dual space
The dual space is the companion space inhabited by bras, sitting alongside the space of kets. Where a ket is a quantum state, its bra is a kind of measuring device: a rule that takes any ket and returns a complex number. The collection of all such rules forms its own vector space, the dual, which is the natural home of every bra ⟨φ|.
There is a perfect one-to-one matching between the two spaces. To each ket |ψ⟩ corresponds exactly one bra ⟨ψ|, found by Hermitian conjugation — transposing and complex-conjugating. The pairing is not quite a plain copy: multiply a ket by a complex number c and its matching bra is multiplied by the conjugate c* instead. This twist is precisely what makes inner products behave correctly and lengths come out real and positive.
Why split states into two spaces at all? Because it cleanly separates the two jobs a state has to do. As a ket it is something that can be transformed and evolved; as a bra it is something that reads out information from other states. Bringing a bra from the dual space together with a ket gives the inner product — a number — and that meeting of the two spaces is where measurable quantities are born.
Every ket in the Hilbert space H has exactly one matching bra in the dual space H*.
The matching between kets and bras is antilinear, not linear: scaling a ket by a complex number scales its bra by the complex conjugate. Forgetting this conjugate is a common source of sign and phase errors.