Table 1.

Structural parameters of amorphous carbons ¹.

Samples	Interlayer Distance, $\mathit{d}$ (Å)	${\mathit{L}}_{\mathit{C}\mathit{S}\mathit{R}}^{\mathit{c}},\mathbf{nm}$	Number of BSU Layers	${\mathit{L}}_{\mathit{C}\mathit{S}\mathit{R}}^{\mathit{a}},\mathbf{nm}$	Ref.
mncr Gr 2	3.35(X)	105	313	550	this work
μncr Gr 2	3.35(X)	49	146	184	this work
ShC	3.47(N); 3.48(X)	2,5(N); 2.0(X)	7(N); 5–6(X)	2.1(X)	[17]
AnthX	3.47(N); 3.47(X)	2.5(N); 1.9(X)	7(N); 5–6(X)	1.6(X)	[17]
AnthC (Donetsk)	3.50(X)	2.2(X)	5–6(X)	2.1(X)	[17]
CB632	3.57(N); 3.58(X)	2.2(N); 1.6(X)	6(N); 4–5(X)	1.4(X)	[17]
CB624 3	3.40(N); 3.45(X)	7.8(N); 6(X)	23(N); 17(X)	14.6	[17]
Ak-rGO	3.50(N)	2.4 (N)	7(N)	>20(N) 4	[27]
TE-rGO	3.36(N)	2.9 (N)	8(N)	>20(N) 4	[28]

¹ Notations (N) and (X) indicate data obtained by neutron and X-ray diffraction, respectively. ² The data are obtained by the treatment of (002) and (110) reflexes using Scherrer’s relation L_CSR = K·λ/B·cosΘ. Here λ is the X-ray radiation wavelength (CuK_α) 0.154 nm, Θ is the position of the (110) ($L_{CSR}^a$) and (002) ($L_{CSR}^c$) peaks, B is the half-height width of the peak in 2Θ (rad) units, and constant K constitutes 0.9 and 1.84 for reflexes (002) and (110), respectively, in the approximation of disk-shaped particles. ³ X-ray data were corrected in the current study. ⁴ $L_{CSR}^a$ = 20 nm means the low limit of the value accessible for the measurements performed.