1998
DOI: 10.1007/bf03162031
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Paramagnetic centres in exinite, vitrinite and inertinite

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Cited by 11 publications
(14 citation statements)
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“…The performed in this work numerical analysis of multi-component structure of EPR spectra of lignite confirmed our earlier results [13][14][15] about complex shape and strong dependence of paramagnetic centres system on metamorphism of coal.…”
Section: Discussionsupporting
confidence: 89%
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“…The performed in this work numerical analysis of multi-component structure of EPR spectra of lignite confirmed our earlier results [13][14][15] about complex shape and strong dependence of paramagnetic centres system on metamorphism of coal.…”
Section: Discussionsupporting
confidence: 89%
“…The fast spin-lattice relaxation processes are characteristic of the multi-ring aromatic structures (narrow Lorentz 3 lines), and relatively slow spin-lattice relaxation processes occur in simple aromatic coal structures (broad Gauss and broad Lorentz 1 lines). The correlations between the coal structures and the spin-lattice relaxation times were confirmed by EPR and FTIR studies earlier [5,6,[13][14][15][16][17]. The influence of microwave power on the three component lines of the EPR spectra of the studied demineralised lignite is shown in Figure 3.…”
Section: Resultssupporting
confidence: 59%
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“…Total intensity of EPR line taking into account the existence of paramagnetic centers in singlet and triplet states is presented in the form [12]: (3) where B and C [K] are constants equal to and aN d /2k, respectively [12]. Accordingly, relative contributions of paramagnetic centers in singlet (S = 0) and triplet (S = 1) states to whole amount of centers in doublet, singlet, and triplet states are given in the form [12]: (4) As mentioned earlier, it was shown [6][7][8][9] that in the total group of paramagnetic centers generating components lines in the form of Lorentzian L1 shape in EPR spectra of coal macerals, exinite, and vitrinite, there is a part of centers in excited triplet state (S = 1). Accordingly, these centers do not fulfi l the Curie law represented by the formula I = C/T.…”
Section: Introductionmentioning
confidence: 97%
“…in temperature T 1 [K] by I 1 = I NC (T 1 ) + C/T 1 (C -Curie constant [K]) and in temperature T 2 by I 2 = I NC (T 2 ) + C/T 2 , respectively, where I NC (T) is a part of total intensity I generated by paramagnetic centers, which do not fulfi l the Curie law, while the paramagnetic centers obeying the Curie law are responsible for the component C/T. The existence of paramagnetic centers in the ground doublet state S = ½, for which the temperature dependence of intensity is described by the Curie law (I = C/T) (and paramagnetic centers in excited triplet states (S = 1) was evidenced in coal and coal macerals [4][5][6][7][8][9].…”
Section: Introductionmentioning
confidence: 99%