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Composite superfield operators $\\Y_{(a,b)}$ are products of the elementary chiral superfields $S$ and $\\ov S$ and the derivative operators $D_\\a$, $\\ov D_{\\dot \\b}$ and $\\pa_{\\a \\dot \\b}$. Such superfields $\\Y_{(a,b)}$ can be chosen to have `$a$' symmetrized undotted indices $\\a_i$ and `$b$' symmetrized dotted indices $\\dot \\b_j$. 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