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Spectrometer electronic Zeeman interaction

The forces which drive the intersystem crossing are the nuclear spin-dependent hyperfine interactions in the radicals and the electron Zeeman interactions. This becomes evident from the following after pair formation in the magnetic field of a NMR spectrometer, say, the two unpaired electron sfnns precess about the magnetic field axis starting from defined initial phase an es. These iititial phase angles are different for the four possible initial electronic states T Tq,... [Pg.10]

The unpaired electron with its spin S = 1/2 in a sample disposed into the resonator of the EPR spectrometer interacts magnetically a) with the external magnetic field H (Zeeman interaction) b) with the nuclear spin of the host atom or metal ion / (hyperfine interaction) c) with other electron spins S existing in the sample (dipole-dipole interaction). In the last case, electrons can be localized either at the same atom or ion (the so called fine interaction), for example in Ni2+, Co2+, Cr3+, high-spin Fe3+, Mn2+, etc., or others. These interac-tions are characterized energetically by the appropriate spin-Hamiltonian... [Pg.205]


See other pages where Spectrometer electronic Zeeman interaction is mentioned: [Pg.10]    [Pg.14]    [Pg.61]    [Pg.123]    [Pg.196]    [Pg.77]    [Pg.6481]    [Pg.158]    [Pg.158]    [Pg.6480]    [Pg.119]   
See also in sourсe #XX -- [ Pg.10 , Pg.14 ]




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