This is the same as the condition hψ|ψi = 1, i.e., the state |ψi must be
normalized, or be a unit vector in Hilbert space. A state vector that does not
have unit norm can be normalized by dividing it by its norm.
The first axiom of quantum mechanics is a statement that embodies all
this.
Exercise 3.1. Normalize the vectors
“
1
1
#
and
“
1
−1
#
. Show that they are
orthogonal.
Exercise 3.2. Normalize the state |0i − 2i|1i.

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