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For a linear map , the dual map sends a linear functional on the output space to the input measurement . It reverses direction because a measurement of the output can be evaluated on an input by first applying :
For and , the input measurement is . The output measurement ignores the part of this transformation contributed by .
If has matrix in specified bases, a row representing changes to . Storing the coefficients of a linear functional as a column in the corresponding dual basis gives , explaining why the transpose of a linear map is represented by the matrix transpose. This algebraic operation uses no inner product; it agrees with a matrix transpose even over the complex numbers, rather than automatically introducing complex conjugation. The adjoint operator is defined using an inner product and is a different construction. [ref].
In finite dimension, the kernel and image of the dual map are described by annihilators of vector subspaces: