Magnetic-field decoupling of an alkali-metal excited-state hyperfine structure

1991 ◽  
Vol 43 (5) ◽  
pp. 2171-2178 ◽  
Author(s):  
W. A. van Wijngaarden ◽  
J. Sagle
2021 ◽  
Vol 502 (4) ◽  
pp. 5658-5667
Author(s):  
G C MacLeod ◽  
Derck P Smits ◽  
J A Green ◽  
S P van den Heever

ABSTRACT The first confirmed periodically varying 6.031 and 6.035 GHz hydroxyl masers are reported here. They vary contemporaneously with the 6.7 GHz methanol masers in G323.459–0.079. The 1.665 GHz hydroxyl and 12.2  GHz methanol masers associated with G323.459–0.079 are also periodic. Evidence for periodicity is seen in all features in all transitions save a single 1.665 GHz hydroxyl maser feature. Historical excited-state hydroxyl maser observations set a stricter upper limit on the epoch in which a significant accretion event occurred. The associated burst in 6.7 GHz methanol maser activity has subsided significantly while the hydroxyl transitions are brightening possibly the result of changing physical conditions in the masing cloudlets. Time lags in methanol are confirmed and may be the result of the periodic flaring propagating outward from the central region of maser activity. A possible magnetic field reversal occurred during the accretion event.


E.p.r. and endor spectra have been measured in ThO 2 containing Tb 4+ . The crystalline electric field is cubic, and the splittings are very large compared with other S state ions. The values of the parameters in the standard cubic spin-Hamiltonian are: g = 2·0146 ±0·0004, 60 B 4 = —2527·53 ±0·10 Mc/s, 1260 B 6 = —24·84 ± 0·04 Mc/s, A = —73·891 ±0·023 Mc/s, B = + 6·194 ± 0·038 Mc/s, μN ( 159 Tb) = + 1·994 ± 0·004 nuclear magnetons. There are also additional small high-order terms. There are very marked differences between these parameters and those for the other S state ions Gd 3+ and Eu 2+ . In addition to the much larger 60 B 4 , the g value is in excess of the free spin value; at the nucleus, the electrons produce a smaller magnetic field (proportional to A / g 1 ) and a larger electric field gradient (proportional to B / Q ) than they do in Gd 3+ and Eu 2+ . These differences are probably due to covalent bonding. The value of the nuclear moment of 159 Tb has been used to obtain a value of <r -3 > = 8·23 a.u. for Tb 3+ from the known hyperfine structure in Tb 3+ .


Sign in / Sign up

Export Citation Format

Share Document