98 Commutators
An operator built from a product difference that is used to measure whether two operators can be applied in either order without change.
The definition of the commutator. The commutator of two operators is \(AB-BA\). This principle is used to test whether the product order matters.
The commutator is
\[ [A,B] = AB - BA \]
where
- \(A\) and \(B\) are operators.
- \([A,B]\) is their commutator.
The canonical relation \([X,P]=i\hbar\). Position and momentum do not commute. This principle is used to write the canonical commutation relation and to derive the uncertainty principle.
The position-momentum commutator is
\[ [X,P] = i\hbar \]
where
- \(X\) is the position operator.
- \(P\) is the momentum operator.
- \(\hbar\) is the reduced Planck constant.
Conservation when \([A,H]=0\). If \([A,H]=0\), then \(A\) is conserved. This principle is used to identify constants of the motion.
Simultaneous eigenbases. If \([A,B]=0\), the operators share a common eigenbasis. This principle is used to measure \(A\) and \(B\) together.
Note: Also called a commutation relation when set equal to a specific value. Also denoted \([A,B]\).
98.1 References
- Hall, B. C. Quantum Theory for Mathematicians. Springer, 2013. — \([A,B]=AB-BA\); \([X,P]=i\hbar\).
- Sakurai, J. J., & Napolitano, J. Modern Quantum Mechanics. Cambridge University Press, 2021. — \([A,B]=AB-BA\); \([x,p_{x}]=i\hbar\).
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