Temperature dependence of intersystem crossing of pyrene

The temperature dependence of the rate constant for intersystem crossing from S₁ of pyrene was determined by means of a method proposed previously. In contrast to the conclusions of Stevens, Thomaz and Jones, and of Kropp, Dawson and Windsor, we conclude that both temperature-independent and temperature-dependent intersystem crossing processes exist. These two processes contribute equally at ≈ 150 K.     

Simultaneous measurements of stress and infrared dichroism on polymers

Summary A method for simultaneous measurements of stress and infrared dichroism as time-dependent behavior of polymer films was devised by using a double beam infrared spectrometer. The film sample held between clamps of a stretching device was placed just in front of the entrance slit of the spectrometer where the sample and reference beams came alternately. Two polarizers were used, one in the sample beam and the other in the reference beam. Thus the sample and reference beams were polarized to have the electric vectors parallel and perpendicular to the stretching direction of the sample, respectively. With this arrangement the spectrometer responded only to the difference in the transmittance of the two beams. Setting the spectrometer at one of the wavenumbers of the absorption band maxima, we could record continuously the change in its dichroism during mechanical treatments which gave rise to the molecular orientation in the sample. The stress was recorded automatically by means of a couple of strain gages pasted on the cantilever beam of the stretching device.By theoretical considerations, a simple relationship was found to exist between the quantity recorded on the spectrometer by this method and the orientation function of transition moment of a vibrational absorption band with respect to the stretching direction.The method was applied to the stress relaxation experiments of vulcanized natural rubber carried out at different elongations less than 600% and at the room temperature. Changes of infrared dichroism were measured for five absorption bands at 1664, 1380, 1361, 1129, and 844 cm^–1, of which the last one is a crystalline band. From the results of this study, it was concluded that the stress relaxation observed was ascribed mainly to the amorphous orientation rather than to the crystalline orientation, which was completed almost immediately after elongation.

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Zusammenfassung Eine Methode für gleichzeitige Messungen von Spannungs-und Infrarot-Dichroismus von Polymerenfolien in AbhÄngigkeit von der Zeit wurde unter Verwendung eines Zweistrahlen-Infrarotspektrometers entwickelt. Die Filmproben, zwischen Klemmen in einer Verstreckungsanordnung gehalten, sind am Ort des Eintrittsspaltes des Spektrometers justiert, an dem der die Probe durchlaufende und der Referenzstrahl alternierend eintreten. Zwei Polarisationen, eine im Probestrahl, die andere im Referenzstrahl, wurden verwendet. So sind der Probe-und Referenzstrahl mit dem elektrischen Vektor parallel bzw. senkrecht zur Streckrichtung der Probe polarisiert. Mit dieser Anordnung am Spektrometer wird nur die Differenz der DurchlÄssigkeit der Probe für beide Strahlen gemessen. Wenn man das Spektrometer auf die Wellenzahl eines Absorptionsmaximums der Probe einstellt, lÄ\t sich also kontinuierlich unmittelbar die Änderung des Dichroismus wÄhrend der mechanischen Verformung verfolgen, die aus molekularer Orientierung in der Probe resultiert. Die Spannung wurde automatisch mit Hilfe von Verlagerungsaufnehmern aufgezeichnet.Theoretische Betrachtungen lassen eine einfache Beziehung zwischen den Spektrometerkurven und der Orientierungsfunktion für die verschiedenen Absorptionsbanden in Bezug auf die Streckrichtung finden.Die Methode wurde auf Spannungsrelaxation in vulkanisiertem Naturkautschuk für verschiedene Strekkungen kleiner als 600% bei Raumtemperatur angewendet. Die Messungen der Änderung des InfrarotDichroismus fanden für die 5 Absorptionsbanden bei 1664, 1380, 1361, 1129 und 844 cm^–1 statt, wobei die letztere eine kristalline Bande ist. Aus den Ergebnissen wird geschlossen, da\ die beobachtete Spannungsrelaxation in der Hauptsache Orientierung im Amorphen und nicht einer Kristallit-Orientierung zuzuordnen ist. Letztere ist offensichtlich schon unmittelbar nach der Streckung fast vollstÄndig ausgebildet.

     

WHAT DOES THE TERM “VIBRONIC COUPLING” MEAN?

Abstract— The term usually referred to as vibronic coupling is discussed. Various adiabatic approximations are exactly defined in an effort to remove the existing ambiguities. The various approaches for improving approximate wavefunctions to obtain more exact wavefunctions are discussed. Transition dipole moments between two vibronic states are evaluated by the different methods, and the mutual relationship among the methods is discussed.     

A study of santonins and their derivatives by mass spectrometry

Fragmentation patterns of santonins and their derivatives under electron impact have been investigated by th use of high resolution mass spectra and a deuterium labelling technique. The relationship between conformation of santonins and their spectra is discussed.     

Morphology modification of TiO<Subscript>2</Subscript> nanotubes by controlling the starting material crystallite size for chemical synthesis

TiO₂ nanotubes (NTs) were prepared by low-temperature chemical synthesis using anatase TiO₂ particles with different crystallite sizes in a NaOH solution followed by water washing and HCl neutralization. The synthesized TiO₂ NTs showed diverse morphologies depending on the starting materials. The crystallite size of TiO₂ raw materials increased with an increase in annealing temperature, and larger TiO₂ NTs, around 31 nm in diameter, were obtained from large raw powder with a crystallite size of 117 nm. X-ray diffraction and Raman spectroscopy revealed that the obtained TiO₂ NT exhibited lower crystallinity; however, Raman vibration seems to be more likely than a rutile structure.     

