Antieigenvalue theory

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In applied mathematics, antieigenvalue theory was developed by Karl Gustafson from 1966 to 1968. The theory is applicable to numerical analysis, wavelets, statistics, quantum mechanics, finance and optimization.

The antieigenvectors x {\displaystyle x} {\displaystyle x} are the vectors most turned by a matrix or operator A {\displaystyle A} {\displaystyle A}, that is to say those for which the angle between the original vector and its transformed image is greatest. The corresponding antieigenvalue μ {\displaystyle \mu } {\displaystyle \mu } is the cosine of the maximal turning angle. The maximal turning angle is ϕ ( A ) {\displaystyle \phi (A)} {\displaystyle \phi (A)} and is called the angle of the operator. Just like the eigenvalues which may be ordered as a spectrum from smallest to largest, the theory of antieigenvalues orders the antieigenvalues of an operator A from the smallest to the largest turning angles.

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