We study why gold forms planar and cage-like clusters while copper and silver do not. We use density functional theory and norm-conserving pseudo-potentials with and without a scalar relativistic component. For the exchange-correlation (xc) functional we use both the generalized gradient (GGA) and the local density (LDA) approximations. We find that planar Aun structures, with up to n = 11, have lower energy than the three-dimensional isomers only with scalar-relativistic pseudopotentials and the GGA. In all other calculations, with more than 6 or 7 noble metal atoms, we obtain three dimensional structures. However, as a general trend we find that planar structures are more favorable with GGA than with LDA. In the total energy balance, kinetic energy favors planar and cage structures, while xc-energy favors 3D structures. As a second step, we construct cluster structures having only surface atoms with O h , T d , and I h symmetry. Then, assuming one valence electron per atom, we select those with 2(l + 1) 2 electrons (with l integer), which correspond to the filling of a spherical electronic shell formed by node-less one electron wave functions. Using scalar relativistic GGA molecular dynamics at T = 600K, we show that the cage-like structures of neutral Au32, Au50, and Au162 are meta-stable. Finally, we calculate the static polarizability of the two lowest energy isomers of Aun clusters as a means to discriminate isomers with planar (or cagelike) geometry from those with compact structures. We also fit our data to a semi-empirical relation for the size dependent polarizability which involves the effective valence and the kinetic energy components for the homogeneous and inhomogeneous electron density. Analyzing that fit, we find that the dipole polarizability of gold clusters with planar and cage-like structures corresponds to the linear response of 1.56 delocalized valence electrons, suggesting a strong screening of the valence interactions due to the d-electrons.