| 10.1098/rspa.1971.0044 | positive anchor for the panel; RT saturation magnetization of very pure bulk iron | Fe | fe-w-calibration | J. Crangle and G. M. Goodman, 'The magnetization of pure iron and nickel', Proc. R. Soc. Lond. A 321, 477-491 (1971) | REF-01 | 2.152 |
| 10.1103/PhysRev.110.1333 | negative control; T_N = 525 K; Ms ~ 0 by physics, recorded null rather than 0.000 because the source reports a magnetic structure, not a magnetization value | NiO | fe-w-calibration | W. L. Roth, 'Magnetic Structures of MnO, FeO, CoO, and NiO', Phys. Rev. 110, 1333-1341 (1958) | REF-02 | |
| 10.1063/1.4926610 | only directly measured magnetization of an ordered Fe-W intermetallic found anywhere; Tc 550 K; K1 286 kerg/cm3 (10 K) with easy-plane <1000> anisotropy, not easy-axis [0001]; NOTE journal is APL Materials 3, 076101, NOT J. Appl. Phys. 118, 013901 as cited on the Fe17W3 dossier thread | WFe2 | fe-w-calibration | M. A. Koten, P. Manchanda, B. Balamurugan, R. Skomski, D. J. Sellmyer, and J. E. Shield, 'Ferromagnetism in Laves-phase WFe2 nanoparticles', APL Materials 3, 076101 (2015) | REF-03 | 0.434 |
| 10.1063/1.4926610 | room-temperature value of the same weak ferromagnet | WFe2 | fe-w-calibration | M. A. Koten et al., APL Materials 3, 076101 (2015) | REF-04 | 0.12 |
| earlier experimental literature reported lambda-WFe2 paramagnetic; no direct bulk magnetization measurement located. The 'bulk WFe2 = 33.8 emu/g (0.92 mu_B/Fe)' figure circulating in secondary sources is a DFT value cited inside Koten 2015, not a measurement | WFe2 | fe-w-calibration | referenced as ref. 12 in Koten et al., APL Materials 3, 076101 (2015) | REF-05 | |
| no measured magnetization located; Materials Project moment (0.092 mu_B/cell) is computed, not measured | Fe7W6 | fe-w-calibration | | REF-06 | |
| no measured magnetization or magnetic ordering located in accessible sources; possible lead: Ren et al., J. Appl. Phys. 116, 083908 (2014), doi:10.1063/1.4894396, claims to clarify experimental controversies on Fe-W magnetic properties (full text needed) | FeW | fe-w-calibration | | REF-07 | |
| 10.1016/j.matdes.2017.11.011 | compositionally adjacent alloy; number seen in full text surfaced by search | Fe-6 at.% W | fe-w-calibration | A. Nicolenco et al., 'Mapping of magnetic and mechanical properties of Fe-W alloys electrodeposited from Fe(III)-based glycolate-citrate bath', Materials & Design 138, 62-72 (2017) | REF-08 | |
| 10.1016/j.matdes.2017.11.011 | steep Ms drop with W content: 184 emu/g at 6 at.% W -> 18 emu/g at 25 at.% W | Fe-25 at.% W | fe-w-calibration | A. Nicolenco et al., Materials & Design 138, 62-72 (2017) | REF-09 | |
| 10.1016/j.matdes.2017.11.011 | weak ferromagnetism attributed to W(Fe) + weakly ferromagnetic Fe2W phases (Moessbauer-verified); 65 C-deposited crystalline alloys keep higher Ms up to 12 at.% W | Fe-(12-16) at.% W | fe-w-calibration | A. Nicolenco et al., Materials & Design 138, 62-72 (2017) | REF-10 | |
| 10.1143/JJAP.30.2839 | abstract-level only: single bcc phase for x<0.2, ferromagnetic for x<0.8, amorphous (0.2<x<0.6) paramagnetic even at 4.2 K; claims Fe moments in Fe-rich bcc EXCEED pure Fe (contested, heavy-5d-addition effect) - per-composition Ms requires full text, left null | Fe1-xWx (x < 0.2) | fe-w-calibration | K. Sumiyama, M. Hirata, W. Teshima, 'Magnetic and Electrical Properties of Nonequilibrium Fe-W Alloys Produced by Sputter Deposition', Jpn. J. Appl. Phys. 30, 2839 (1991) | REF-11 | |
| 10.1063/1.345964 | abstract-level only: magnetic ordering only in the bcc state (x<=30, x>=80); no ordering down to 4.2 K for amorphous 40<=x<=70; per-composition Ms requires full text, left null | FexW100-x (x <= 30 and x >= 80) | fe-w-calibration | Ming-Hui Lu and C. L. Chien, 'Structural and magnetic properties of Fe-W alloys', J. Appl. Phys. 67, 5787-5789 (1990) | REF-12 | |