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Given a subspace basis \( \beta = \setlr{ \Bx_1, \Bx_2, \cdots \Bx_m } \), not
necessarily orthonormal, the \textit{reciprocal frame} is the set \( \setlr{ \Bx^1, \Bx^2, \cdots \Bx^m } \in \Span \beta \) satisfying
\begin{equation*}
\Bx_i \cdot \Bx^j = {\delta_i}^j,
\end{equation*}
where the vector \( \Bx^j \) is not the j-th power of \( \Bx \), but is a superscript index, the conventional way of denoting a reciprocal frame vector, and \( {\delta_i}^j \) is the Kronecker delta.