Bra-ket notation is a standard notation for describing quantum states in the theory of quantum mechanics composed of angle brackets and vertical bars. It can also be used to denote abstract vectors and linear functionals in pure mathematics. It is so called because the inner product of two states is denoted by a bracket,, consisting of a left part,, called the bra, and a right part,, called the ket. The notation was introduced in 1939 by Paul Dirac, and is also known as Dirac notation.
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