Body-centered-cubic ni and its magnetic properties

The body-centered-cubic (bcc) 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 bcc Ni is ferromagnetic with a Curie temperature of 456 K and possesses a magnetic moment of 0.52+/-0.08 micro(B)/atom. The cubic magnetoc...

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Veröffentlicht in:Physical review letters 2005-04, Vol.94 (13), p.137210.1-137210.4, Article 137210
Hauptverfasser: TIAN, C. S, QIAN, D, JIANG, X. M, LIU, F. Q, QIAN, H. J, SUN, K, WANG, L. M, ROSSI, G, QIU, Z. Q, SHI, J, WU, D, HE, R. H, WU, Y. Z, TANG, W. X, YIN, L. F, SHI, Y. S, DONG, G. S, JIN, X. F
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Sprache:eng
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Zusammenfassung:The body-centered-cubic (bcc) 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 bcc Ni is ferromagnetic with a Curie temperature of 456 K and possesses a magnetic moment of 0.52+/-0.08 micro(B)/atom. The cubic magnetocrystalline anisotropy of bcc Ni is determined to be +4.0x10(5) ergs x cm(-3), as opposed to -5.7x10(4) ergs x 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 bcc Ni and fcc Ni, which are determined using angle-resolved photoemission with synchrotron radiation.
ISSN:0031-9007
1079-7114
DOI:10.1103/PhysRevLett.94.137210