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Eighth Condensed Phase and Interfacial Molecular Science (CPIMS)

Eighth Condensed Phase and Interfacial Molecular Science (CPIMS)

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increasing propanol coverage, the TiO2-related TPD peaks were occupied before the appearance<br />

of any Au(111)-related peaks, which indicate sufficient mobility of 2-propanol<br />

molecules on both Au(111) <strong>and</strong> nano-TiO2 surfaces below 270 K. Our calculations <strong>and</strong><br />

experimental measurements showed that in comparison with rutile(110), the nano-<br />

TiO2/Au(111) surface shows higher reactivity both in terms of the fraction of reactive<br />

sites <strong>and</strong> in terms of lower reaction barrier. Also the desorption temperatures of products<br />

from supported TiO2 nanocrystals were shown to depend strongly on the morphology of<br />

the nanocrystals.<br />

The experimental observations made as a result of our work are as follows: (1)<br />

propanol completely fills adsorption sites on TiO2 nanocrystals before filling Au(111)<br />

sites; the local adsorption site density of the nanocrystals is 0.4 ML; (2) almost ½ of propanol<br />

molecules adsorbed on TiO2 nanocrystals desorb at ~310 K, exhibiting behavior,<br />

which is identical to propanol adsorbed on the Ti (5) atoms of rutile(110) surface; (3) more<br />

than ¼ of propanol molecules undergo chemical reactions either of dehydration to form<br />

propene or, in smaller part, dehydrogenation to form acetone. Some sites on TiO2<br />

nanocrystals show almost 40 kJ/mol reduction in the reaction barrier for propene formation<br />

compared to BBOv on rutile(110), while acetone is not produced on rutile(110).<br />

Thus, in comparison with rutile(110), the nano-TiO2/Au(111) surface shows higher reactivity<br />

both in terms of the fraction of reactive sites <strong>and</strong> of reaction barrier.<br />

STM Tip-Induced Dissociation Dynamics on Surfaces.<br />

Scanning tunneling microscopy offers a unique ap-<br />

proach to exploration of molecular dissociation dynamics<br />

at an atomic scale. Namely, as shown by the<br />

W. Ho Group, an STM allows injection of an electron<br />

or electrons with a specified energy into a selected<br />

molecule in a specific adsorption configuration. Initial<br />

studies of this approach have been carried out in<br />

the Palmer <strong>and</strong> Polanyi Groups for reactions on semiconductor<br />

surfaces <strong>and</strong> shown to yield dynamical information<br />

on the chargetransfer<br />

threshold electron<br />

energy for a specific reaction,<br />

the identity of<br />

adsorbate states suitable for<br />

dissociation, fragment trajectories<br />

across the surface<br />

following bond scission,<br />

Fig. 4: Cartoon showing<br />

the change in 2chloroanthracenefollowing<br />

tip-induced e reaction.<br />

The green atom is<br />

the remaining Cl.<br />

nano-TiO 2 /Au(111)<br />

propanol<br />

propene<br />

acetone<br />

100 200 300 400 500 600 700 800<br />

Temperature, K<br />

<strong>and</strong> the nature <strong>and</strong> sensitivity to the adsorption geometry of the<br />

products. Note that for photocatalysis, the electron-induced reaction<br />

similarly involves charge transfer from the bulk of a<br />

substrate to an adsorbed molecule followed by bond cleavage.<br />

Such a study thus tries to answer the same fundamental chemical<br />

physics questions as in gas phase reaction dynamics except<br />

that on a surface determine the role of the surface perturbation<br />

on the half-collision event <strong>and</strong> fragments.<br />

141<br />

M .S. s ignal, a.u.<br />

ML<br />

0.3<br />

0.2<br />

0.1<br />

0.0<br />

2-propanol<br />

(tail)<br />

Fig. 3. TPD spectrum from a nano-<br />

TiO 2/Au(111) surface having 0.1<br />

ML of 2-propanol coverage. The<br />

inserts show the calculated distribution<br />

of the desorption products.<br />

p r op e ne<br />

a c et on e

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