Literature DB >> 17583936

Electron spin relaxation in x-lithium phthalocyanine.

Hideo Sato1, Lauraine A Dalton, Duc Ha, Richard W Quine, Sandra S Eaton, Gareth R Eaton.   

Abstract

Continuous-wave linewidths and spin susceptibilities, spin-spin relaxation rates (1/T2), and spin-lattice relaxation rates (1/T1) for two sources of x-LiPc were measured at 9.5 GHz between 15 and 298 K. Relaxation rates at 34 GHz were measured between 80 and 298 K. Room-temperature relaxation rates also were measured at 250 MHz, 1.9 GHz, and 2.76 GHz. The temperature dependences of linewidths and spin susceptibilities are characteristic of 1-D organic conductors. The ratio of populations of localized and delocalized electrons varies with sample preparation. For a single needle between 15 and about 200 K, 1/T2 is higher for the parallel orientation, but 1/T1 is higher for the perpendicular orientation, consistent with predictions based on dipolar interactions. Between about 60 and 150 K, which is the temperature regime in which spin susceptibility is changing rapidly with temperature, 1/T1 exhibits a non-monotonic dependence on temperature and is lower at 34 GHz than at 9.5 GHz. In other organic conductors, this dependence has been attributed to a bottleneck mechanism of relaxation. At higher temperatures, 1/T1 becomes less orientation-dependent. At room temperature, T1 increases rapidly between 250 MHz (3.0 micros) and 2.76 GHz (6.3 micros) and then shows less frequency dependence up to 34 GHz (9.8 micros). The relaxation rate near room temperature might have a substantial contribution from spin hopping perpendicular to the stacking axis of the molecules.

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Year:  2007        PMID: 17583936     DOI: 10.1021/jp070810y

Source DB:  PubMed          Journal:  J Phys Chem B        ISSN: 1520-5207            Impact factor:   2.991


  2 in total

1.  A Pulse EPR 25 mT magnetometer with 10ppm resolution.

Authors:  Subramanian V Sundramoorthy; Boris Epel; Howard J Halpern
Journal:  Appl Magn Reson       Date:  2017-06-05       Impact factor: 0.831

2.  Digital EPR with an arbitrary waveform generator and direct detection at the carrier frequency.

Authors:  Mark Tseitlin; Richard W Quine; George A Rinard; Sandra S Eaton; Gareth R Eaton
Journal:  J Magn Reson       Date:  2011-09-14       Impact factor: 2.229

  2 in total

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