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It is commonly believed that ($\alpha$-d) and (${^3}He$ - ${^3}H$) representequivalent states of ${^6}Li$. It is shown here that this is not correct. Thesetwo are actually orthogonal to each other. It is shown here that these two withvery different shapes and forms actually co-exist for the ground state of${^6}Li$. This shape co-existence is the same as similar phenomenon in heavynuclei. The puzzling anomaly of extremely small branching ratio for betadelayed deuteron emission in ${^6}He$ is explained here. In addition theanomalously large branching ratio for beta delayed triton emission in ${^8}He$is explained. The cluster structure of the ground state and of the low-lyingstates of ${^6}He$, ${^6}Li$ and ${^6}Be$ is clarified.Comment: Latex file, 8 pages, no figure

STRUCTURE OF A=6 NUCLEI: 6He, 6Li AND 6Be

STRUCTURE OF A=6 NUCLEI: ⁶He, ⁶Li AND ⁶Be