A new method has been developed to synthesize compact yttriumtrihydrid
e by making use of a thin film technique. For electrical measurements
yttrium films of typically 500 nm thickness are covered under UHV cond
itions by a 5 nm thick palladium overlayer which consists of electrica
lly disconnected islands. Loading of these films with hydrogen up to t
he trihydride phase can then be done ex-situ in a reasonably short tim
e (around 20-40 h) by applying gas pressures of about 60 x 10(5) Pa. F
or a thicker Pd layer (above 20 nm) this time can be considerably shor
ter (t similar to 125 s). The film morphology stays intact during the
loading process although the film thickness increases by approximately
11% and the crystal structure changes from h.c.p. to f.c.c. and back
to h.c.p. These samples are: therefore, very well suited for an invest
igation of the remarkable electrical and optical properties of trihydr
ides, as recently reported by Huiberts et al. (Nature, 380, 1996, 231)
. In this article we give evidence for the island structure of the pal
ladium overlayer and make a comparison of a number of physical propert
ies of yttrium and its related hydrides as thin films with literature
values for the same material in bulk form. These properties include la
ttice parameters for the different hydride phases, electrical resistiv
ity for yttrium and its dihydride and Hall coefficient for yttrium. Th
e characteristics of the yttriumhydride thin films are very similar to
those of bulk material. Furthermore, we performed concentration measu
rements and resistivity measurements during hydrogen loading. It is sh
own that the resistivity rises three orders of magnitude when yttrium
is loaded up to the trihydride phase at 60 X 10(5) Pa.