. 2016 Apr 21;6:24686. doi: 10.1038/srep24686

Table 2. Comparison of the magnetization, the anisotropy constant K₁ and the anisotropy field H_a calculated with TB-LMTO-ASA with experimental data taken from ^aref. ¹⁹ (Table 11.1), ^bref. ²², ^cref. ⁴², ^dref. ⁶ (no bulk but films of thickness up to 360 nm) and ^eref. ²¹.

System	μ₀M^exp [T]	μ₀M^ASA [T]	[MJ/m³]	[MJ/m³]	/	[T]	[T]	/
SmCo₅	1.07^a	1.04	17.2^a	69 (26)	25%	40.4^a	166	25%
Sm₂Co₁₇	1.25^a	1.22	4.2^a	25 (11)	17%	8.4^a	53	16%
Y₂Co₁₇	1.26^a	1.17	−0.34^a	0 (0)		−0.7^a	0
Sm₂Fe₁₇N₃	1.54^a	1.69	8.6^a	27 (25)	32%	14.0^a	40	35%
Ce₂Fe₁₄B	1.44^b	1.75	1.5^b	54 (14)	2.8%	2.6^b	76	3.4%
Nd₂Fe₁₄B	1.86^b	1.87	4.9^a	19 (6)	26%	6.6^a 7.3	26	25%^a
Nd₂Fe₁₄C	1.61^b	1.85	4^c	24 (7)	17%	6.3^c	32	20%
Sm₂Fe₁₄B	1.65^b	1.62	≤ −13^a	−31 (−10)	42%	≥15^b	−47	32%
NdFe₁₂N	1.66^d	2.06	5.3^d	47 (28)	11%	8d	57	14%
NdFe₁₁Ti	1.70^e	1.65	1.35	4 (2)	31%	2.0^e	7	28%
CeFe₁₁Ti	1.55^e	1.57	1.4^e	11 (4)	13%	2.3^e	18	13%

The experimental values for K₁ and H_a in columns 3 and 5 are given for room-temperature. Experimental magnetization values are given for T ≈ 4K. The calculated K₁ values in brackets are determined with a cut-off radius r_c = 1.005 Å as in ref. 8.

Table 2. Comparison of the magnetization, the anisotropy constant K1 and the anisotropy field Ha calculated with TB-LMTO-ASA with experimental data taken from aref. 19 (Table 11.1), bref. 22, cref. 42, dref. 6 (no bulk but films of thickness up to 360 nm) and eref. 21.

Table 2. Comparison of the magnetization, the anisotropy constant K₁ and the anisotropy field H_a calculated with TB-LMTO-ASA with experimental data taken from ^aref. ¹⁹ (Table 11.1), ^bref. ²², ^cref. ⁴², ^dref. ⁶ (no bulk but films of thickness up to 360 nm) and ^eref. ²¹.