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Name (Title):<br />

Norifusa Satoh (Research Associate (Non-tenured))<br />

Affiliation:<br />

Department of Chemistry, Keio University<br />

Address:<br />

3-14-1 Hiyoshi Yokohama 223-8522, Japan<br />

Email: satoh@chem.keio.ac.jp<br />

Home Page: http://www.educ.cc.keio.ac.jp/~kylab/<br />

Presentation Title:<br />

Stepwise metal assembling dendrimers and the application to organic electronics devices and<br />

atom technology for novel metal oxide materials<br />

<strong>Abstract</strong>:<br />

There has never been nanotechnology to<br />

control particle size according to the number of<br />

the component. We succeeded the atomic level<br />

size-control of TiO2 particles (both of rutile and<br />

anatase) with a standard deviation of 0.2 nm,<br />

using fine controlled metal assembly on a<br />

phenylazomethine dendrimer (DPA G4, Fig.<br />

1A) [1].<br />

The number and location of the loaded metal<br />

ions tend to be random within the previous<br />

dendrimers, resulting in a wide distribution of<br />

the templated particle in size. However, the<br />

number and location of metal ions can be finely<br />

controlled in DPA G4 because of the πconjugated<br />

rigid framework. The rigid<br />

framework maintains the desirable dendritic and<br />

cascade structure [2, 3]. It is reflected on the<br />

cascade in the imine basicity on each layer.<br />

Poster Session PM-27<br />

Fig. 1 A. Phenylazomethine dendrimer. B. OLED.<br />

C. DSSC. D. Scheme of Q-size TiO2.<br />

The π-conjugated dendrimers with a triphenylamine core are also useful for the application to<br />

organic electronics devices, such as organic light emitting diodes (OLED, Fig. 1B) and dyesensitized<br />

solar cells (DSSC, Fig. 1C). The electron transfer through the π-conjugated<br />

framework contributes the control of the electron vector, resulting in higher cell performances [2,<br />

3].<br />

The fine size-control using the dendrimer template on substrate (Fig. 1D) revealed the<br />

quantum size effect in TiO2. The energy gap of the obtained particles showed a blue shift as<br />

decreasing in size and a difference in energy between the anatase and rutile forms. The sizedependency<br />

and difference between the crystal forms in bandgap energy is described using a<br />

semi-empirical effective mass approximation [1].<br />

References:<br />

[1] N. Satoh, T. Nakashima, K. Kamikura, K. Yamamoto, Nature Nanotech., 3, 106–111 (2008).<br />

[2] N. Satoh, J.-S. Cho, M. Higuchi, K. Yamamoto, J. Am. Chem. Soc., 125, 8104–8105 (2003).<br />

[3] N. Satoh, T. Nakashima, K. Yamamoto, J. Am. Chem. Soc., 127, 13030–13038 (2005).<br />

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