Superhyperfine structure of the EPR spectra of impurity ions in the LiYF4 : Nd3+ system doped by 143Nd isotopes

2015 ◽  
Vol 57 (12) ◽  
pp. 2400-2403 ◽  
Author(s):  
L. K. Aminov ◽  
M. R. Gafurov ◽  
S. L. Korableva ◽  
I. N. Kurkin ◽  
A. A. Rodionov
2018 ◽  
Vol 60 (5) ◽  
pp. 912-915
Author(s):  
L. K. Aminov ◽  
M. R. Gafurov ◽  
I. N. Kurkin ◽  
B. Z. Malkin ◽  
A. A. Rodionov

1992 ◽  
Vol 13 (1) ◽  
pp. 18-20 ◽  
Author(s):  
Yu.S. Gromovoj ◽  
S.V. Plyatsko ◽  
G.E. Kostyunin

2017 ◽  
Vol 59 (3) ◽  
pp. 564-568 ◽  
Author(s):  
L. K. Aminov ◽  
M. R. Gafurov ◽  
S. L. Korableva ◽  
I. N. Kurkin ◽  
A. A. Rodionov

1986 ◽  
Vol 89 ◽  
Author(s):  
Marian Bartkowski ◽  
D. J. Northcott ◽  
A. H. Reddoch ◽  
D. F. Williams ◽  
F. T. Hedgcock ◽  
...  

AbstractThe EPR spectra of manganese and gadolinium doped PbTe and SnTe semiconductors were measured from 4.2K up to 400K for dopant concentrations ranging from 50 to 50000 ppm. Resolved fine, hyperfine and superhyperfine structure as well as forbidden and cluster lines were measured. The combination of Lorentzian absorption and dispersion derivatives fits the recorded spectra well. Nonlinear broadening of linewidths with temperature is characteristic in these semiconductors. A manganese-induced broad maximum in linewidth versus temperature was found in PbTe around 180K for dopant concentrations in excess of 1.5at%.


1982 ◽  
Vol 60 (11) ◽  
pp. 1573-1588 ◽  
Author(s):  
V. M. Malhotra ◽  
H. A. Buckmaster

The 34 GHz EPR spectra of 5-state (4f7, 8S) Gd3+ impurity ions (~1%) in the isostructural [Formula: see text] symmetry Ln(OH)3 host lattice (Ln ≡ La, Sm, Eu, Tb, Ho, Y) have been studied at 77 and 294 K. The expected seven line ΔM = ± 1 spectrum is observed for Ln = La, Eu, Ho, and Y whereas only a single broad transition is observed for Ln ≡ Sm and Tb. The observed values of the zero field splitting (ZFS) parameter B20 as well as the TZFS are found to be related linearly to (i) the ionic radius, (ii) the Ln–O1 distance, and (iii) the Ln–O2 distance where O1 and O2 are the nearest neighbour equatorial and apical oxygens. However, the slopes are opposite to that predicted by a point charge lattice model. This paper discusses (i) the SH parameters, (ii) the host lattice effect, (iii) the ZFS processes, and (iv) the linewidths observed in the Ln(OH)3 host lattice and attempts to explain the observations using the existing theory. It is found that this apparently simple host lattice exhibits complex effects which do not change systematically with the host lanthanide ion, unlike that observed in most other isostructural lanthanide hosts that have been studied using Gd3+ impurity ions.


2008 ◽  
Vol 33 (4) ◽  
pp. 351-364 ◽  
Author(s):  
L. K. Aminov ◽  
A. A. Ershova ◽  
D. G. Zverev ◽  
S. L. Korableva ◽  
I. N. Kurkin ◽  
...  

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