Conjugated Conducting Polymers |
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Page 63
Although calculations performed in this limit are not expected to be immediately
relevant to a - conjugated polymers , they are nonetheless very important as
benchmarks for numerical methods which are used to probe the difficult but
important ...
Although calculations performed in this limit are not expected to be immediately
relevant to a - conjugated polymers , they are nonetheless very important as
benchmarks for numerical methods which are used to probe the difficult but
important ...
Page 104
100 ) is 12 = 0 , representing the Goldstone mode of the broken continuous
translational symmetry . It is important to notice that in this case the structure of
the defect does not enter at all . Therefore these vibrational modes , when
observed [ 2 .
100 ) is 12 = 0 , representing the Goldstone mode of the broken continuous
translational symmetry . It is important to notice that in this case the structure of
the defect does not enter at all . Therefore these vibrational modes , when
observed [ 2 .
Page 141
Nevertheless , a coplanar conformation can turn out to be of importance since out
- of - plane distortions can give rise to ... However , conducting polymers do by no
means behave like conventional semiconductors , the important difference ...
Nevertheless , a coplanar conformation can turn out to be of importance since out
- of - plane distortions can give rise to ... However , conducting polymers do by no
means behave like conventional semiconductors , the important difference ...
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Contents
Introduction | 1 |
An Overview of the Theory of rConjugated Polymers | 7 |
IndependentElectron | 17 |
Copyright | |
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absorption addition applied approach approximation atoms band behaviour bipolarons bond bond alternation calculations carriers chain charged chemical concentration conductivity configuration conjugated polymers correlation corresponding Coulomb Coulomb interactions coupling decreases defects density dependence described determined dimerization discussed dopant doping effects electron electron-electron electron-phonon ENDOR energy excitations expected experimental experiments field finite frequency function give ground Hamiltonian hopping Hubbard hyperfine important increase indicated interactions interpretation involving lattice leads length Lett limit magnetic materials measurements metallic methods modes motion neutral nuclear observed obtained one-dimensional optical pair parameter peak phonon Phys physical polarons polyacetylene polyenes polymers position properties range relaxation resonance respect samples Sect shift shown shows similar single Solid soliton spectra spectrum spin structure studies symmetry Synth temperature theoretical theory trans-(CH transition units valence values whereas