SPECTROSCOPIC STUDIES OF EXCHANGE INTERACTIONS IN POLYNUCLEAR TRANSITION METAL COMPLEXES I. [(NH3)5Cr(OH)Cr(NH3)5] Cl5,3H20.

1973 ◽  
Vol 26 (3) ◽  
pp. 505 ◽  
Author(s):  
J Ferguson ◽  
HU Gudel

Large single crystals of ,u-hydroxo-bis[pentaamminechromium(III) chloride trihydrate have been prepared and their spectroscopic properties determined. The analysis of polarized single-crystal luminescence spectra provides an accurate ground electronic level scheme for the weakly coupled chromium ions in the dimeric cluster. The splitting is described by the isotropic Hamiltonian X = JS,.Sb-j(S,.Sb)2 with J = 31.9 cm-1 and j = 0.23 cm-1. The temperature dependence of the polarized absorption spectrum is consistent with this level scheme. The positions of the components of the singly excited (4A2-2E) state have been determined.

1973 ◽  
Vol 26 (3) ◽  
pp. 513 ◽  
Author(s):  
J Ferguson ◽  
H.U Gudel ◽  
M Puza

Single crystals of phydroxo-bis[pentaamminechromium(III)] chloride monohydrate have been prepared. The spectroscopic properties of these crystals have been measured and two crystal forms have been characterized. The first form is obtained from solutions at 2�C and it changes to the second, stable form, at room temperature. The latter is tetragonal, space group D44-P41212 with a = 16.28 %L, c = 14.84 A, and Z = 8. The spectroscopic properties require two inequivalent sets of dimer units in the unit cell and this result is consistent with the X-ray data. The spectroscopic properties of the first form require four inequivalent sets of dimers and the ground state energy levels of each of these are described by the isotropic Hamiltonian H = JSa . Sb - j(Sa. Sb)2 with the following values: set 1, J = 30.4+/- 0.2, j = 0.32+/-0. 10; set 2, J = 30.4 +/-0.2, j = 0.221 0.10; set 3, J = 31.4 +/-0.2, j = 0-18+/- 0.10; set 4, J = 31-4+/- 0.4, j = 0.0+/- 0.20. High-resolution luminescence excitation spectroscopy shows that sets 1 and 2 are not strongly coupled to sets 3 and 4. The small differences between sets 1 and 2 and between sets 3 and 4 suggest that these differences arise from structural disorder within the two inequivalent sets of the room temperature stable form. Previous differences in the interpretation of the earlier magnetic and


2001 ◽  
Vol 708 ◽  
Author(s):  
S. Guha ◽  
J.D. Rice ◽  
C. M. Martin ◽  
W. Graupner ◽  
M. Chandrasekhar ◽  
...  

ABSTRACTSpectroscopic properties of conjugated molecules/polymers have varying degrees of sensitivity to backbone conformation. Optical studies are presented as a function of temperature and hydrostatic pressure, using photoluminescence and Raman scattering from two polymers with distinct differences in their backbone conformation, namely, polyfluorene (PF) and ladder type poly(para-phenylene)(m-LPPP). In contrast to the photoluminescence (PL) vibronics in mLPPP, the 0-0 PL vibronic peak in PF shows a red-shift with increasing temperatures. Pressure studies reveal that the PL spectrum of PF red-shifts and broadens with increasing pressures. The phonon lines in PF show an antiresonance effect at higher pressures indicating a strong electron-phonon interaction.


1997 ◽  
Vol 106 (8) ◽  
pp. 3067-3077 ◽  
Author(s):  
M. Karbowiak ◽  
J. Drozdzynski ◽  
K. M. Murdoch ◽  
N. M. Edelstein ◽  
S. Hubert

2003 ◽  
Vol 102-103 ◽  
pp. 395-401 ◽  
Author(s):  
I. Földvári ◽  
E. Beregi ◽  
A. Baraldi ◽  
R. Capelletti ◽  
W. Ryba-Romanowski ◽  
...  

1981 ◽  
Vol 103 (15) ◽  
pp. 4382-4388 ◽  
Author(s):  
K. W. Penfield ◽  
R. R. Gay ◽  
R. S. Himmelwright ◽  
N. C. Eickman ◽  
V. A. Norris ◽  
...  

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