Hcp Cu has been grown by epitaxy on the W(100) surface. The epitaxial
relationship of the hcp films is determined by RHEED as (11 (2) over b
ar 0) parallel to (100) and [1 (1) over bar 00] parallel to [011]. The
growth of Cu in the hcp structure is attributed to the small energy d
ifference between the hcp and fee structure and the much smaller misfi
t of this hcp orientation in the [1 (1) over bar 00] direction than of
any fee orientation. The RHEED oscillations at 150 K show a differenc
e between the period of the even and odd oscillations, that coincides
with changes in UPS intensity at selected energies. The electronic str
ucture of the thin him grown at 150 and 300 K shows only small differe
nces, At 500 K and above. the Cu grows in high and narrow islands.