Change of Energy of the Cubic Subnanocluster of Iron Under Influence of Interstitial and Substitutional Atoms

Table 2 Cluster energy at different positions of carbon and nickel atoms

С in CIS	N₀	u \( \left(\frac{\mathrm{meV}}{\mathrm{atom}}\right) \)	∆₁ \( \left(\frac{\mathrm{meV}}{\mathrm{atom}}\right) \)	Equivalent positions	N₁	\|∆₂\| \( \left(\frac{\mathrm{meV}}{\mathrm{atom}}\right) \)	N₂	\|∆₃\| \( \left(\frac{\mathrm{meV}}{\mathrm{atom}}\right) \)	N₃
1 ÷ 8	І	3018	427	1 = 4	a	481	a	909	a
			457	2 = 3 = 5 = 8	b	397	b	854	bd
			458	6 = 7	b	397	b	855	bd
9 ÷ 14	ІІ	2787	462	9 = 13	b	400	b	862	bd
			506	10 = 12	c	318	cd	824	c
			534	11 = 14	d	315	cd	849	bd

Cluster energy at different positions of carbon and nickel atoms where numbering is performed: N ₀—by symmetry, N ₁—by Δ ₁; N ₂—by Δ ₂; N ₃—by Δ ₃ criteria