The surface science of titanium dioxide - Niser
The surface science of titanium dioxide - Niser
The surface science of titanium dioxide - Niser
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100 U. Diebold / Surface Science Reports 48 (2003) 53±229<br />
Table 4<br />
Comparison <strong>of</strong> calculated <strong>surface</strong> formation energies (J/m 2 ) for relaxed, unreconstructed TiO 2 <strong>surface</strong>s a<br />
Rutile (1 1 0) Anatase<br />
(1 0 1) (1 0 0) (0 0 1) (1 0 3)f (1 0 3)s (1 1 0)<br />
0.31 0.44 0.53 0.90 0.84 0.93 1.09<br />
a Two different structures for the (1 0 3) <strong>surface</strong>s (a `faceted' and a `smooth' one) have been considered. From [216,217].<br />
Interestingly, the average <strong>surface</strong> energy <strong>of</strong> an equilibrium-shape anatase crystal is smaller than the one <strong>of</strong><br />
rutile [216,217], which might explain the fact that nanoscopic TiO 2 particles are less stable in the rutile<br />
phase.<br />
Experimental investigations on single-crystalline anatase are just starting. Meaningful <strong>surface</strong><br />
<strong>science</strong> investigations necessitate single-crystalline samples. While rutile crystals are readily available,<br />
suf®cientlylarge and pure anatase crystals are more dif®cult to obtain. Because anatase is a metastable<br />
phase, it transforms into rutile at relativelylow temperatures [210], with the transition temperature<br />
dependent on impurities, crystal size, sample history, etc. From the recent progress in synthesizing<br />
single-crystalline anatase samples with high purity [209] as well as the successful growth <strong>of</strong> epitaxial<br />
thin-®lms on appropriate substrates [218±221] one can expect a rapid increase in the interest in anatase<br />
TiO 2 in the near future.<br />
2.6.1. Anatase (1 0 1)<br />
Two reports on the structure <strong>of</strong> anatase (1 0 1) <strong>surface</strong>s have appeared veryrecently[220,222]. <strong>The</strong><br />
(1 0 1) <strong>surface</strong> on an anatase sample grown bychemical transport [209] showed a (1 1) <strong>surface</strong> after<br />
mild sputtering and annealing [222]. A mineral sample similar to the one displayed in Fig. 27 was used<br />
in an STM studybyHebenstreit et al. [220]. In order to avoid the contaminations in this natural single<br />
crystal, a 700 AÊ thick, epitaxial ®lm was grown on the <strong>surface</strong>, as described in [221]. Sputtering and<br />
Fig. 27. (a) <strong>The</strong> equilibrium shape <strong>of</strong> a TiO 2 crystal in the anatase phase, according to the Wulff construction and <strong>surface</strong><br />
energies calculated in [216] (from Lazzeri et al. [216], # 2001 <strong>The</strong> American Physical Society). (b) Picture <strong>of</strong> an anatase<br />
mineral crystal.