4À unit is characterized by the shortest GeÀGe distance (2.390(1) ) ever observed in aZintl phase and thus represents the first Ge = Ge double bond under such conditions,a sa lso suggested by the (8ÀN) rule.R aman measurements support these findings.T he multiple-bond character is confirmed by electronic-structure calculations,and an upfield 6 Li NMR shift of À10.0 ppm, whichwas assigned to the Li cations surrounded by the p systems of three Ge dumbbells,further underlines this interpretation. Fort he unperturbed, ligand-free dumbbell in Li 3 NaGe 2 ,the p-bonding p y and p z orbitals are degenerate as in molecular oxygen, which has singly occupied orbitals.T he partially filled p-type bands of the neat solid Li 3 NaGe 2 cross the Fermi level, resulting in metallic properties.Li 3 NaGe 2 was synthesized from the elements as well as from binary reactants and subsequently characterized crystallographically.Multiple bonds of the heavier homologues of boron, carbon, and nitrogen have been intensively investigated during the last decades.[1-3] Among those,t he heavier tetrel homologues all adopt a trans-bent structure in contrast to planar ethylene.The pyramidalization at the Eatom in R 2 E= ER 2 drastically influences the possibility of forming aclassical p bond between the two metal atoms for E = Ge,Sn, and Pb.TheC GMT model proposed by Tr inquier and Malrieu [4] traces the deviation from planarity in R 2 E=ER 2 molecules back to the relative values of the singlet and triplet energies of the monomeric units ER 2 (E S and E T ,r espectively) and the energy of the double-bonded system:F or E s+ +p > 2 DE SÀT ac lassical planar structure is obtained, whereas E s+ +p < 2 DE SÀT favors the trans-bent structure.E s+ +p < DE SÀT results in monomeric ER 2 fragments without E À Eb onding. [1,5] Theinteratomic EÀEdistance is another strong indicator for the bond order.S cheme 1g ives an overview of several homonuclear double-bonded Si and Ge species.F or secondrow elements,double bonds are considerably shorter than the sum of the covalent radii, whereas for the heavier homologues,d eviations occur owing to the strict requirements of the bulky ligands that are often used to stabilize the reactive bonds or owing to electrostatic repulsion in the case of charged systems.F or example,i nR 2 Ge = GeR 2 ,t he Ge À Ge bond lengths are in the range of 2.21 to 2.51 , [2] most of them being shorter than aG e ÀGe single bond (2.44 ), but for [RGe=GeR] 2À ,greater bond lengths are observed.[6]In general, trans-bent structures are energetically favored over planar structures.L igand-free and thus symmetrically unperturbed germanide dumbbells have been observed in Zintl phases. [7] Assuming acomplete valence electron transfer in BaMg 2 Ge 2 ,a14 valence electron [GeÀGe] 6À dumbbell should be obtained. However,t he GeÀGe bond (2.58 ) [8] is significantly longer than atypical Ge single bond, which was sketchily explained by Coulombic repulsion of the negatively charged atoms.R ecently,t he strong interaction of alkalineearth metal dstat...