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PNNL-13501 - Pacific Northwest National Laboratory

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Removal of the organics (in Figure 3a) by heat treatment<br />

at 450°C will result in crystal growth. However, in the<br />

presence of metal oxide spacer, such as MoO3<br />

(Figure 3b), particle size and architectural features are<br />

stabilized due to interfacial diffusional barriers at the<br />

nanoscale. Figure 4 shows the entropies of<br />

nanoarchitectured materials and nanoparticle mechanical<br />

mixture relative to bulk rutile TiO2 and bulk baddelyite<br />

ZrO2. The two sets of entropy data are similar, and this<br />

indicates that the stability of the nanoarchitectured<br />

materials is due primarily to the presence of diffusion<br />

barriers (see Figure 3b).<br />

(a)<br />

micelle<br />

(b)<br />

Summary and Conclusions<br />

micelle<br />

TiO2 nanocrystal<br />

TiO2 nanocrystal<br />

metal oxide spacer<br />

Figure 3. A cross-section view of nucleation of TiO 2<br />

nanocrystallites at the surface of CTAC micelles: (a) TiO 2<br />

only, (b) with metal oxide spacer<br />

We have synthesized a series of solid-state<br />

nanocrystalline TiO2- (MoO3) core-shell materials from a<br />

novel surfactant micelle assisted reaction pathway. The<br />

structural and optical properties are governed by, and a<br />

direct result of, the intimate nanoarchitectured<br />

arrangement between the TiO2 core and the MoO3 shell.<br />

We also have a fundamental understanding of the reaction<br />

mechanism for the synthesis of nanoarchitectured<br />

materials and the underlying thermodynamics properties<br />

that gives rise to their stability. The TiO2-(MoO3)<br />

compounds are potentially a significant step in the right<br />

direction for understanding how to synthesize and design<br />

advanced metal oxides with fundamentally new physical<br />

and chemical properties.<br />

ent halpy (kJ/mol)<br />

45<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

References<br />

Haus JW, HS Shou, I Honma, and H Komiyama. 1993.<br />

“Quantum confinement in semiconductor heterostructure<br />

nanometer-size particles.” Phys. ReV.B 47, 1359.<br />

Kortan AR, et al. 1990. J. Am. Chem. Soc. 112, 1327.<br />

Elder SH, Y Gao, X Li, J Liu, DE McCready, and<br />

CF Windisch, Jr. 1998. “Zirconia-stabilized 25-Å TiO2<br />

anatase crystallites in a mesoporous structure.” Chem.<br />

Mater. 10, 3140.<br />

Nozik AJ and R Memming. 1996. “Physical chemistry<br />

of semiconductor-liquid interfaces.” J. Phys. Chem. 100,<br />

13061.<br />

Publication<br />

nanoarchitectured materials<br />

(measured)<br />

nanoparticle mechanical<br />

mixture (calculated)<br />

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8<br />

x in xZrO 2 -(1-x)TiO 2<br />

Figure 4. Comparison of entropies of nanoarchitectured<br />

materials and nanoparticle mechanical mixture relative to<br />

bulk rutile TiO 2 and bulk baddelyite ZrO 2<br />

Elder SH, FM Cot, Y Su, SM Heald, AM Tyryshkin,<br />

MK Bowman, Y Gao, AG Joly, ML Balmer,<br />

AC Kolwaite, KA Magrini, and DM Blake. 2000. “The<br />

discovery and study of nanocrystalline TiO2-(MoO3)<br />

core-shell materials.” J. Am. Chem. Soc. 122:5138-5146.<br />

Materials Science and Technology 329

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