Designing supramolecular porphyrin arrays that self-organize into nanoscale optical and magnetic materials
- Charles Michael Drain*,†,
- James D. Batteas†,‡,
- George W. Flynn†,§,
- Tatjana Milic*,
- Ning Chi‡,
- Dalia G. Yablon§, and
- Heather Sommers‡
- *Department of Chemistry and Biochemistry, Hunter College and Graduate Center of City University of New York, 695 Park Avenue, New York, NY 10021; ‡Department of Chemistry, College of Staten Island and Graduate Center of City University of New York, 2800 Victory Boulevard, Staten Island, NY 10314; and §Department of Chemistry, Columbia University, 3000 Broadway, MC 3167, New York, NY 10027
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Contributed by George W. Flynn
Abstract
Tessellation of nine free-base porphyrins into a 3 × 3 array is accomplished by the self-assembly of 21 molecular entities of four different kinds, one central, four corner, and four side porphyrins with 12 trans Pd(II) complexes, by specifically designed and targeted intermolecular interactions. Strikingly, the self-assembly of 30 components into a metalloporphyrin nonamer results from the addition of nine equivalents of a first-row transition metal to the above milieu. In this case each porphyrin in the nonameric array coordinates the same metal such as Mn(II), Ni(II), Co(II), or Zn(II). This feat is accomplished by taking advantage of the highly selective porphyrin complexation kinetics and thermodynamics for different metals. In a second, hierarchical self-assembly process, nonspecific intermolecular interactions can be exploited to form nanoscaled three-dimensional aggregates of the supramolecular porphyrin arrays. In solution, the size of the nanoscaled aggregate can be directed by fine-tuning the properties of the component macrocycles, by choice of metalloporphyrin, and the kinetics of the secondary self-assembly process. As precursors to device formation, nanoscale structures of the porphyrin arrays and aggregates of controlled size may be deposited on surfaces. Atomic force microscopy and scanning tunneling microscopy of these materials show that the choice of surface (gold, mica, glass, etc.) may be used to modulate the aggregate size and thus its photophysical properties. Once on the surface the materials are extremely robust.
Footnotes
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↵ † To whom reprint requests may be addressed. E-mail: flynn{at}chem.columbia.edu, cdrain{at}hunter.cuny.edu, or batteas{at}postbox.csi.cuny.edu.
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This paper results from the Arthur M. Sackler Colloquium of the National Academy of Sciences, “Nanoscience: Underlying Physical Concepts and Phenomena,” held May 18–20, 2001, at the National Academy of Sciences in Washington, DC.
- Abbreviation:
- AFM,
- atomic force microscopy
- Copyright © 2002, The National Academy of Sciences





