We have measured the electrical resistivity in the range 1.5-300 K of the h
ydrogenated alloy system YyTb1-yH(D)(x), for y = 0.9 and 0.2, and for hydro
gen concentrations 0 less than or equal to x less than or equal to 0.25. It
is found that, in the case y = 0.9, hydrogen forms alpha*-solid solutions
up to concentrations x(max)(alpha)*=0.21(1). Like in binary alpha*-YHx, one
observes ordering in the H sublattice near 170 K; a correlation between th
e periodicity of the helical antiferromagnetic (AF) structure in this alloy
and that of the modulated chainlike H-H pair configuration in the ordered
H sublattice is noted. For y = 0.2, hydrogen precipitates at once as dihydr
ide, which is, e.g., seen through the emergence of an H-dependent peak at 1
0 K due to the AF transition of beta-TbH2; the same is also noted, for x>x(
max)(alpha)* in the case y = 0.9. Hydrogen influences the various magnetic
structures present by generally weakening the Ruderman-Kittel-Kasuya-Yosida
polarization interaction. Thus, H addition results in a decrease of the sp
in-disorder scattering and of the magnetic manifestations at T-N(Tb) and T-
C(Tb). The low-T intrinsic resistivities are analyzed in terms of various t
ypes of spin-wave spectra for the two alloys and their interaction with hyd
rogen. [S0163-1829(99)10513-7].