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quantum probability theory – observables and states
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quantum algorithms:
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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
for an observable in the form of a Hermitean operator on the given Hilbert space of pure quantum states with Hermitian inner product
denoting the projection operator on a given eigenstate of this operator,
a pure state;
then the probability of observing the given eigenstate in a quantum system which is in state equals (in bra-ket notation):
In particular, if is an orthonormal basis for the Hilbert space of states associated with a quantum measurement-procedure, then the probability of measuring the result on a system in state is
and so if the state is normalized to begin with ( = 1 ), then the probability is
Essentially in this form the rule was first formulated by Born 1926b p 805.
quantum probability theory – observables and states
The Born rule is named in honor of
where it appears (though disregarding the norm symbol) as a brief footnote-added-in-proof:
\begin{imagefromfile} “file_name”: “Born_stating_the_BornRule-Footnote.jpg”, “width”: 500, 560, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
and its expanded version
which provides the mathematical details (p. 805):
\begin{imagefromfile} “file_name”: “Born_stating_the_BornRule-Expanded.jpg”, “width”: 460, 480, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
and finally in the followup
which makes the interpretation more explicit (p. 171):
\begin{imagefromfile} “file_name”: “Born_stating_the_BornRule-ExpandedII.jpg”, “width”: 500, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
Early The adoption generalization of the this Born idea rule: to probabilitydensities for continuous observables is due to Wolfgang Pauli, as first recounted in:
\begin{imagefromfile} “file_name”: “Jordan-PauliBornRule.jpg”, “width”: 510, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
and then by Pauli himself, again in a footnote:
\begin{imagefromfile} “file_name”: “PauliStatingBornPauliRule.jpg”, “width”: 540, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
Early review of the Born-Pauli rule:
where it is once again a footnote:
\begin{imagefromfile} “file_name”: “HilbertNeumannNordheim-BornRule.jpg”, “width”: 500, 530, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
and then in its full recognition and amplification as a pillar of quantum physics:
\begin{imagefromfile} “file_name”: “Dirac_OnBornPauliRule.jpg”, “width”: 530, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
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:
John von Neumann, Die quantenmechanische Statistik, Part III in:
Mathematische Grundlagen der Quantenmechanik, Springer (1932, 1971) [[doi:10.1007/978-3-642-96048-2](https://link.springer.com/book/10.1007/978-3-642-96048-2)]
Mathematical Foundations of Quantum Mechanics Princeton University Press (1955) [[doi:10.1515/9781400889921](https://doi.org/10.1515/9781400889921), Wikipedia entry]
\begin{imagefromfile} “file_name”: “vonNeumann-BornRule.jpg”, “width”: 500, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
\begin{imagefromfile} “file_name”: “vonNeumann-QMStatistics.jpg”, “width”: 500, “unit”: “px”, “margin”: { “top”: -20, “bottom”: 20, “right”: 0, “left”: 10 } \end{imagefromfile}
Historical survey:
Review:
See also:
Last revised on September 3, 2023 at 20:05:44. See the history of this page for a list of all contributions to it.