Structural coupling of an arginine side chain with the oxygen-evolving Mn4Ca cluster in photosystem II as revealed by isotope-edited Fourier transform infrared spectroscopy

Photosynthetic oxygen evolution by plants, algae, and cyanobacteria is performed at the Mn(4)Ca cluster in photosystem II (PSII) by light-driven water oxidation. It has been proposed that CP43-Arg357, which is located in the vicinity of the Mn(4)Ca cluster, plays a key role in the O(2) evolution mechanism; however, direct evidence for its involvement in the reaction has not yet been obtained. In this study, we have for the first time detected the structural coupling of CP43-Arg357 with the Mn(4)Ca cluster by means of isotope-edited Fourier transform infrared (FTIR) spectroscopy. Light-induced FTIR difference spectra upon the S(1)→S(2) transition (S(2)/S(1) difference spectra) of the Mn(4)Ca cluster were measured using isolated PSII core complexes from Synechocystis sp. PCC 6803 cells, where the Arg side chains were labeled with either [η(1,2)-(15)N(2)]Arg or [ζ-(13)C]Arg. Bands due to Arg side chain vibrations, which were extracted by taking a double difference between the S(2)/S(1) spectra of isotope-labeled and unlabeled samples, were found at 1700-1600 and 1700-1550 cm(-1) for [η(1,2)-(15)N(2)]Arg- and [ζ-(13)C]Arg-labeled PSII, respectively. These frequency regions are in good agreement with those of the CN/NH(2) vibrations of a guanidinium group in difference spectra between isotope-labeled and unlabeled Arg in aqueous solutions. The detected Arg bands in the S(2)/S(1) difference spectra were attributed to CP43-Arg357, which is the only Arg residue located near the Mn(4)Ca cluster. The presence of relatively high frequency bands arising from unlabeled Arg suggested that the guanidinium N(η)H(2) is engaged in strong hydrogen bonding. These results indicate that CP43-Arg357 interacts with the Mn(4)Ca cluster probably through direct hydrogen bonding to a first coordination shell ligand of a redox-active Mn ion. This structural coupling of CP43-Arg357 may play a crucial role in the water oxidation reactions.     

Synthesis and charge-transfer chemistry of La2@I(h)-C80/Sc3N@I(h)-C80-zinc porphyrin conjugates: impact of endohedral cluster

Two stable electron donor-acceptor conjugates, that is, 3 and 5b, employing La(2)@I(h)-C(80) and Sc(3)N@I(h)-C(80), on one hand, and zinc tetraphenylporphyrin, on the other hand, have been prepared via [1+2] cycloaddition reactions of a diazo precursor. Combined studies of crystallography and NMR suggest a common (6,6)-open addition pattern of 3 and 5b. Still, subtly different conformations, that is, a restricted and a comparatively more flexible topography, emerge for 3 and 5b, respectively. In line with this aforementioned difference are the electrochemical assays, which imply appreciably stronger I(h)-C(80)/ZnP interactions in 3 when compared to those in 5b. Density functional calculations reveal significant attractions between the two entities of these conjugates, as well as their separately localized HOMOs and LUMOs. The geometrical conformations and LUMO distributions of 3 and 5b, at our applied computational level, are slightly varied with their different endohedral clusters. The clusters also exert different impact on the excited state reactivity of the conjugates. For example, 3 undergoes, upon photoexcitation, a fast charge separation process and yields a radical ion pair, whose nature, namely, (La(2)@C(80))(?-)-(ZnP)(?+)) versus (La(2)@C(80))(?+)-(ZnP)(?-)), varies with solvent polarity. 5b, on the other hand, afforded the same (Sc(3)N@C(80))(?-)-(ZnP)(?+)) radical ion pair regardless of the solvent.     

Where does the metal cation stay in Gd@C2v(9)-C82? A single-crystal X-ray diffraction study

Metal positions in endohedral metallofullerenes (EMFs) are of special importance because their molecular symmetry and intrinsic properties are strongly influenced by the location and motion of the encapsulated metals. X-ray analyses of the cocrystals of Gd@C(2v)(9)-C(82) with nickel(II) octaethylporphyrin [Ni(II)(OEP)] reveal that the Gd(3+) cation is off-center, being located under a hexagonal ring along the 2-fold axis of the C(2v)(9)-C(82) cage. This result is in sharp contrast to that of a previous study, showing that Gd@C(2v)(9)-C(82) has an anomalous endohedral structure, with the metal being positioned over a [6,6] bond, which is opposite to the hexagonal ring along the C(2) axis (Phys. Rev. B 2004, 69, 113412). In agreement with theoretical calculations and related studies, it is conclusive that the single rare-earth metal in M@C(2v)(9)-C(82) always tends to coordinate with the hexagonal ring along the 2-fold axis, instead of interacting with the [6,6] bond on the other end, regardless of the type of metal atom.