,E'), for the various systems are reported and the shape of the curves for various systems and initial conditions is discussed. The major findings for polyatomic-polyatomic collisions are: CET takes place mainly via vibration-to-vibration energy transfer assisted by overall rotations. Internal free rotors in the excited molecule hinder energy exchange while in the bath molecule they do not. Energy transfer at low temperatures and high temperatures is more efficient than that at intermediate temperatures. Low-frequency modes are the gateway modes for energy transfer. Vibrational temperatures affect energy transfer. The CET probability density function, P(E,E'), is convex at low temperatures and can be concave at high temperatures. A mechanism that explains the high values of and the convex shape of P(E,E') is that in addition to short impulsive collisions there are chattering collisions where energy is transferred in a sequence of short encounters during the lifetime of the collision complex. This also leads to the observed supercollision tail at the down wing of P(E,E'). Polyatomic-Ar collisions show mechanistic similarities to polyatomic-polyatomic collisions, but there are also many dissimilarities: internal rotations do not inhibit energy transfer, P(E,E') is concave at all temperatures, and there is no contribution of chattering collisions.

Journal Article↗

Correlation of substituent effects and energy levels of the two lowest excited states of the azulenic chromophore

[structure: see text] Experimental and calculated data show that the relative energy levels of the two lowest excited states of azulene are sensitive to the nature and position of substituents on the nonalternant hydrocarbon. Extending such investigations led to a rational explanation for some of the baffling data on azulenic bacteriorhodopsin analogues in the literature.

Journal Article↗

Energy transfer between azulene and krypton: comparison between experiment and computation.

Trajectory calculations of collisional energy transfer between excited azulene and Kr are reported, and the results are compared with recent crossed molecular beam experiments by Liu et al. [J. Chem. Phys. 123, 131102 (2005); 124, 054302 (2006)]. Average energy transfer quantities are reported and compared with results obtained before for azulene-Ar collisions. A collisional energy transfer probability density function P(E,E'), calculated at identical initial conditions as experiments, shows a peak at the up-collision branch of P(E,E') at low initial relative translational energy. This peak is absent at higher relative translational energies. There is a supercollision tail at the down-collision side of the probability distribution. Various intermolecular potentials are used and compared. There is broad agreement between experiment and computation, but there are some differences as well.

Journal Article↗

The nature of the delocalized cations in azulenic bacteriorhodopsin analogs.

Depending on the size and shape of their azulenic chromophores, azulenic bacteriorhodopsin (bR) pigment analogs can exist as either an initial pigment P1, a more red-shifted final pigment P2 or an equilibrium mixture of both. The absorption spectra of red-shifted bR analogs exhibit characteristic narrow-band shapes similar to charge fully delocalized cyanine-like dyes. Therefore, all such red-shifted pigments are believed to be highly delocalized, bond-equalized carbocations. We have determined structural requirements that facilitate their formation. To describe fully the red-shift potentials of these retinal analogs, we have introduced a new parameter-percent red-shift (PRS). A large PRS value not only reflects the extent of red-shift, but is also suggestive of extensive delocalization of the positive charge. Relevance of these findings in consideration of the possibility of forming stable O-intermediates is presented. The postulated resonance hybrid-like structures for different cations of the positively charged protonated Schiff base chromophores are in fact structurally distinct species, equilibrating in response to local perturbations within the supramolecular protein environment.

Bacteriorhodopsins↗

Cardiovascular and antiarrhythmic effects of the azulene-1-carboxamidine derivative N1,N1-dimethyl-N2-(2-pyridylmethyl)-5-isopropyl-3, 8-dimethylazulene-1-carboxamidine.

The azulene-1-carboxamidine derivative N1,N1-Dimethyl-N2-(2- pyridylmethyl)-5-isopropyl-3,8-dimethyl-azulene-1-carboxamidine (CAS 186086-10-2, HNS-32) is a newly synthesized compound. In the present study, direct cardiovascular effects of HNS-32 were assessed using the canine isolated, blood-perfused sinoatrial node, papillary muscle and atrioventricular node preparations, while the antiarrhythmic action was examined using the canine two-stage coronary ligation-induced arrhythmia model. Intracoronary administration of HNS-32 (1-300 micrograms) suppressed the sinus nodal automaticity and ventricular contractile force, while it increased the atrio-His and His-ventricular conduction time as well as the coronary blood flow. Intravenous administration of HNS-32 (5 mg/kg) suppressed the ventricular arrhythmia for approximately 30 min. Since HNS-32 possesses multiple cardiac direct effects which are unique compared with well-established antiarrhythmic drugs, it may become a leading compound in the search for novel antiarrhythmic agents.

Animals↗

Kinetic study of the malonaldehyde-azulene reaction determination of malonaldehyde in human plasma.

The influence of physicochemical conditions in the formation of derivatized malonaldehyde (MLD)-azulene was studied, and kinetic and conventional spectrophotometric data were compared. Conventional and kinetic spectrophotometric procedures were used to study inference of several compounds. An advantageous kinetic method was used to determine MLD in human plasma. The proposed method is faster than the thiobarbituric acid (TBA) method, because 150 s is sufficient to develop the reaction and the kinetic measurements. A comparative study of the results obtained using the proposed kinetic method and those reported in the literature for MLD determination by using the TBA reaction is presented.

Azulenes↗

Azulene derivatives as TXA2/PGH2 receptor antagonists--II. Synthesis and biological activity of 6-mono- and 6-dihydroxylated-isopropylazulenes.

In order to examine the correlation between activity and hydrophilicity of the side chain of sodium 3-[4-(4-chlorobenzenesulfonylamino)butyl]-6-isopropylazulene -1-sulfonate (KT2-962), a non-prostanoid TXA2/PGH2 receptor antagonist, one or two hydroxyl groups were introduced into the isopropyl moiety. A series of 6-hydroxylated-isopropylazulenes were synthesized by regioselective oxidation of 6-isopropylazulenes and their in vitro and in vivo antagonistic activities were studied. Both the primary and tertiary alcohols, monohydroxylated derivatives, exhibited potent biological activities comparable to unmodified 6-isopropylazulenes both in vitro and in vivo. In contrast, the activities of 1,2- and 1,3-diols of 6-substituted derivatives, markedly decreased, but recovered by O-isopropylidenation of the dihydroxyl moiety. These findings indicate that the moderate hydrophobicity of substituent at the 6-position of the azulene ring might be required for the activity and the size of the substituent at this position, not so rigid for keeping potent biological activity.

15-Hydroxy-11 alpha,9 alpha-(epoxymethano)prosta-5↗