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Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

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312 DETECTION AND ESTIMATION OF INTERMEDIATESate molecules an interaction between the magnetic moment and the spin momentmay occur. The exact nature <strong>of</strong> the contribution depends on the coupling caseinvolved. If the coupling is described by the Hund (a) case, then microwave absorptionin the presence <strong>of</strong> a magnetic field can arise from transitions between thedifferent M, values (subject to the selection rule AM, = kl). However, somedecoupling in the magnetic field may occur: that is to say, there may be an incipientPaschen-Back effect. With magnetic fields large compared with the internal field<strong>of</strong> the species, the electronic spin and orbital angular momentum will be quantisedseparately along the direction <strong>of</strong> the field. Such a decoupling effect is observed inthe resonance spectrum <strong>of</strong> nitrogen dioxide‘74, but not at all with nitric oxide17’:molecular oxygen shows appreciable but not complete deco~pling”~. Hyperfinestructure <strong>of</strong> the resonance spectrum <strong>of</strong> gases may result from interactions bothwith nuclear spin and with molecular rotation. A number <strong>of</strong> resonances are observedfrom each main electronic level, depending upon the multiplicity <strong>of</strong> thespecies. Fig. 11 shows the transitions expected in the three sublevels 3P0, 3P1 and’P, <strong>of</strong> ground state atomic oxygen. It will be appreciated that while the gas-phaseresonance spectra may be more complex than those <strong>of</strong> condensed-phase systems,the information carried by the spectra is also more complete. In suitable cases, boththe chemical identity and the electronic state <strong>of</strong> the resonant species can be established.Absolute concentrations may be obtained by calculation from absoluteabsorption intensities, or, preferably, by calibration <strong>of</strong> the spectrometer with asuitable gas-phase standard (see below). Considerable effort has gone into relatingline shapes and absorption intensities with perturbing factors such as field modulation(see ref. 177).cE0$-1-2I T .-----Fig. 11. Zeeman energy levels <strong>of</strong> atomic oxygen in the aP states.V

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