Paramagnetic centers in detonation nanodiamonds studied by CW and pulse EPR

Dispersed detonation nanodiamonds have been studied by continuous-wave (CW) and pulse EPR techniques. The spectrum of bulk radicals ( g = 2.0025 ± 0.0002, a Lorentz line shape with Δ H pp = 0.95 ± 0.05 mT) dominated in CW EPR and prevented to record spectra from other paramagnetic species. The pulse...

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Veröffentlicht in:Chemical physics letters 2010-06, Vol.493 (4), p.319-322
Hauptverfasser: Fionov, A.V., Lund, A., Chen, W.M., Rozhkova, N.N., Buyanova, I.A., Emel’yanova, G.I., Gorlenko, L.E., Golubina, E.V., Lokteva, E.S., Ōsawa, E., Lunin, V.V.
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Sprache:eng
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Zusammenfassung:Dispersed detonation nanodiamonds have been studied by continuous-wave (CW) and pulse EPR techniques. The spectrum of bulk radicals ( g = 2.0025 ± 0.0002, a Lorentz line shape with Δ H pp = 0.95 ± 0.05 mT) dominated in CW EPR and prevented to record spectra from other paramagnetic species. The pulse EPR-spectrum was the superposition of the distorted P1-center spectrum with parameters ( g = 2.0025, A xx = 2.57 mT, A yy = 3.08 mT, A zz = 4.07 mT), the H1-center spectrum ( g = 2.0028) and the single line ( g = 2.0025, Δ H pp = 0.40 ± 0.05 mT) from other centers which may be assigned to surface radicals. The concentration of P1-centers has been estimated by CW EPR as 2 ± 1 ppm N.
ISSN:0009-2614
1873-4448
1873-4448
DOI:10.1016/j.cplett.2010.05.050