We use two old ideas for which layered structures are particularly relevant
. The first is that the pairing can occur in different parts of the unit ce
ll and interact symbiotically, behaving in some ways as a natural realizati
on of the sandwich models discussed in the early days of this conference. P
airing and large current flow in the CuO2 layers are enhanced by additional
pairing in other layers. The second idea is that additional pairing intera
ctions can be due to negative U-atoms (Tl+3-Tl+1), molecules (Hg-2(+2)-2Hg(
+2)), or due to interactions in the quasi one-dimensional Cu-O chain layers
of the YBCO-123 and 248 cuprates. Further, coulomb interactions in the CuO
2 planes between pairs moving in a and b directions lead to d-wave supercon
ductivity.