Abstract
Magnetic order M(H, T) was determined as a function of temperature and external field for the monolayer Fe on W (110) using spin polarized low energy electron diffraction (SPLEED). The differential susceptibility χ = ∂M/∂H has a maximum at Tc∗ = 222.65 K. A power-law fit M(H = 0) ∝ (T−T′c)β results in T′c/Tc∗ = 0.997, whereas M(H = 0) vanishes at T∗/Tc∗ = 1.003.
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