Resonating Valence-Bond Ground State in a Phenalenyl-Based Neutral Radical Conductor

An organic material composed of neutral free radicals based on the spirobiphenalenyl system exhibits a room temperature conductivity of 0.3 siemens per centimeter and a high-symmetry crystal structure. It displays the temperature-independent Pauli paramagnetism characteristic of a metal with a magnetic susceptibility that implies a density of states at the Fermi level of 15.5 states per electron volt per mole. Extended Hückel calculations indicate that the solid is a three-dimensional organic metal with a band width of ∼0.5 electron volts. However, the compound shows activated conductivity (activation energy, 0.054 electron volts) and an optical energy gap of 0.34 electron volts. We argue that these apparently contradictory properties are best resolved in terms of the resonating valence-bond ground state originally suggested by Pauling, but with the modifications introduced by Anderson.

[1]  B. Powell,et al.  Half-filled layered organic superconductors and the resonating-valence-bond theory of the hubbard-heisenberg model. , 2005, Physical review letters.

[2]  T. Takui,et al.  A purely organic molecular metal based on a hydrogen-bonded charge-transfer complex: crystal structure and electronic properties of TTF-imidazole-p-chloranil. , 2004, Angewandte Chemie.

[3]  David W. Small,et al.  Intermolecular pi-to-pi bonding between stacked aromatic dyads. Experimental and theoretical binding energies and near-IR optical transitions for phenalenyl radical/radical versus radical/cation dimerizations. , 2004, Journal of the American Chemical Society.

[4]  A. W. Cordes,et al.  Synthesis, structure and physical properties of the first one-dimensional phenalenyl-based neutral radical molecular conductor. , 2004, Journal of the American Chemical Society.

[5]  M. Kertész,et al.  Spin crossover of spiro-biphenalenyl neutral radical molecular conductors. , 2003, Journal of the American Chemical Society.

[6]  J. Kochi,et al.  Stable (long-bonded) dimers via the quantitative self-association of different cationic, anionic, and uncharged pi-radicals: structures, energetics, and optical transitions. , 2003, Journal of the American Chemical Society.

[7]  V. Ganesan,et al.  Isolation of the latent precursor complex in electron-transfer dynamics. Intermolecular association and self-exchange with acceptor anion radicals. , 2003, Journal of the American Chemical Society.

[8]  A. W. Cordes,et al.  Magneto-Opto-Electronic Bistability in a Phenalenyl-Based Neutral Radical , 2002, Science.

[9]  A. W. Cordes,et al.  Dimeric phenalenyl-based neutral radical molecular conductors. , 2001, Journal of the American Chemical Society.

[10]  A. W. Cordes,et al.  The first phenalenyl-based neutral radical molecular conductor , 1999 .

[11]  J. Ouyang,et al.  A Stable Neutral Hydrocarbon Radical: Synthesis, Crystal Structure, and Physical Properties of 2,5,8-Tri-tert-butyl-phenalenyl , 1999 .

[12]  P. Anderson The Resonating Valence Bond State in La2CuO4 and Superconductivity , 1987, Science.

[13]  R. Haddon,et al.  Electron delocalization in 9-oxidophenalenone complexes of boron and beryllium , 1986 .

[14]  K. Hirakawa,et al.  ESR Study of the Triangular Lattice Antiferromagnets with S=1/2: NaTiO2 and LiNiO2 , 1985 .

[15]  H. Kadowaki,et al.  Experimental Studies of Triangular Lattice Antiferromagnets with S=1/2: NaTiO2 and LiNiO2 , 1985 .

[16]  Philip W. Anderson,et al.  On the ground state properties of the anisotropic triangular antiferromagnet , 1974 .

[17]  Philip W. Anderson,et al.  Resonating valence bonds: A new kind of insulator? , 1973 .

[18]  A. Aten Reported Radioactivity of Osmium , 1948, Nature.