Operators with commutator ihbar

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SUMMARY

The commutator of the position and momentum operators, represented as [x, p_{x}] = iħ, is not unique; it also applies to angular position and angular momentum, specifically [θ, L_{θ}] = iħ. According to Dirac, the transition from classical mechanics to quantum mechanics involves substituting Poisson brackets with iħ times the corresponding commutators. This principle indicates that the commutator of any generalized coordinate with its conjugate momentum consistently results in iħ.

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I know that the commutator of the position and momentum operators is ihbar. Can any other combination of two different operators produce this same result, or is it unique to position and momentum only?
 
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Any position and its conjugate momentum have commutator i \hbar.

It's not just linear position and momentum,
[x,p_{x}]=i\hbar,
but angular position and (the proper component of) the angular momentum (the component being the one parallel to the axis of rotation),
[\theta,L_{\theta}]=i\hbar.

Going into a bit more detail:
According to Dirac, one way of getting quantum mechanics from classical mechanics is by substituting the Poisson bracket algebra with i hbar times the corresponding commutator algebra.
[\hat{q_{j}},\hat{p_{j}}] = i \hbar \{q_{j},p_{j}\} = i \hbar.
Assuming this always works, then the commutator of any generalized coordinate with its conjugate momentum will always be i hbar.
 
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Thank you, jfizzix... That is a very helpful answer! Thanks for posting !
 

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