6533b7d1fe1ef96bd125c197
RESEARCH PRODUCT
In situobservation of the formation, diffusion, and reactions of hydrogenous species inF2-laser-irradiatedSiO2glass using a pump-and-probe technique
Koichi KajiharaMasahiro HiranoHideo HosonoLinards SkujaLinards Skujasubject
PhysicsDiffusionDangling bondQuantum yieldCondensed Matter PhysicsLaserElectronic Optical and Magnetic MaterialsAmorphous solidlaw.inventionNonbridging oxygenCrystallographyDistribution functionlawIrradiationdescription
We quantitatively studied the formation, diffusion, and reactions of mobile interstitial hydrogen atoms $({\mathrm{H}}^{0})$ and molecules $({\mathrm{H}}_{2})$ in ${\mathrm{F}}_{2}$-laser-irradiated silica $(\mathrm{Si}{\mathrm{O}}_{2})$ glass between 10 and $330\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. Two key techniques were used: single-pulse ${\mathrm{F}}_{2}$ laser photolysis of silanol (SiOH) groups to selectively create pairs of ${\mathrm{H}}^{0}$ and oxygen dangling bonds (nonbridging oxygen hole centers, NBOHC), and in situ photoluminescence measurements of NBOHCs to monitor their reactions with ${\mathrm{H}}^{0}$ and ${\mathrm{H}}_{2}$ as a function of time and temperature. A smaller quantum yield of the photolysis of the $\mathrm{Si}\mathrm{O}\mathrm{H}$ bond $(0.15\ifmmode\pm\else\textpm\fi{}0.05)$ compared with values reported for gas molecules containing $\mathrm{O}\mathrm{H}$ bonds $(\ensuremath{\sim}1)$ suggests that the separation of photogenerated ${\mathrm{H}}^{0}$ from NBOHC is hindered by the cage effect of the $\mathrm{Si}{\mathrm{O}}_{2}$ glass network. Distribution functions for the diffusion coefficients of ${\mathrm{H}}^{0}$ and ${\mathrm{H}}_{2}$ in the structurally disordered $\mathrm{Si}{\mathrm{O}}_{2}$ glass were evaluated by numerical analysis of the concentration changes of NBOHC based on diffusion-limited reaction theory. The average diffusion coefficient of ${\mathrm{H}}_{2}$ obtained by integrating the distribution agrees well with the values measured by the permeation of ${\mathrm{H}}_{2}$ through $\mathrm{Si}{\mathrm{O}}_{2}$ glass plates. In contrast, the average diffusion coefficient of ${\mathrm{H}}^{0}$ significantly decreases with time because the distribution of the diffusion coefficient of ${\mathrm{H}}^{0}$ is broad and ${\mathrm{H}}^{0}\mathrm{s}$ with greater mobility disappear at a faster rate. We suggest that the efficient conversion of ${\mathrm{H}}^{0}$ into ${\mathrm{H}}_{2}$ in $\mathrm{Si}{\mathrm{O}}_{2}$ glass is due to dissipation of the excess energy of the reaction intermediate via inelastic collisions with the glass network. The fraction of ${\mathrm{H}}^{0}$ that forms ${\mathrm{H}}_{2}$ is determined by the ratio of the capture radii of ${\mathrm{H}}^{0}$ and NBOHC, and it is independent of the diffusion coefficient and the initial concentration of ${\mathrm{H}}^{0}$.
year | journal | country | edition | language |
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2006-09-25 | Physical Review B |