Phenomenological description of the longitudinal vibrations of the quasi-one-dimensional solid PtCl: calculation of the valence defect frequencies

The longitudinal vibrations of the PtCl linear chain and those of various valence defects are described by a one-dimensional model in a first-nearest-neighbour interaction approximation. The analysis is performed as a function of the K2/K1 ratio (K1 and K2 representing the PtClIV-Cl and PtII-Cl force constants, respectively), which is shown to play an important role in the vibrational characteristics of the defects while the infrared frequencies are not strongly dependent on a particular ratio. A coherent description of the frequencies of the modes of the perfect chain and those of the polaronic defects is obtained for K2/K1=0.3. For this ratio the electron polaron and the electron bipolaron give rise to one Raman-active mode while at least two are predicted for the other investigated defects. The shapes of the Raman bands associated with the electron and hole polarons are explained by the chlorine isotopic effect. The vibration associated with the electron bipolaron is predicted to be at about 210 cm-1 where a broad line grows upon photolysis. An elementary calculation based upon a Born-Mayer potential for short-range interactions, adjusted from the interionic distances, leads to force constants of the same magnitude as those adjusted from the experimental frequencies.

[1]  Bishop,et al.  Electron and hole polaron asymmetry in a two-band Peierls-Hubbard material. , 1990, Physical review. B, Condensed matter.

[2]  B. Swanson,et al.  Resonance Raman evidence for electron and hole defect asymmetry in the quasi-one-dimensional mixed-valence solid [PtII(en)2][PtIV(en)2Cl2][ClO4]4 (en = ethylenediamine) , 1990 .

[3]  B. Swanson,et al.  The red and near-infrared resonance Raman spectroscopy of photo-induced defects in the mixed-valence linear chain complex [PtII(en)2][PtIV(en)2Cl2][ClO4]4 , 1990 .

[4]  Wachter,et al.  Far-infrared optical investigations on quasi-one-dimensional halogen-bridged mixed-valence compounds. , 1989, Physical review. B, Condensed matter.

[5]  B. Swanson,et al.  The mid-infrared signature of photo-induced defects in the quasi-one-dimensional mixed-valence solid [PtII(en)2][PtIV(en)2Cl2][ClO4]4 , 1989 .

[6]  S. Kurita,et al.  Experimental evidence of polaronic states in halogen bridged mixed valence platinum complexes , 1989 .

[7]  S. Kurita,et al.  Photo-Induced Defect States in a Quasi One-Dimensional Mixed-Valence Platinum Complex , 1988 .

[8]  W. Schaefer,et al.  Translational symmetries in the linear-chain semiconductors K4[Pt2(P2O5H2)4X].cntdot.nH2O (X = Cl, Br, I) , 1988 .

[9]  B. Swanson,et al.  Charge density waves and local states in quasi-one-dimensional mixed valence inorganic complexes , 1988 .

[10]  D. Baeriswyl,et al.  Localised polaronic states in mixed-valence linear chain complexes , 1988 .

[11]  L. Butler,et al.  Karplus-type relationship for quadrupole coupling constants and asymmetry parameters for substituted acetic acids , 1988 .

[12]  N. Matsushita,et al.  Photo-Induced Absorption Band in One-Dimensional Halogen-Bridged Mixed-Valence Platinum Complex: [Pt(en)2][PtI2(en)2](SO4)2·6H2O and its Au-Doped Complex: [AuxPt1-xI(en)2]SO4·3H2O , 1987 .

[13]  Y. Onodera Soliton Model for Halogen-Bridged Mixed-Valence Platinum Complexes , 1987 .

[14]  M. Tanaka,et al.  Fine structures of the resonant Raman spectra in quasi-one-dimensional crystals of halogen-bridged mixed-valence platinum compounds , 1986 .

[15]  R. Clark,et al.  Advances in Infrared and Raman Spectroscopy , 1982 .

[16]  Jeremy R. Campbell,et al.  Electronic Spectra and Resonance Raman Spectra of Mixed-Valence Linear-Chain Complexes of Platinum with 1,2-Diaminoethane , 1978 .

[17]  A. S. Barker,et al.  Optical studies of the vibrational properties of disordered systems , 1975 .