103As a rule, organic radical ions in solutions have rather short lifetimes, which makes them unsuitable for study by ESR, and at lifetimes shorter than 10 ns, even by a more sensitive method of optically detected ESR (OD ESR) of spin correlated radical ion pairs [1,2]. At the same time, the method of time resolved mag netic field effect (TR MFE) in recombination fluores cence of such pairs [2, 3] enables the detection of even shorter lived particles. This possibility is determined, first of all, by the time resolution of a setup, which we have managed to improve to ≈1 ns. An additional nec essary condition for identification of such short lived radicals is the existence of hyperfine coupling (HFC) constants in them sufficiently large (≈10 mT) to induce singlet-triplet transitions in the nanosecond time range. It is worth noting that the class of com pounds of interest includes only those with rather short fluorescence times.In this work, the potentialities of the TR MFE method have been demonstrated by the examples of radical anions of two fluoro substituted aromatic compounds-1,2,3,5 tetrafluorobenzene (TFB) and pentafluoroaniline (PFA)-generated by X ray irradi ation of solutions. This method is based on analysis of specific features of the ratio between the kinetic curves of recombination fluorescence in a magnetic field (I B (t) and in the absence of a field (I 0 (t)). In low polar ity solutions, the fluorescence intensity decay caused by recombination of radical ion pairs, in the limit of infinitely short fluorescence time and narrow instru mental function, is given bywhere F(t) is the pair recombination rate, θ is the frac tion of pairs generated in the singlet correlated state, and ρ ss (t) is the population of the singlet stage of such pairs [3]. In this approximation, the ratio(2) referred to as time resolved magnetic field effect, is independent of recombination kinetics F(t). However, at sufficiently high frequencies of ρ ss (t) oscillations caused by large HFC constants, the fluorescence kinetics must be described, not by Eq.(1), but by its integral convolution with the fluorescence probability of excited molecules, which changes exponentially with time, and the Gaussian instrumental function (see, e.g., [4]). Radical ions studied in this work have more than two different HFC constants. Therefore, in simulation of TR MFE curves, the singlet state population ρ ss (t) in strong and zero fields was calculated numerically. The spin relaxation times of the radical ions in the pair were considered in the framework of approximations described elsewhere [3,5].Studies of radical anions by the TR MFE method were carried out in 1-10 mM liquid solutions of TFB and PFA in 2,2,4 trimethylpentane (isooctane). In isooctane, the mobility of excess electrons is very high, and radical anions of electron acceptors form in the subnanosecond time domain. To reduce the contribu tion of the isooctane radical cation (the ESR spectrum width, ≈2 mT) to the spin evolution of the radical pair, a positive charge acceptor-hexameth...