The Ir(110) surface is studied by STM, assisted by LEED and AES. The c
lean surface exhibits a mesoscopic ''rippling'' due to formation of (3
31) facets, confirming former results. The ''ridges'' formed by the in
clining and declining facets are up to several 100 Angstrom long in [1
(1) over bar 0] direction and have an average width of approximately 4
0 Angstrom, resulting in a quite rough topography on a mesoscopic scal
e. At the top of the ridges a close packed double row separating the f
acets has been found. The Ir(110) surface is the only known fcc(110) s
urface that exhibits stabilization via (331) facets, whereas Au(110) a
nd Pt(110) reconstruct in the (1 x 2) missing row structure with(111)
facets. (C) 1998 Elsevier Science B.V. All rights reserved.