The Mossbauer spectra of Gd2Fe17Hx (for x = 0, 3, and 5) and Sm2Fe17D5 have
been measured between 85 and 295 K and have been analysed with a model whi
ch takes into account the basal orientation of the iron magnetic moments, t
he near-neighbor environment of the four crystallographically inequivalent
iron sites, and the structural changes occurring upon hydrogen or deuterium
insertion. The temperature dependences of the individual iron site isomer
shifts and hyperfine fields follow the expected second-order Doppler shift
and Brillouin law behavior, respectively, and provide support for the adequ
acy of the fitting model. The increases in the isomer shifts upon going fro
m R2Fe17, to R2Fe17H3, to R2Fe17H5, and finally to R2Fe17N3, where R is a r
are-earth atom, correlate well with the observed increases in the unit-cell
volume and the iron Wigner-Seitz cell volumes upon hydrogen and nitrogen i
nsertion. The 85 K weighted average hyperfine field in R2Fe17 and R2Fe17H3
is at a maximum for the gadolinium compounds in agreement with their higher
Curie temperatures. Pr2Fe17H3 and Sm2Fe17N3, which both exhibit axial magn
etization, show large 85 K weighted average hyperfine fields than the remai
ning R2Fe17H3 and R2Fe17N3 compounds, respectively. Finally, the difference
s in the 18 h iron site environment, due to the insertion of the fourth and
fifth hydrogen atoms into R2Fe17H5, where R is Nd, Sm, and Gd, are not obs
erved in the Mossbauer spectra, and hence the hydrogen atoms on the 18 g te
trahedral interstitial sites must be rapidly moving on the Mossbauer timesc
ale. The magnetization curves of Sm2Fe17 and Sm2Fe17D5 have been measured a
t 5 and 300 K. The increase in the saturation magnetization upon deuterium
insertion is well explained by the increase in the Curie temperature and co
rrelates very well with the increase in the 85 K weighted average hyperfine
field. (C) 1999 Elsevier Science B.V. All rights reserved.