Physics:Quantum Commutator: Difference between revisions

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{{Short description|Operator expression measuring non-commutativity}}
{{Short description|Operator expression measuring non-commutativity}}
{{Quantum book/methods backlink|Foundations}}
{{Quantum book backlink|Foundations}}
{{Quantum article nav|previous=Physics:Quantum Matrix mechanics|previous label=Matrix mechanics|next=Physics:Quantum Measurement problem|next label=Measurement problem}}
 
[[File:Quantum_Commutator_educational_yellow.png|thumb|right|A commutator compares doing two quantum operations in different orders.]]


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
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
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The canonical position and momentum commutator is
The canonical position and momentum commutator is


<math>[x,p] = i\hbar.</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]] and is one of the basic structures of [[Physics:Quantum Matrix mechanics|matrix mechanics]].

Revision as of 09:57, 23 May 2026

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A commutator compares doing two quantum operations in different orders.

In quantum mechanics, a commutator measures how much two operators fail to commute. For two operators A and B, the commutator is

[A,B]=ABBA.

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]=iI.

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

References


Author: Harold Foppele