400 research outputs found
Electron Photodetachment from Aqueous Anions. III. Dynamics of Geminate Pairs Derived from Photoexcitation of Mono- vs. Poly- atomic Anions
Photostimulated electron detachment from aqueous inorganic anions is the
simplest example of solvent-mediated electron transfer. Here we contrast the
behavior of halide anions with that of small polyatomic anions, such as
pseudohalide anions (e.g., HS-) and common polyvalent anions (e.g., SO32-).
Geminate recombination dynamics of hydrated electrons generated by 200 nm
photoexcitation of aqueous anions (I-, Br-, OH-, HS-, CNS-, CO32-, SO32-, and
Fe(CN)64-) have been studied. Prompt quantum yields for the formation of
solvated, thermalized electrons and quantum yields for free electrons were
determined. Pump-probe kinetics for 200 nm photoexcitation were compared with
kinetics obtained at lower photoexcitation energy (225 nm or 242 nm) for the
same anions, where possible. Free diffusion and mean force potential models of
geminate recombination dynamics were used to analyze these kinetics. These
analyses suggest that for polyatomic anions (including all polyvalent anions
studied) the initial electron distribution has a broad component, even at
relatively low photoexcitation energy. There seem to be no well-defined
threshold energy below which the broadening of the distribution does not occur,
as is the case for halide anions. Direct ionization to the conduction band of
water is the most likely photoprocess broadening the electron distribution. Our
study suggests that halide anions are in the class of their own; electron
photodetachment from polyatomic, especially polyvalent, anions follows a
different set of rules.Comment: to be submitted to J. Phys. Chem. A; 28 pages, 5 figs + Supplemen
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New Insights into the Charge-Transfer-to-Solvent Spectrum of Aqueous Iodide: Surface versus Bulk.
Liquid phase charge-transfer-to-solvent (CTTS) transitions are important, as they serve as photochemical routes to solvated electrons. In this work, broadband deep-ultraviolet electronic sum frequency generation (DUV-ESFG) and two-photon absorption (2PA) spectroscopic techniques were used to assign and compare the nature of the aqueous iodide CTTS excitations at the air/water interface and in bulk solution. In the one-photon absorption (1PA) spectrum, excitation to the 6s Rydberg-like orbital (5p → 6s) gives rise to a pair of spin-orbit split iodine states, 2P3/2 and 2P1/2. In the 2PA spectra, the lower-energy 2P3/2 peak is absent and the observed 2PA peak, which is ∼0.14 eV blue-shifted relative to the upper 2P1/2 CTTS peak seen in 1PA, arises from 5p → 6p electronic promotion. The band observed in the ESFG spectrum is attributed to mixing of excited states involving 5p → 6p and 5p → 6s promotions caused by both vibronic coupling and the external electric field generated by asymmetric interfacial solvation
Exploring Redox Properties of Aromatic Amino Acids in Water Contrasting Single Photon vs Resonant Multiphoton Ionization in Aqueous Solutions
Direct measurements of the valence ionization energies and the reorganization energies of the three aromatic amino acids, L Tyrosine, L Tryptophan, and L Phenylalanine in aqueous solution using the liquid microjet technique and two different photoemission methods X ray photoelectron spectroscopy at 180 eV photon energy and resonant two photon ionization using 2 x 267 nm 4.64 eV UV laser light are reported. L Tryptophan has the lowest vertical ionization energy, 7.3 eV, followed by Tyrosine 7.8 eV and Phenylalanine 8.7 eV . Essentially, no variation in recovered orbital energies is observed comparing near threshold ionization to X ray ionization. Superior sensitivity of the background free R2PI scheme for solutions with very low solute concentration lt;2 millimolar is demonstrated in contrast to the single photon XPS measurements, which often requires solute concentrations of 0.1 to 1 molar. This higher sensitivity along with chemical selectivity of the R2PI technique can be exploited for both spectroscopic assignment and as an analytical tool. The nature of the adiabatic ionization energy for the three aromatic amino acids has been explored by the R2PI approach and by empirically formulating the correlation between the estimated ionization onset with electronic and nuclear relaxation on the excited state surface. Our results have implications for understanding one electron transfer within enzymes and in redox situations where ir reversible deprotonation occur such as those manifest in the biochemistry of oxidation damag
Exploring the energy disposal immediately after bond-breaking in solution:the wavelength-dependent excited state dissociation pathways of para-methylthiophenol
Excited state dynamics of liquid water: Insight from the dissociation reaction following two-photon excitation
We use transient absorption spectroscopy to monitor the ionization and dissociation products following two-photon excitation of pure liquid water. The two decay mechanisms occur with similar yield for an excitation energy of 9.3 eV, whereas the major channel at 8.3 eV is dissociation. The geminate recombination kinetics of the H and OH fragments, which can be followed in the transient absorption probed at 267 nm, provide a window on the dissociation dynamics at the lower excitation energy. Modeling the OH geminate recombination indicates that the dissociating H atoms have enough kinetic energy to escape the solvent cage and one or two additional solvent shells. The average initial separation of H and OH fragments is 0.7+-0.2 nm. Our observation suggests that the hydrogen bonding environment does not prevent direct dissociation of an O-H bond in the excited state. We discuss the implications of our measurement for the excited state dynamics of liquid water and explore the role of those dynamics in the ionization mechanism at low excitation energies
