X-ray absorption near edge spectroscopy at the Mn K-edge in highly homogeneous GaMnN diluted magnetic semiconductors

2006 ◽  
Vol 243 (7) ◽  
pp. 1692-1695 ◽  
Author(s):  
O. Sancho-Juan ◽  
A. Cantarero ◽  
G. Martínez-Criado ◽  
D. Olguín ◽  
N. Garro ◽  
...  
2008 ◽  
Vol 1111 ◽  
Author(s):  
Shuichi Emura ◽  
Masahiro Takahashi ◽  
Hiroyuki Tambo ◽  
Akira Suzuki ◽  
Tetsuya Nakamura ◽  
...  

AbstractThe magnetic characteristics of the dilute magnetic system GaGdN are investigated by mainly soft-X-ray magnetic circular dichroism (MCD) in energy range of 1160 – 1240 eV. The strong MCD signals up to 30 % at 15K are observed. The temperature dependence of its intensity is not on simple Curie-Weiss curve and depicts three-step curve. A step around 40 – 100K suggests a new magnetic phase. The luminescence spectrum of GaGdN at low temperature is divided into three parts consisting of two broad bands around 432 nm and 503 nm and a sharp peak at 652 nm. This sharp line is assigned to the intra-transition of f – f orbital owing to the weak temperature dependence of the intensity and peak position. AlGdN grown by molecular beam epitaxy produces luminescence at 318.5 nm. X-ray absorption fine structure is examined to survey the occupancy of the Gd ion in the grown specimens.


2013 ◽  
Vol 2013 ◽  
pp. 1-10 ◽  
Author(s):  
V. N. Antonov ◽  
L. V. Bekenov ◽  
L. P. Germash ◽  
N. A. Plotnikov

The electronic structure of the Co-doped indium tin oxide (ITO) diluted magnetic semiconductors (DMSs) were investigated theoretically from first principles, using the fully relativistic Dirac linear muffin-tin orbital band structure method. The X-ray absorption spectra (XAS) and X-ray magnetic circular dichroism (XMCD) spectra at the Co L3, In M2, Sn M2, and O K edges were investigated theoretically from first principles. The origin of the XMCD spectra in these compounds was examined. The calculated results are compared with available experimental data.


2010 ◽  
Vol 22 (21) ◽  
pp. 216006 ◽  
Author(s):  
R Gunnella ◽  
L Morresi ◽  
N Pinto ◽  
A Di Cicco ◽  
L Ottaviano ◽  
...  

2006 ◽  
Vol 243 (7) ◽  
pp. 1696-1700 ◽  
Author(s):  
J. I. Hwang ◽  
Y. Ishida ◽  
M. Kobayashi ◽  
Y. Osafune ◽  
T. Mizokawa ◽  
...  

1994 ◽  
Vol 375 ◽  
Author(s):  
Y. L. Soo ◽  
S. W. Huang ◽  
Z. H. Ming ◽  
Y. H. Kao ◽  
H. Munekata ◽  
...  

AbstractExtended x-ray absorption fine structure (EXAFS) techniques have been used to investigate the local structures in Inl-xMnxAs films grown by molecular beam epitaxy (MBE) under different processing conditions. For samples grown at low substrate temperatures (near 200°C) or with a low Mn concentration (about 1 atomic%), the Mn atoms can substitute for In in the InAs host, thus indicating that III-V diluted magnetic semiconductors (DMS) can indeed be prepared by substitutional doping of magnetic impurities. On the other hand, substitution dose not take place in high Mn concentration (above 10%) samples grown at high substrate temperatures (around 300°C); these samples contain a large amount of MnAs clusters and become ferromagnetic


2004 ◽  
Vol 95 (7) ◽  
pp. 3573-3575 ◽  
Author(s):  
J. Okabayashi ◽  
K. Ono ◽  
M. Mizuguchi ◽  
M. Oshima ◽  
Subhra Sen Gupta ◽  
...  

2013 ◽  
Vol 785-786 ◽  
pp. 582-585
Author(s):  
Zhi Qiang Wei ◽  
Xiao Juan Wu ◽  
Ling Ling Zhang ◽  
Wang Jun Feng ◽  
Hua Yang

Ni-doped ZnO diluted magnetic semiconductors nanorods were successfully synthesized by hydrothermal method. The crystal structure, morphology, constituent elements and optical proprety of the products using this method were investigated via X-ray diffraction (XRD), transmission electron microscopy (TEM), X-ray energy dispersive spectrometry (XEDS) and ultraviolet-visible spectroscopy (UV-vis). The experiment results show that the morphology of samples were nanorods with good dispersion, all the diffraction peaks correspond to the wurtzite structure hexagonal phase, no other impurity phase appeare, and the Ni2+ions successfully substituted for the lattice site and generate single-phase Zn1-xNixO. The band gap increases firstly and reduces afterward with the increase of Ni2+contents.


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