Κανών Born


Μαθηματικό Θεώρημα Νόμοι Μαθηματικών
Φυσικός Νόμος Νόμοι Φυσικής
Νόμοι Χημείας
Νόμοι Γεωλογίας
Νόμοι Βιολογίας
Νόμοι Οικονομίας

Τεχνολογία
Επιστημονικός Κλάδος Επιστημονικός Νόμος Επιστημονική Μέθοδος Επιστημονική Θεωρία Επιστημονικά Κέντρα Γης Επιστήμονες Γης
- Ακριβέστερα, είναι ένας νόμος της Κβαντικής Φυσικής
Ετυμολογία[]
Η ονομασία "νόμος" σχετίζεται ετυμολογικά με το όνομα του φυσικού επιστήμονα "[[ ]]".
Διατύπωση[]
The Born rule (also called the Born law, Born's rule, or Born's law) is a law of quantum mechanics which gives the probability that a measurement on a quantum system will yield a given result. It is named after its originator, the physicist Max Born. The Born rule is one of the key principles of quantum mechanics. There have been many attempts to derive the Born rule from the other assumptions of quantum mechanics, with inconclusive results.
The rule[]
The Born rule states that if an observable corresponding to a Hermitian operator with discrete spectrum is measured in a system with normalized wave function (see bra–ket notation), then
- the measured result will be one of the eigenvalues of , and
- the probability of measuring a given eigenvalue will equal , where is the projection onto the eigenspace of corresponding to .
- (In the case where the eigenspace of corresponding to is one-dimensional and spanned by the normalized eigenvector , is equal to , so the probability is equal to . Since the complex number is known as the probability amplitude that the state vector assigns to the eigenvector , it is common to describe the Born rule as telling us that probability is equal to the amplitude-squared (really the amplitude times its own complex conjugate). Equivalently, the probability can be written as .)
In the case where the spectrum of is not wholly discrete, the spectral theorem proves the existence of a certain projection-valued measure , the spectral measure of . In this case,
- the probability that the result of the measurement lies in a measurable set will be given by .
If we are given a wave function for a single structureless particle in position space, this reduces to saying that the probability density function for a measurement of the position at time will be given by
History[]
The Born rule was formulated by Born in a 1926 paper.[1]
In this paper, Born solves the Schrödinger equation for a scattering problem and, inspired by Einstein's work on the photoelectric effect,[2] concluded, in a footnote, that the Born rule gives the only possible interpretation of the solution. In 1954, together with Walther Bothe, Born was awarded the Nobel Prize in Physics for this and other work. John von Neumann discussed the application of spectral theory to Born's rule in his 1932 book.[3]
Interpretations[]
While it has been claimed that Born's law can be derived from the Many Worlds Interpretation, the existing proofs have been criticized as circular.[4] Within the Quantum Bayesianism interpretation of quantum theory, the Born rule is seen as an extension of the standard Law of Total Probability, which takes into account the Hilbert space dimension of the physical system involved.[5] In the ambit of the so-called Hidden-Measurements Interpretation of quantum mechanics the Born rule can be derived by averaging over all possible measurement-interactions that can take place between the quantum entity and the measuring system.[6][7]
Υποσημειώσεις[]
- ↑ Born, Max (1926). Wheeler, J. A.; Zurek, W. H.. επιμ. Zur Quantenmechanik der Stoßvorgänge. Princeton University Press. 1983. σελ. 863–867. doi: . ISBN 0-691-08316-9.
- ↑ Born, Max (11 December 1954). The statistical interpretation of quantum mechanics. www.nobelprize.org. nobelprize.org. http://www.nobelprize.org/nobel_prizes/physics/laureates/1954/born-lecture.pdf. Ανακτήθηκε την 30 December 2016. "Again an idea of Einstein's gave me the lead. He had tried to make the duality of particles - light quanta or photons - and waves comprehensible by interpreting the square of the optical wave amplitudes as probability density for the occurrence of photons. This concept could at once be carried over to the psi-function: |psi|2 ought to represent the probability density for electrons (or other particles)."
- ↑ Neumann (von), John (1932). Mathematische Grundlagen der Quantenmechanik. Princeton University Press (δημοσιεύθηκε 1996). ISBN 0691028931.
- ↑ N.P. Landsman, "The conclusion seems to be that no generally accepted derivation of the Born rule has been given to date, but this does not imply that such a derivation is impossible in principle.", in Compendium of Quantum Physics (eds.) F.Weinert, K. Hentschel, D.Greenberger and B. Falkenburg (Springer, 2008), ISBN 3-540-70622-4
- ↑ Fuchs, C. A. QBism: the Perimeter of Quantum Bayesianism 2010
- ↑ Aerts, D. (1986). A possible explanation for the probabilities of quantum mechanics, Journal of Mathematical Physics, 27, pp. 202-210.
- ↑ Aerts, D. and Sassoli de Bianchi, M. (2014). The extended Bloch representation of quantum mechanics and the hidden-measurement solution to the measurement problem. Annals of Physics 351, Pages 975–1025 (Open Access).
Εσωτερική Αρθρογραφία[]
- Επιστημονικός Νόμος
- Φυσικός Νόμος
- Νόμοι Διατήρησης
- Νόμοι Νεύτωνα
- Unitarity
- Quantum non-equilibrium
- Gleason's theorem
- Transactional interpretation of quantum mechanics
- Hidden-measurements interpretation of quantum mechanics
Βιβλιογραφία[]
Ιστογραφία[]
- Ομώνυμο άρθρο στην Βικιπαίδεια
- Ομώνυμο άρθρο στην Livepedia
- Quantum Mechanics Not in Jeopardy: Physicists Confirm a Decades-Old Key Principle Experimentally ScienceDaily (July 23, 2010)
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αν διαφωνείτε με όσα αναγράφονται σε αυτήν
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