Chasing charge localization and chemical reactivity following photoionization in liquid water
The ultrafast dynamics of the cationic hole formed in bulk liquid water following ionization is investigated by ab initio molecular dynamics simulations and an experimentally accessible signature is suggested that might be tracked by femtosecond pump-probe spectroscopy. This is one of the fastest fundamental processes occurring in radiation-induced chemistry in aqueous systems and biological tissue. However, unlike the excess electron formed in the same process, the nature and time evolution of the cationic hole has been hitherto little studied. Simulations show that an initially partially delocalized cationic hole localizes within similar to 30 fs after which proton transfer to a neighboring water molecule proceeds practically immediately, leading to the formation of the OH radical and the hydronium cation in a reaction which can be formally written as H(2)O(+) + H(2)O -> OH + H(3)O(+). The exact amount of initial spin delocalization is, however, somewhat method dependent, being realistically described by approximate density functional theory methods corrected for the self-interaction error. Localization, and then the evolving separation of spin and charge, changes the electronic structure of the radical center. This is manifested in the spectrum of electronic excitations which is calculated for the ensemble of ab initio molecular dynamics trajectories using a quantum mechanics/molecular mechanics (QM/MM) formalism applying the equation of motion coupled-clusters method to the radical core. A clear spectroscopic signature is predicted by the theoretical model: as the hole transforms into a hydroxyl radical, a transient electronic absorption in the visible shifts to the blue, growing toward the near ultraviolet. Experimental evidence for this primary radiation-induced process is sought using femtosecond photoionization of liquid water excited with two photons at 11 eV. Transient absorption measurements carried out with similar to 40 fs time resolution and broadband spectral probing across the near-UV and visible are presented and direct comparisons with the theoretical simulations are made. Within the sensitivity and time resolution of the current measurement, a matching spectral signature is not detected. This result is used to place an upper limit on the absorption strength and/or lifetime of the localized H(2)O((aq))(+) species. (C) 2011 American Institute of Physics. doi:10.1063/1.3664746
Exploring autoionization and photo-induced proton-coupled electron transfer pathways of phenol in aqueous solution
The excited state dynamics of phenol
in water have been investigated
using transient absorption spectroscopy. Solvated electrons and vibrationally
cold phenoxyl radicals are observed upon 200 and 267 nm excitation,
but with formation time scales that differ by more than 4 orders of
magnitude. The impact of these findings is assessed in terms of the
relative importance of autoionization versus proton-coupled electron
transfer mechanisms in this computationally tractable model system
Vibronic Structure in Room Temperature Photoluminescence of the Halide Perovskite Cs3Bi2Br9
We report a study on the optical properties of the layered polymorph of vacancy-ordered triple perovskite Cs3Bi2Br9. The electronic structure, determined from density functional theory calculations, shows the top of the valence band and bottom of the conduction band minima are, unusually, dominated by Bi s and p states, respectively. This produces a sharp exciton peak in the absorption spectra with a binding energy that was approximated to be 940 meV, which is substantially stronger than values found in other halide perovskites and, instead, more closely reflects values seen in alkali halide crystals. This large binding energy is indicative of a strongly localized character and results in a highly structured emission at room temperature as the exciton couples to vibrations in the lattice
Lanthanum fluoride nanoparticles for radiosensitization of tumors
Dense inorganic nanoparticles have recently been identified as promising radiosensitizers. In addition to dose enhancement through increased attenuation of ionizing radiation relative to biological tissue, scintillating nanoparticles can transfer energy to coupled photosensitizers to amplify production of reactive oxygen species, as well as provide UVvisible emission for optical imaging. Lanthanum fluoride is a transparent material that is easily prepared as nanocrystals, and which can provide radioluminescence at a number of wavelengths through simple substitution of lanthanum ions with other luminescent lanthanides. We have prepared lanthanum fluoride nanoparticles doped with cerium, terbium, or both, that have good spectral overlap with chlorine6 or Rose Bengal photosensitizer molecules. We have also developed a strategy for stable conjugation of the photosensitizers to the nanoparticle surface, allowing for high energy transfer efficiencies on a per molecule basis. Additionally, we have succeeded in making our conjugates colloidally stable under physiological conditions. Here we present our latest results, using nanoparticles and nanoparticle-photosensitizer conjugates to demonstrate radiation dose enhancement in B16 melanoma cells. The effects of nanoparticle treatment prior to 250 kVp x-ray irradiation were investigated through clonogenic survival assays and cell cycle analysis. Using a custom apparatus, we have also observed scintillation of the nanoparticles and conjugates under the same conditions that the cell samples are irradiated
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