Magnetocrystalline anisotropy in x-ray magnetic linear dichroism at the 3pedges of crystalline Fe thin films

2014 ◽  
Vol 89 (14) ◽  
Author(s):  
M. F. Tesch ◽  
D. Legut ◽  
H.-Ch. Mertins ◽  
M. C. Gilbert ◽  
C. Jansing ◽  
...  
2011 ◽  
Vol 84 (13) ◽  
Author(s):  
Markus Meinert ◽  
Jan-Michael Schmalhorst ◽  
Christoph Klewe ◽  
Günter Reiss ◽  
Elke Arenholz ◽  
...  

2018 ◽  
Vol 87 (11) ◽  
pp. 114713
Author(s):  
Goro Shibata ◽  
Kohei Yoshimatsu ◽  
Keisuke Ishigami ◽  
Takayuki Harano ◽  
Yukio Takahashi ◽  
...  

2014 ◽  
Vol 50 (11) ◽  
pp. 1-4 ◽  
Author(s):  
Hans-Christoph Mertins ◽  
Dominik Legut ◽  
Marc Tesch ◽  
Christine Jansing ◽  
Markus Gilbert ◽  
...  

2019 ◽  
Vol 780 ◽  
pp. 79-84
Author(s):  
Shu Chih Haw ◽  
Chang Yang Kuo ◽  
Zhiwei Hu ◽  
Je Wei Lin ◽  
Jenn Min Lee ◽  
...  

2002 ◽  
Vol 80 (9) ◽  
pp. 1613-1615 ◽  
Author(s):  
S. S. Dhesi ◽  
G. van der Laan ◽  
E. Dudzik

1996 ◽  
Vol 437 ◽  
Author(s):  
G.J. Mankey ◽  
K. Subramanian ◽  
R.L. Stockbauer ◽  
R.L. Kurtz

AbstractWe present measurements of the evolution with film thickness of the 3d electronic states at the Fermi energy of ultrathin Ni films. The morphology and thickness of the films is determined from x-ray photoelectron spectroscopy. x-ray photoelectron diffraction and x-ray magnetic linear dichroism using synchrotron radiation. Photoelectron angular distributions were measured using an ellipsoidal mirror analyzer. Even at submonolayer Ni coverages, the 3d electronic states exhibit bulk-like properties. This is attributed to the short screening length of electrons in metals, the localization of the 3d electrons, the similarity of the Ni and Cu ion cores, and finally the interaction with the underlying fcc periodic potential.


2006 ◽  
Vol 73 (2) ◽  
Author(s):  
S. Czekaj ◽  
F. Nolting ◽  
L. J. Heyderman ◽  
P. R. Willmott ◽  
G. van der Laan

2014 ◽  
Vol 70 (a1) ◽  
pp. C225-C225
Author(s):  
N. G. Deshpande ◽  
C. H. Weng ◽  
Y. F. Wang ◽  
Y. C. Shao ◽  
D. C. Ling ◽  
...  

The electronic and magnetic properties of strained tetravalent-ion-doped La0.85Zr0.15MnO3 (LZMO) thin films that were epitaxially grown on SrTiO3 (STO) and MgO substrates were studied using temperature-dependent x-ray diffraction (XRD), x-ray absorption near-edge structure (XANES), x-ray linear dichroism (XLD) and x-ray magnetic circular dichroism (XMCD) at the Mn L3,2- and K-edge. XRD studies reveal that the LZMO thin films have compressive and tensile strains on the STO and MgO substrates, respectively. As temperature is reduced from room temperature to below magnetic transition temperature, the preferentially occupied Mn majority-spin eg orbital changes from the in-plane dx2-y2 to the out-of-plane d3z2-r2 orbital for LZMO/STO, and vice versa for LZMO/MgO. Experimental results suggest that the new hopping path that is mediated by the Mn2+ ions triggers a stronger d3z2-r2 orbital ordering of Mn3+ ions and enhances the ferromagnetic coupling between the Mn spin moments of t2g electrons in LZMO/STO, whereas the tensile strain stabilizes the dx2-y2 orbital by inducing lattice distortions of the MnO6 octahedra in LZMO/MgO.


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