## Conjugated Conducting Polymers |

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Page 224

isotropic hyperfine interaction Q ; = [ Au + A22 + A33 ] / 3 of the conduction

electrons with the nuclear

- ( 5 . 1 . 22 ) 00 * hielo where xs is the electron

...

isotropic hyperfine interaction Q ; = [ Au + A22 + A33 ] / 3 of the conduction

electrons with the nuclear

**spins**and is given by [ 5 . 15 , 16 , 21 - 23 ] = K = 40 Za- ( 5 . 1 . 22 ) 00 * hielo where xs is the electron

**spin**susceptibility per conduction...

Page 232

designed to give a vanishing dipole - dipole interaction of the

leaving chemical shift interaction ... In order to obtain a detectable signal of the

rare nuclei (

designed to give a vanishing dipole - dipole interaction of the

**spins**on average ,leaving chemical shift interaction ... In order to obtain a detectable signal of the

rare nuclei (

**spin**S ) they must be polarized with the help of the abundant nuclei ...Page 310

structure , crystal polyacetylene 107 structure dynamics 233 – 245 susceptibility

196 Curie 163 , 167 , 267 , 270 magnetic ( see also magnetic susceptibility ) 269

Pauli 161 , 165 – 169 , 209 , 211 , 219 , 267 - 270

...

structure , crystal polyacetylene 107 structure dynamics 233 – 245 susceptibility

196 Curie 163 , 167 , 267 , 270 magnetic ( see also magnetic susceptibility ) 269

Pauli 161 , 165 – 169 , 209 , 211 , 219 , 267 - 270

**spin**264 , 267 , 268 symmetry...

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### Contents

Introduction | 1 |

An Overview of the Theory of rConjugated Polymers | 7 |

References | 114 |

Copyright | |

7 other sections not shown

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### Common terms and phrases

absorption addition applied approach approximation atoms band behaviour bipolarons bond bond alternation calculations carriers chain charged chemical concentration conductivity configuration conjugated polymers contribution correlation corresponding Coulomb Coulomb interactions coupling decreases defects density dependence described determined dimerization discussed dopant doping effects electron electron-electron energy excitations expected experimental experiments field finite frequency function give ground Hamiltonian hopping Hubbard important increase indicated interactions interpretation involving lattice leads length Lett limit localized magnetic materials measurements metallic methods modes molecules motion neutral nuclear observed obtained optical pair parameter peak phonon Phys Physics polarons polyacetylene polyenes polymers position properties range relaxation resonance respect samples Sect separation shift shown shows similar single soliton spectra spectrum spin structure studies symmetry Synth temperature theoretical theory trans-(CH transition units valence values whereas