Conjugated Conducting PolymersHelmut G. Kiess, Dionys Baeriswyl |
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Page 229
... ( ENDOR ) lines , whereas N nonequivalent nuclear spins ( S = 1/2 ) result in 2N ESR lines , but only 2N NMR ( ENDOR ) lines . Thus , for a fairly small number N , the ESR spectrum may become unresolved , whereas fewer lines in the NMR ...
... ( ENDOR ) lines , whereas N nonequivalent nuclear spins ( S = 1/2 ) result in 2N ESR lines , but only 2N NMR ( ENDOR ) lines . Thus , for a fairly small number N , the ESR spectrum may become unresolved , whereas fewer lines in the NMR ...
Page 249
... ENDOR where the spectrum results from simple summation rather than multiple product of the various spectral lines , as in the ESR case . Any form of p ; must therefore reproduce simultaneously the ENDOR spectrum . Detailed ENDOR ...
... ENDOR where the spectrum results from simple summation rather than multiple product of the various spectral lines , as in the ESR case . Any form of p ; must therefore reproduce simultaneously the ENDOR spectrum . Detailed ENDOR ...
Page 251
Helmut G. Kiess, Dionys Baeriswyl. 251 middle of the Davies - type ENDOR spectrum is due to spin alignment effects . These spin alignment effects are also present in CW ENDOR and must not be interpreted as spectral features . Independent ...
Helmut G. Kiess, Dionys Baeriswyl. 251 middle of the Davies - type ENDOR spectrum is due to spin alignment effects . These spin alignment effects are also present in CW ENDOR and must not be interpreted as spectral features . Independent ...
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A.J. Heeger atoms Baeriswyl band gap behaviour bipolarons bond alternation bond lengths calculations chain charge carriers charged solitons Chem chemical shift cis-(CH conducting polymers conjugated polymers correlation Coulomb interaction coupling Cryst D.K. Campbell defects dielectric function diffusion dimerization discussed dopant dopant concentration dopant molecules doping doping levels e-e interactions effects electron correlation electron spin electron-electron interactions electron-phonon ENDOR energy excitations exciton experimental frequency function Hamiltonian Hartree-Fock hopping Hubbard model Hückel hyperfine interactions inter-chain Kivelson lattice Lett linewidth magnetic metallic molecular neutral solitons nonlinear nonlinear optical nuclear observed obtained one-dimensional optical absorption optical gap parameters peak Peierls Peierls-Hubbard model phonon Phys polarons polyacetylene polyenes polypyrrole polythiophene properties proton quantum quasi-particles Raman resonance samples Sect shown in Fig spectra spectrum spin density structure symmetry Synth tensor theory trans trans-(CH trans-polyacetylene transition valence values Vardeny