Articles you may be interested inMagnetic field effects in singlet-polaron quenching in molecularly doped fluorescence organic light-emitting diodes J. Appl. Phys. 116, 064308 (2014); 10.1063/1.4892625Hyperfine interaction mechanism of magnetic field effects in sequential fluorophore and exciplex fluorescence D 1 ( 2 B 2g )→D 0 ( 2 A u ) fluorescence from the matrix-isolated perylene cation following laser excitation into the D 5 ( 2 B 3g ) and D 2 ( 2 B 3g ) electronic states Yield determination of OH (v=0,1) radicals produced by the electron-ion recombination of protonated moleculesThe recombination fluorescence from anthracene that has been photoionized at 188 nm in isooctane solutions containing low concentrations of either perfluorocyclobutane (C 4 F 8 ) or perfluorobenzene (C 6 F 6 ) has been examined as a function of magnetic-field strength. Level crossing resonances are found at magnetic-field positions predicted by the theory of a hyperfine driven spin evolution on the perfluoroanion ͑i.e., 0, 452, 757, and 903 G for C 4 F 8 and at 0, 411, and 822 G for C 6 F 6 ͒. The widths of the zero-field resonances have been studied as a function of perfluorocarbon concentration. For perfluorocyclobutane, the peak to peak widths of the derivative spectra vary from 6.8 to 13 G over a concentration range from 0.005 to 0.21 M. This variation is quantitatively predicted using the analytic solution to the time-dependent diffusion equation in a Coulomb field to determine how the distribution function for thermalized electron-cation distances evolves into its concentration dependent counterpart for anion-cation separation distances. For perfluorobenzene, the widths are observed to vary over a wider range from 3.0 to 38.5 G for concentrations from 0.0044 to 0.13 M. The additional concentration broadening in this case is consistent with previous estimates of the spin-dephasing rate constant for C 6 F 6 -C 6 F 6 Ϫ charge exchange.