The XANES region of the LII and LIII absorption discontinuities of some rare earths in their oxides and cuprates is studied. The main absorption peak and the peak adjacent to it are attributed to the transitions of electrons from the inner L levels to the outer levels t2g and eg, which are formed due to the crystalline field in the materials. It is observed that the energy difference between these two peaks varies linearly with the atomic number Z for the oxides as well as the cuprates
L3-X-ray absorption near edge structure (XANES) of valence susceptible 4f lanthanide ions, Eu and Yb...
In this disseration we focus on luminescent materials. They are able to emit light, which is not cau...
The intensities are studied of the white lines associated with the LII and LIII absorption discontin...
Energies of the 1s→3d. 1s→4s and 1s→4p transitions of Mn, Fe and Co in a series of...
Energies of the 1s → 3d. 1s → 4s and 1s → 4p transitions of Mn, Fe and Co in a series of oxides have...
We have found a genaral rule that links the presence of a particular feature at about 20 eV from the...
The shape and near edge structure of the LIII absorption discontinuity of tungsten in some rare eart...
Characteristic features of Ho, Er, and Yb L<sub>1</sub>-edge and L<sub>3</sub>-edge XANES spectra of...
La L<sub>1</sub> and L<sub>3</sub>-edge X-ray absorption near-edge structure (XANES) of various La o...
Pr, Nd, and Sm L<sub>1</sub>-edge and L<sub>3</sub>-edge X-ray absorption near edge structure (XANES...
L3 and L1 X-ray absorption spectra of single crystals of TmSe and Tm metal were measured at the sync...
Variation of electronic structure at the Fermi level in superconducting LaRu2 intermetallic system h...
Two now X-ray curved crystal vacuum spectrometers are described. With the first of these the LX1,2 l...
A deconvolution procedure has been applied to K-edge X-ray absorption near-edge structure (XANES) sp...
A deconvolution procedure has been applied to K-edge X-ray absorption near-edge structure (XANES) sp...
L3-X-ray absorption near edge structure (XANES) of valence susceptible 4f lanthanide ions, Eu and Yb...
In this disseration we focus on luminescent materials. They are able to emit light, which is not cau...
The intensities are studied of the white lines associated with the LII and LIII absorption discontin...
Energies of the 1s→3d. 1s→4s and 1s→4p transitions of Mn, Fe and Co in a series of...
Energies of the 1s → 3d. 1s → 4s and 1s → 4p transitions of Mn, Fe and Co in a series of oxides have...
We have found a genaral rule that links the presence of a particular feature at about 20 eV from the...
The shape and near edge structure of the LIII absorption discontinuity of tungsten in some rare eart...
Characteristic features of Ho, Er, and Yb L<sub>1</sub>-edge and L<sub>3</sub>-edge XANES spectra of...
La L<sub>1</sub> and L<sub>3</sub>-edge X-ray absorption near-edge structure (XANES) of various La o...
Pr, Nd, and Sm L<sub>1</sub>-edge and L<sub>3</sub>-edge X-ray absorption near edge structure (XANES...
L3 and L1 X-ray absorption spectra of single crystals of TmSe and Tm metal were measured at the sync...
Variation of electronic structure at the Fermi level in superconducting LaRu2 intermetallic system h...
Two now X-ray curved crystal vacuum spectrometers are described. With the first of these the LX1,2 l...
A deconvolution procedure has been applied to K-edge X-ray absorption near-edge structure (XANES) sp...
A deconvolution procedure has been applied to K-edge X-ray absorption near-edge structure (XANES) sp...
L3-X-ray absorption near edge structure (XANES) of valence susceptible 4f lanthanide ions, Eu and Yb...
In this disseration we focus on luminescent materials. They are able to emit light, which is not cau...
The intensities are studied of the white lines associated with the LII and LIII absorption discontin...