nLab Born rule

Contents

Context

Quantum systems

quantum logic


quantum physics


quantum probability theoryobservables and states


quantum information


quantum technology


quantum computing

Probability theory

Contents

Idea

The Born rule is the core statement of coordination in the foundations of quantum physics:

In its version for pure states the Born rule says that

then the probability of observing the given eigenstate in a quantum system which is in state ψ\psi equals (in bra-ket notation):

ψ|P|ψψ|ψ. \frac{ \langle \psi \vert P \vert \psi \rangle }{ \langle \psi \vert \psi \rangle } \,.

In particular, if WW is an orthonormal basis for the Hilbert space of states associated with a quantum measurement-procedure, then the probability of measuring the result ww on a system in state |ψ\left\vert \psi \right\rangle is

ψ|ww|ψψ|ψ=|w|ψ| 2ψ|ψ \frac{ \langle \psi \vert w \rangle \langle w \vert \psi \rangle }{ \langle \psi \vert \psi \rangle } \;\;=\;\; \frac{ \big\vert \langle w \vert \psi \rangle \big\vert^2 }{ \langle \psi \vert \psi \rangle }

and so if the state is normalized to begin with (ψ|ψ\langle \psi \vert \psi \rangle = 1 ), then the probability is

P ψ(w)=|w|ψ| 2. P_\psi(w) \;=\; \big\vert \langle w \vert \psi \rangle \big\vert^2 \,.

Essentially in this form the rule was first formulated by Born 1926b p 805.

quantum probability theoryobservables and states

References

Historical origins

The Born rule is named in honor of

where it appears (though disregarding the norm symbol) as a brief footnote-added-in-proof:

and its expanded version

which provides the mathematical details (p. 805):

and finally in the followup

which makes the interpretation more explicit (p. 171):

The generalization of this idea to probability densities for continuous observables is due to Wolfgang Pauli, as first recounted in:

and then by Pauli himself, again in a footnote:

Early review of the Born-Pauli rule:

where it is once again a footnote:

and in

The full recognition and amplification of the Born rule as a pillar of quantum physics making it a probabilistic theory (cf. quantum probability) is (maybe besides Jordan 1927) due to:

Historical survey:

  • Jagdish Mehra, Helmut Rechenberg, The Probability Interpretation and the Statistical Transformation Theory, the Physical Interpretation, and the Empirical and Mathematical Foundations of Quantum Mechanics 1926-1932, Part 1 in: The Historical Development of Quantum Theory. Volume 6: The Completion of Quantum Mechanics, 1926-1941, Springer (2001) [ISBN:978-0-387-98971-6]

Further discussion

Review:

See also:

Last revised on February 14, 2025 at 08:46:21. See the history of this page for a list of all contributions to it.