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Eighth Condensed Phase and Interfacial Molecular Science (CPIMS)

Eighth Condensed Phase and Interfacial Molecular Science (CPIMS)

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Integrated O 2 PSD (ML)<br />

Integrated O 2 PSD (ML)<br />

0.1<br />

0.08<br />

0.06<br />

0.04<br />

0.02<br />

0<br />

0.06<br />

0.05<br />

0.04<br />

0.03<br />

0.02<br />

0.01<br />

a)<br />

b)<br />

18 O2<br />

16 O 18 O<br />

16 O2 (x 0.2)<br />

0<br />

0 100 200 300 400 500 600<br />

T<br />

anneal<br />

Figure 1: Integrated O2 PSD yields versus annealing<br />

temperature, Tanneal. 18 O2 was deposited at 30 K<br />

<strong>and</strong> annealed. Then physisorbed 16 O2 was<br />

deposited <strong>and</strong> the system was irradiated with<br />

UV light while the desorption of the O2 isotopes<br />

was monitored with a mass spectrometer.<br />

11 th -20 th cycle:<br />

Physisorb 18 O<br />

2<br />

Figure 1 shows the time-integrated 16 O2,<br />

18 O2, <strong>and</strong> 16 O 18 O photon-stimulated desorption<br />

(PSD) yields versus annealing temperature, Tanneal,<br />

of chemisorbed oxygen. 18 O2 was adsorbed at 30 K<br />

<strong>and</strong> annealed at Tanneal for 240 s. Then 0.4 ML 16 O2<br />

was adsorbed <strong>and</strong> the sample was irradiated (both<br />

at 30 K). The 16 O 18 O PSD signal results from<br />

photon-stimulated reactions involving the exchange<br />

of atoms between the chemisorbed oxygen <strong>and</strong><br />

physisorbed O2. The 18 O2 PSD yield decreases approximately monotonically as Tanneal increases <strong>and</strong> is<br />

essentially zero above 400 K (Fig. 1a, red triangles). The 16 O2 PSD yield is nearly independent of Tanneal<br />

(Fig. 1a, blue squares). In contrast, the 16 O 18 O PSD yield initially increases with increasing annealing<br />

temperature, goes through a maximum at Tanneal ~ 375 K, <strong>and</strong> then rapidly drops to zero for high<br />

temperatures (Fig. 1b, black circles). Annealing above ~400 K brings Ti interstitials to the surface that<br />

react with the adsorbed oxygen to form TiOx isl<strong>and</strong>s, resulting in the observed decrease in the 16 O2 <strong>and</strong><br />

16 O 18 O PSD yields. The results in Figure 1 suggest that annealing TiO2(110) with adsorbed oxygen leads<br />

to the creation of a distinct, stable species on the surface, <strong>and</strong> changes in the angular distribution of the<br />

desorbing oxygen versus Tanneal support this hypothesis (data not shown).<br />

Remarkably, the chemisorbed oxygen species responsible for the photon-stimulated exchange<br />

reactions is not destroyed by repeated cycles of UV irradiation. Figure 2 shows the 16 O 18 O PSD signals<br />

versus time for an experiment with repeated UV irradiations. For this experiment, 18 O2 was annealed at<br />

350 K. The sample was subsequently dosed with physisorbed 16 O2 at 30 K <strong>and</strong> irradiated with UV light.<br />

The black trace in the upper left corner of Figure 2 (labeled “1 st ”) shows the 16 O 18 O PSD versus time for<br />

the first irradiation. This was followed by nine more cycles where the sample was heated to 100 K (to<br />

desorb any remaining physisorbed O2), dosed with 16 O2 <strong>and</strong> UV irradiated. The red <strong>and</strong> blue traces on the<br />

left side of Figure 2 show the 16 O 18 O PSD signals for the third <strong>and</strong> tenth irradiation cycles, respectively.<br />

By the tenth irradiation cycle, the 16 O 18 O PSD is essentially zero. Following the first ten UV irradiation<br />

116<br />

16 O 18 O PSD Signal (arb. units)<br />

1 st -10 th cycle:<br />

Physisorb 16 a)<br />

O<br />

2<br />

1 st<br />

3 rd<br />

10 th<br />

11 th<br />

13 th<br />

20 th<br />

Integrated 16 O 18 O PSD (ML)<br />

0 50 100 150 0 50 100 150<br />

time (s)<br />

Figure 2: 16 O 18 O PSD signals versus time for<br />

repeated UV irradiations. See text for details.

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