Rb-TCNQ(II) is shown to be a realization of the BOW phase of half-filled extended Hubbard models. The BOW phase has a regular array of sites with inversion (Ci) symmetry, a finite magnetic gap Em and broken electronic Ci symmetry. The phase is conditionally stable against dimerization for linear electron-phonon (e-ph) coupling. At 100 K, Rb-TCNQ(II) crystals have regular TCNQ- stacks at Ci centers, negligible spin susceptibility that indicates finite Em, and infrared (ir) spectra that indicate broken Ci symmetry. The 100 and 295 K crystal structures rule out a dimerization transition around 220 K that had previously been inferred from magnetic and ir data.
|Original language||English (US)|
|Number of pages||5|
|Journal||Chemical Physics Letters|
|State||Published - Jun 16 2009|
All Science Journal Classification (ASJC) codes
- Physics and Astronomy(all)
- Physical and Theoretical Chemistry