Hadamard

The '''Hadamard transform''' ('''Hadamard transformation''', also known as the '''Walsh-Hadamard transformation''') is an example of a generalized class of [[Fourier transform]]s. It is named for the [[France|French]] [[mathematician]] [[Jacques Hadamard]]. In [[quantum information processing]] the Hadamard transformation, more often called '''Hadamard gate''' in this context (cf. [[quantum gate]]), is a one-[[qubit]] [[rotation]], mapping the qubit-basis states |0› and |1› to two superposition states with equal weight of the computational basis states |0 \rangle and |1 \rangle . Usually the phases are chosen so that we have :\frac{|0\rangle+|1\rangle}{\sqrt{2}}\langle0|+\frac{|0\rangle-|1\rangle}{\sqrt{2}}\langle1| in [[Dirac notation]]. This corresponds to the [[transformation matrix]] :H=\frac{1}{\sqrt{2}}\begin{pmatrix} 1 & 1 \\ 1 & -1 \end{pmatrix} in the |0 \rangle , |1 \rangle basis. Many [[quantum algorithm]]s use the Hadamard transform as an initial step, since it maps ''n'' qubits initialized with |0› to a superposition of all 2''n'' orthogonal states in the |0 \rangle , |1 \rangle basis with equal weight. The Hadamard matrix can also be regarded as the [[Fourier transform]] on the two-element ''additive'' group of '''Z'''/(2). The Hadamard transform is used in many [[signal processing]], and [[data compression]] [[algorithms]]. ==See also== * [[Hadamard matrix]] {{FromWikipedia}} [[Category:Evolutions and Operations]]