Physics:Quantum Commutator: Difference between revisions

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In quantum mechanics, a '''commutator''' measures how much two operators fail to commute. For two operators <math>A</math> and <math>B</math>, the commutator is
'''Commutator''' is a Book I topic in the Quantum Collection. In quantum mechanics, a '''commutator''' measures how much two operators fail to commute. For two operators <math>A</math> and <math>B</math>, the commutator is<ref>{{Cite book |last=Griffiths |first=David J. |title=Introduction to Quantum Mechanics |edition=2nd |publisher=Prentice Hall |year=2004 |isbn=0-13-805326-X}}</ref>


<math>[A,B] = AB - BA.</math>
<math>[A,B] = AB - BA.</math> Commutators are important because they encode the non-classical algebra of observables. When two operators do not commute, the order of operations matters and the corresponding measurements generally cannot both have sharp values. This structure underlies uncertainty relations, angular momentum algebra, symmetry generators, time evolution, and the operator language used throughout quantum mechanics.
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<math>[x,p] = i\hbar I.</math>
<math>[x,p] = i\hbar I.</math>


This relation underlies the [[Physics:Quantum Uncertainty principle|uncertainty principle]] and is one of the basic structures of [[Physics:Quantum Matrix mechanics|matrix mechanics]].
This relation underlies the [[Physics:Quantum Uncertainty principle|uncertainty principle]]<ref>{{Cite book |last=Liboff |first=Richard L. |title=Introductory Quantum Mechanics |edition=4th |publisher=Addison-Wesley |year=2003 |isbn=0-8053-8714-5}}</ref> and is one of the basic structures of [[Physics:Quantum Matrix mechanics|matrix mechanics]].


== See also ==
== See also ==
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== References ==
== References ==
{{reflist|3}}
{{reflist|3}}
* {{Cite book |last=Griffiths |first=David J. |title=Introduction to Quantum Mechanics |edition=2nd |publisher=Prentice Hall |year=2004 |isbn=0-13-805326-X}}
* {{Cite book |last=Liboff |first=Richard L. |title=Introductory Quantum Mechanics |edition=4th |publisher=Addison-Wesley |year=2003 |isbn=0-8053-8714-5}}
* {{Cite book |last=McMahon |first=David |title=Quantum Field Theory |publisher=McGraw Hill |year=2008 |isbn=978-0-07-154382-8}}


{{Author|Harold Foppele}}
{{Author|Harold Foppele}}

Latest revision as of 22:58, 23 May 2026

← Back to Foundations Book I
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Next : Measurement problem →

Commutator is a Book I topic in the Quantum Collection. In quantum mechanics, a commutator measures how much two operators fail to commute. For two operators A and B, the commutator is[1]

[A,B]=AB−BA. Commutators are important because they encode the non-classical algebra of observables. When two operators do not commute, the order of operations matters and the corresponding measurements generally cannot both have sharp values. This structure underlies uncertainty relations, angular momentum algebra, symmetry generators, time evolution, and the operator language used throughout quantum mechanics.

A commutator compares doing two quantum operations in different orders.

Role in quantum mechanics

Commutators are central because quantum observables are represented by operators. If two observables have a nonzero commutator, the corresponding quantities generally cannot both have sharply defined values in the same state.

The canonical position and momentum commutator is

[x,p]=iℏI.

This relation underlies the uncertainty principle[2] and is one of the basic structures of matrix mechanics.

See also

Table of contents (217 articles)

Index

Full contents

References

  1. ↑ Griffiths, David J. (2004). Introduction to Quantum Mechanics (2nd ed.). Prentice Hall. ISBN 0-13-805326-X. 
  2. ↑ Liboff, Richard L. (2003). Introductory Quantum Mechanics (4th ed.). Addison-Wesley. ISBN 0-8053-8714-5. 


Author: Harold Foppele


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