The body-centered-cubic (bec) phase of Ni, which does not exist in nature, has been achieved as a thin film on GaAs(001) at 170 K via molecular beam epitaxy. The bec Ni is ferromagnetic with a Curie temperature of 456 K and possesses a magnetic moment of 0.52 ± 0.08 μB/atom. The cubic magneto-crystalline anisotropy of bec Ni is determined to be +4.0 × 105 ergs · cm-3, as opposed to -5.7 × 10 4 ergs · cm-3 for the naturally occurring face-centered-cubic (fcc) Ni. This sharp contrast in the magnetic anisotropy is attributed to the different electronic band structures between bec Ni and fcc Ni, which are determined using angle-resolved photoemission with synchrotron radiation.

Body-centered-cubic Ni and its magnetic properties / C.S. Tian, D. Qian, D. Wu, R.H. He, Y.Z. Wu, W.X. Tang, L.F. Yin, Y.S. Shi, G.S. Dong, X.F. Jin, X.M. Jiang, F.Q. Liu, H.J. Qian, K. Sun, L.M. Wang, G. Rossi, Z.Q. Qiu, J. Shi. - In: PHYSICAL REVIEW LETTERS. - ISSN 0031-9007. - 94:13(2005), pp. 137210.1-137210.4.

Body-centered-cubic Ni and its magnetic properties

G. Rossi;
2005

Abstract

The body-centered-cubic (bec) phase of Ni, which does not exist in nature, has been achieved as a thin film on GaAs(001) at 170 K via molecular beam epitaxy. The bec Ni is ferromagnetic with a Curie temperature of 456 K and possesses a magnetic moment of 0.52 ± 0.08 μB/atom. The cubic magneto-crystalline anisotropy of bec Ni is determined to be +4.0 × 105 ergs · cm-3, as opposed to -5.7 × 10 4 ergs · cm-3 for the naturally occurring face-centered-cubic (fcc) Ni. This sharp contrast in the magnetic anisotropy is attributed to the different electronic band structures between bec Ni and fcc Ni, which are determined using angle-resolved photoemission with synchrotron radiation.
Ferromagnetic-resonance; epitaxial-growth; thin-films; BCC CO; FE; anisotropy; GAAS(001); FCC; surface; overlayers
Settore FIS/03 - Fisica della Materia
2005
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2434/555024
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