Do operators that commute also indicate if their powers commute?

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Discussion Overview

The discussion revolves around the commutation properties of operators, specifically whether the commutation of two operators, ##A## and ##B##, implies that their powers, ##A^m## and ##B^n##, also commute. Participants explore various cases, including positive integers, negative integers, and fractional powers, while considering the implications of these cases on the commutation relations.

Discussion Character

  • Debate/contested
  • Exploratory
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that if ##[A, B] = 0##, then ##AB = BA##, allowing for the interchange of operators under certain conditions.
  • Others express uncertainty regarding the behavior of negative and fractional powers of operators, suggesting that assumptions about convergence may be necessary.
  • A participant raises the question of how operators raised to fractional powers, such as ##A^{\frac{1}{2}}##, behave, citing examples from the Pauli matrices that do not commute.
  • There is a discussion about defining operators with fractional exponents and the potential multi-valued nature of such definitions, particularly in the context of eigenvalues.
  • Some participants suggest that the algebraic structure must be defined to determine the validity of operations involving powers of operators.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether the commutation of operators extends to their powers. Multiple competing views remain regarding the implications of fractional and negative powers, as well as the definitions required for such operations.

Contextual Notes

Limitations include the need for clear definitions of operator powers, especially for non-integer exponents, and the potential for multi-valued functions in the context of certain operators.

TheCanadian
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If ##A## and ##B## are two operators that commute (i.e. [##A##,##B##] = 0), does that indicate if ##A^m## and ## B^n## more generally commute where m and n are not necessarily non-negative integers?
 
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What does it mean, that ##[A,B]=0##?
 
fresh_42 said:
What does it mean, that ##[A,B]=0##?

AB - BA = 0
 
TheCanadian said:
AB - BA = 0
Yep. So ##AB = BA##, i.e. you can pull one or many ##B## through how many ever ##A##'s there are, step by step.
Edit: I don't know how it is for negative exponents since there must first be defined an inverse. There probably have to be made some assumptions on convergence, too.
Edt2: I think I got it. Let ##C = B A^{-1}##, i.e. ##B=CA##. Then ##AB = ACA = BA = CA^2##.
Thus ##ABA^{-1} = CA = B## or ##BA^{-1} = A^{-1}B##.
 
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fresh_42 said:
Yep. So ##AB = BA##, i.e. you can pull one or many ##B## through how many ever ##A##'s there are, step by step.
Edit: I don't know how it is for negative exponents since there must first be defined an inverse. There probably have to be made some assumptions on convergence, too.
Edt2: I think I got it. Let ##C = B A^{-1}##, i.e. ##B=CA##. Then ##AB = ACA = BA = CA^2##.
Thus ##ABA^{-1} = CA = B## or ##BA^{-1} = A^{-1}B##.

Thank you for the reply. That helps a lot. One of the other cases I was wondering about was decimals. Does raising two operators to different fractions alter the operators in such a way they no longer commute?
 
TheCanadian said:
Thank you for the reply. That helps a lot. One of the other cases I was wondering about was decimals. Does raising two operators to different fractions alter the operators in such a way they no longer commute?
Interesting question. At the moment I'm not sure how to define them in a rigorous manner other than, e.g. ##A^3 = B^2## and then apply the tricks above. What would ##A^{e}## be? Probably a convergent Taylor series or something like that in which case crossing to the limits has to be considered.
 
fresh_42 said:
What would ##A^{e}## be?

First, what would ##A^{e}## be when ##A## is a positive real number?
 
George Jones said:
First, what would ##A^{e}## be when ##A## is a positive real number?
The solution of ##e \cdot \ln{A} = \ln{x} ## with all terms defined by their Taylor series.
 
An easy counter-example via the Pauli matrices not commuting and being their own inverse. Not sure if you'll consider it cheating.

Note that:

##[X, Z] = 2iY##

##[X^2, Z^2] = [I, I] = 0##

##I## has many square roots, ##X## and ##Z## among them. We can pick different ones for ##A## and ##B## when setting ##A=B=I##. So ##[A, B] = [I, I] = 0## but ##[A^{\frac{1}{2}}, B^{\frac{1}{2}}] = [X, Z] = 2iY##.

I guess technically ##[A^{\frac{1}{2}}, B^{\frac{1}{2}}]## is not really well defined here. It's a multi-valued function, but some of those values aren't 0.

Your propose rule might hold if we restrict ourselves to the principle powers of a matrix. Require that ##A^x## be interpreted as raising its eigenvalues to ##x##. Further require that ##(e^{i y})^x## only allows the ##e^{i x y} = \cos(x y) + i \sin(x y)## solution. Not so sure in that case.
 
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  • #10
Strilanc said:
An easy counter-example via the Pauli matrices not commuting and being their own inverse. Not sure if you'll consider it cheating.

Note that:

##[X, Z] = 2iY##

##[X^2, Z^2] = [I, I] = 0##

##I## has many square roots, ##X## and ##Z## among them. We can pick different ones for ##A## and ##B## when setting ##A=B=I##. So ##[A, B] = [I, I] = 0## but ##[A^{\frac{1}{2}}, B^{\frac{1}{2}}] = [X, Z] = 2iY##.

I guess technically ##[A^{\frac{1}{2}}, B^{\frac{1}{2}}]## is not really well defined here. It's a multi-valued function, but some of those values aren't 0.

It might still be the case if we restrict ourselves to the principle powers of a matrix. Require that ##A^x## be interpreted as raising its eigenvalues to ##x##. Further require that ##(e^{i y})^x## only allows the ##e^{i x y} = \cos(x y) + i \sin(x y)## solution. Not so sure in that case.
To define ##X = A^{\frac{1}{2}}## is rather edgy, isn't it?
 
  • #11
fresh_42 said:
To define ##X = A^{\frac{1}{2}}## is rather edgy, isn't it?

Well, ##X## is a valid solution to the equation ##M^2 = I##. All 2x2 unitary matrices with eigenvalues of ##\pm1## are. So if you want to be exhaustive then you would say that ##I_2^{\frac{1}{2}}## is the set ##\{M \in U(2) | M^2 = I\}## which includes X and Y and Z and H and I and uncountably many other matrices corresponding to 180 degree rotations around an arbitrary axis in 3-d space (and also their negations).

This problem of multiplicity occurs for matrices besides ##I##. ##X## has four square roots. ##X \otimes X## has sixteen. ##X \otimes I## has uncountably many.

If you want to restrict yourself to a specific matrix or a subset of matrices out of the set of satisfying results, you need to pick a rule for doing that and specify it.
 
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  • #12
Strilanc said:
If you want to restrict yourself to a specific matrix or a subset of matrices out of the set of satisfying results, you need to pick a rule for doing that and specify it.
I think that is the crucial point. One has to define the algebraic structure first in which the operations "live". Thus one can distinguish between what makes sense and what doesn't. (At least this has been the first time I've read about a Pauli matrix being a square root. But why not. As a ##ℂ##-basis of the ring ##ℂ^{2 \times 2}## ...)
 
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