An attempt is made in this paper to present the characteristic structural features of rare metals in the liquid state, particularly liquid 3d transition metals and 4f rare earth metals. The first peak of the structure factors of rare metals is quite symmetrical, and the profile looks quite similar to those of such simple cases as Al, in contrast to Zn and Sn which show an asymmetrical first peak, or a small hump on the high angle side of the first peak in the structure factors. However, the oscillations in the structure factor systematically increase in amplitude as the atomic number increases from Ti to Ni or from Ce to Yb. This gives qualitative support for the suggestion that the partial overlap between atoms which have a nearly empty 3d-shell or 4f-shell, such as Ti or Ce, is larger than of those having a nearly filled 3d-shell or 4f-shell, such as Ni or Yb. Clearer evidence of such overlap effects, mainly related to the outer electronic shell, was detected in liquid Ce alloys with Co and Ni. For quantitative discussion about these interesting structural features, further information on the valence electron distribution around an ion is required. The principle of a new method for estimating such information in liquid metals from measured structural data recently proposed has also been described, with some selected examples. -IB) Model 1 ^ J Eu 4f 7 6s 2 J C· 4f 2 6s 2 J V ~ "" Q' -Q/Q]Fig. 3: Reduced structure factors of 3d and 4f metals in the liquid state. Qi is the first peak position in S(Q).determined by high temperature x-ray diffraction 15,6/. The basic profile of the structure factors for 23 rare metals, including 12 lanthanoid elements, were found to be similar to those of simple metals such as 13 Brought to you by | Purdue University Libraries Authenticated Download Date | 6/17/15 10:48 PM