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Letter
Nature 441, 1122-1125 (29 June 2006) | doi:10.1038/nature04833; Received 3 February 2006; Accepted 24 April 2006
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Professor / Associate Professor (Pharmaceutics / Pharmaceutical Analysis&quality Control)
- Alliance Institute of Advanced Pharmacy and Health Sciences
- Hyderabad 500038 India
Assistant or Associate Professor, Section of Anatomic Pathology
- The Medical College of Georgia
- Augusta, Georgia, USA
Mesostructured germanium with cubic pore symmetry
Gerasimos S. Armatas1 & Mercouri G. Kanatzidis1
- Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
Correspondence to: Mercouri G. Kanatzidis1 Correspondence and requests for materials should be addressed to M.G.K. (Email: kanatzid@cem.msu.edu).
Abstract
Regular mesoporous oxide materials have been widely studied1, 2, 3, 4, 5, 6, 7, 8 and have a range of potential applications, such as catalysis, absorption and separation. They are not generally considered for their optical and electronic properties. Elemental semiconductors with nanopores running through them represent a different form of framework material with physical characteristics contrasting with those of the more conventional bulk, thin film and nanocrystalline forms1. Here we describe cubic mesostructured germanium, MSU-Ge-1, with gyroidal channels containing surfactant molecules, separated by amorphous walls that lie on the gyroid (G) minimal surface as in the mesoporous silica MCM-48 (ref. 2). Although Ge is a high-melting, covalent semiconductor that is difficult to prepare from solution polymerization, we succeeded in assembling a continuous Ge network using a suitable precursor for Ge4- atoms. Our results indicate that elemental semiconductors from group 14 of the periodic table can be made to adopt mesostructured forms such as MSU-Ge-1, which features two three-dimensional labyrinthine tunnels obeying
space group symmetry and separated by a continuous germanium minimal surface that is otherwise amorphous. A consequence of this new structure for germanium, which has walls only one nanometre thick, is a wider electronic energy bandgap (1.4 eV versus 0.66 eV) than has crystalline or amorphous Ge. Controlled oxidation of MSU-Ge-1 creates a range of germanium suboxides with continuously varying Ge:O ratio and a smoothly increasing energy gap.
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