Super Hyperfine Structure in the EPR Spectrum of Divalent Manganese in Single Crystal Zinc Selenide

1990 ◽  
Vol 160 (2) ◽  
pp. 591-600 ◽  
Author(s):  
S. A. Marshall ◽  
D. R. Yoder-Short ◽  
C. Yu ◽  
Y. N. Zhang ◽  
J. K. Furdyna
1982 ◽  
Vol 59 (1-2) ◽  
pp. 183-188 ◽  
Author(s):  
P.L. Jones ◽  
D. Moore ◽  
D.R. Cotton

1982 ◽  
Vol 49 (2) ◽  
pp. 225-232
Author(s):  
T Lionel ◽  
J.R Morton ◽  
K.F Preston
Keyword(s):  

2019 ◽  
Vol 54 (4) ◽  
pp. 1800231 ◽  
Author(s):  
Narsingh Bahadur Singh ◽  
Ching-Hua Su ◽  
Bradley Arnold ◽  
Fow-Sen Choa ◽  
Brian Cullum ◽  
...  

2003 ◽  
Vol 377 (3-4) ◽  
pp. 367-370 ◽  
Author(s):  
Ying-Chun Zhu ◽  
Yoshio Bando
Keyword(s):  

1965 ◽  
Vol 43 (12) ◽  
pp. 2361-2373 ◽  
Author(s):  
David J. Griffiths ◽  
Hans Glättli

The technique of detecting electron paramagnetic resonance and measuring paramagnetic relaxation times at liquid-helium temperatures by the magneto-optical Faraday rotation has been applied to the even number (4f2) electron system of Pr3+ in praseodymium ethylsulphate (PrES). The EPR spectrum (X band) of undiluted PrES at 1.37 °K is a broad band extending over several kilo-gauss with no evidence of hyperfine structure. The band intensity decreases at [Formula: see text] and covers [Formula: see text] from its maximum to half-power point. The absence of any hyperfine structure indicates that crystal-field distortion is the main source of line broadening.The relaxation times measured as a function of temperature over the range 1.40 to 2.18 °K and at 4.22 °K range from 0.1 to 10 msec. For [Formula: see text], τ decreases from 0.40 to 0.15 msec, is proportional to T−(3.5 ± 0.6), and is considered to be the phonon–bath relaxation time. Values of τ show a scatter within 0.20 ± 0.02 msec for [Formula: see text]. Near the λ point [Formula: see text], τ exhibits a very rapid increase, having a value of 0.20 msec at 2.155 °K and 0.85 msec at 2.165 °K. This behavior appears to be related to the energy exchange between the crystal and liquid-helium bath. Measurements of τ at 2.18 °K and 4.22 °K indicate that the rate at which the spin–phonon system returns to initial thermal equilibrium is governed by the thermal conductivity of the liquid-helium bath.


1992 ◽  
Vol 41 (7) ◽  
pp. 1196-1199
Author(s):  
A. V. Il'yasov ◽  
L. A. Kazitsyna ◽  
I. D. Morozova ◽  
A. A. Vafina ◽  
V. I. Morozov ◽  
...  

1986 ◽  
Vol 25 (10) ◽  
pp. 1650-1654 ◽  
Author(s):  
Karl Wieghardt ◽  
Wolfgang Walz ◽  
Bernhard Nuber ◽  
Johannes Weiss ◽  
Andrej Ozarowski ◽  
...  

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