Table 1 Values of the exponents β, γ, and δ as determined from the modified Arrott plot, Kouvel-Fischer plot and critical isotherm for Fe2CrAl, Fe1.75Mn0.25CrAl, Fe1.5Mn0.5CrAl, and Fe1.25Mn0.75CrAl.
From: Unconventional critical behaviour in weak ferromagnets Fe2-xMnxCrAl (0 ≤ x < 1)
Composition | Ref | Method | β | TC (MS) K | γ | TC (χ0) K | δ | TC17 |
|---|---|---|---|---|---|---|---|---|
Fe2CrAl | This work | MAP | 0.2730 | 201.89 ± 0.37 | 1.34 | 201.11 ± 0.14 | 5.91 | 202 K |
KF plot | 0.273 ± 0.01 | 201.06 ± 0.04 | 1.35 ± 0.02 | 201.01 ± 0.03 | 5.94 ± 0.03 | |||
CI | – | – | – | – | 5.69 ± 0.08 | |||
Fe1.75Mn0.25CrAl | This work | MAP | 0.2822 | 120.90 ± 0.05 | 1.42 | 121.19 ± 0.06 | 6.03 | 120 K |
KF plot | 0.282 ± 0.02 | 120.34 ± 0.09 | 1.41 ± 0.03 | 121.02 ± 0.02 | 6 ± 0.01 | |||
CI | – | – | – | – | 5.94 ± 0.05 | |||
Fe1.5Mn0.5CrAl | This work | MAP | 0.3281 | 48.6 ± 0.25 | 1.46 | 47.32 ± 0.05 | 5.45 | 48 K |
KF plot | 0.326 ± 0.02 | 46.67 ± 0.01 | 1.47 ± 0.05 | 47.41 ± 0.01 | 5.45 ± 0.02 | |||
CI | – | – | – | – | 5.28 ± 0.08 | |||
Fe1.25Mn0.75CrAl | This work | MAP | 0.3474 | 26.86 ± 0.09 | 1.6 | 27.15 ± 0.05 | 5.61 | 27 K |
KF plot | 0.345 ± 0.13 | 26.79 ± 0.06 | 1.61 ± 0.04 | 27.10 ± 0.04 | 5.60 ± 0.07 | |||
CI | – | – | – | – | 5.56 ± 0.01 | |||
Co50Cr25Al25 | MAP | 0.488 (3) | 1.144 (4) | 3.336 (5) | ||||
KF Plot | 0.482 (13) | 1.148 (16) | 3.382(20) | |||||
CI | 3.401(4) | |||||||
Co45Ni5Cr25Al45 | MAP | 0.513(7) | 1.048(4) | 3.043 (7) | ||||
KF plot | 0.511(7) | 1.028 (6) | 3.012(8) | |||||
CI | 2.976 (11) | |||||||
Co2TiGe | MAP | 0.495 | 1.325 | 3.677 | ||||
KF plot | 0.495 | 1.324(4) | 3.675 | |||||
CI | 3.671(1) | |||||||
Mean field theory | Theory | 0.5 | 1 | 3 | ||||
3D Heisenberg model (O*) | Theory | 0.365 | 1.386 | 4.80 | ||||
3D Heisenberg model (D*) | Theory | 0.5 | 2 | 5 | ||||
3D Ising model | Theory | 0.325 | 1.241 | 4.82 | ||||
3D XY model | Theory | 0.346 | 1.316 | 4.81 |