Communication: Molecular dynamics simulations of the interfacial structure of alkali metal fluoride solutions Intercalation of heavy alkali metals (K, Rb and Cs) in the bundles of single wall nanotubes AIP Conf.Liquid alloys of metals with mercury ͑amalgams͒ are used to synthesize the fullerides A n Hg x C 60 ͑A=K,Rb,Cs; n =2;3; x Ͻ 1͒, A n Tl m Hg x C 60 ͑A=K,Rb,Cs; n =1;2; m = 0.25-2; x Ͻ 1͒, and Na n C 60 ͑n=2,3͒. The samples are studied by x-ray diffraction, nuclear magnetic resonance, electron paramagnetic resonance, Raman scattering, and differential scanning calorimetry. The Na n C 60 ͑n=2,3͒ fullerides are not superconducting. Structural phase transitions are observed in them as the temperature is varied. K 2 Hg x C 60 is a superconductor with a transition temperature T c = 22 K, while K 3 Hg x C 60 is not superconducting. Rb n Hg x C 60 ͑n=2,3͒ are superconductors with T c = 24-25 K. The cesium fullerides with an assumed composition of Cs n Hg x C 60 ͑n=1-3͒ are either polymers ͑n=2,3͒ or crystallize in a rhombic lattice, but none are superconducting. A maximum T c = 22 K is observed in the K 2 Tl m Hg x C 60 fulleride with a thallium concentration m = 0.5. Cs n Tl m Hg x C 60 ͑n=1-3; m=1,2͒ is not superconducting, but KCsTlC 60 produced by means of exchange reactions with TlCl is a superconductor with T c = 21.7 K.