states, with n (7, of the two-electron ions from He through Ne +. The variational energies are the best available for 180 of the 261 states. Electron-nuclear and electron-electron cusp checks are used to test the wave functions. For each ion, dipole oscillator strengths are calculated for 55 S-P and 40 P-D transitions. Our oscillator strengths are more accurate than previous values for 739 of the 855 transitions considered. Some coefficients for the 1/Z expansions of the energies and oscillator strengths have been estimated as an aid to extrapolating our results to higher nuclear charges.PACS number(s): 32.70.Cs, 31. 20.Tz X k( -12) I e P(~krl~kr2 Ykr12) k=1 X YL 0( 0 ] ) Yo o ( Q~) in which Xis the number of terms, P]p is the permutation operator, the plus and minus signs refer to the singlet and triplet states, respectively, L is the total orbital angular in which r;=(r;, Q;) is the position vector of electron i for i = 1,2, r, z is the interelectronic distance, and Z is the nuclear charge. Schiff, Pekeris, and Accad [l], Kono and Hattori [2,3), and Sanders and Knight [4] all used Hylleraas-type [5] wave functions containing several hundred and, in some cases, a few thousand terms. We have previously [6 -8] shown that use of exponential correlation factors [5,9] can lead to compact wave functions of similar accuracy. Although our original work was restricted to low-lying states [6,7], the success of our ansatz for obtaining pseudospectra [8] encouraged us to expect that it would do well for more highly excited states as well. Thus, for the S and P states, we use spin free wave functions of the form [6 -8] 46 5397