Commutation and Non-Linear Operators

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Discussion Overview

The discussion revolves around the properties of a non-linear operator defined in terms of a linear operator and its implications for commutation relations. Participants explore whether certain commutation relations hold, particularly in the context of quantum mechanics and Heisenberg's uncertainty principle. The scope includes theoretical considerations and mathematical reasoning related to operator algebra.

Discussion Character

  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant defines a non-linear operator ##\langle A \rangle## and questions whether ## \langle A \rangle A = A\langle A \rangle ## and ## \langle A \rangle B = B\langle A \rangle ## hold true.
  • Another participant suggests testing the commutation relations by expanding both sides using the definitions provided.
  • A different participant expresses uncertainty about the associative property in this context and presents calculations that suggest the two expressions may not be equal.
  • Concerns are raised regarding the implications of these results on the validity of the Heisenberg uncertainty principle, particularly questioning the nature of ##\langle A \rangle## in that context.
  • Some participants clarify that in the Heisenberg formula, ##\langle A \rangle## is a scalar, not a non-linear operator, and question the initial assumption that it is a non-linear operator.
  • It is noted that the average of an operator indeed depends on the state on which it acts, and that ##\langle A \rangle## can be treated as a scalar that commutes with linear operators.
  • Clarifications are made regarding the notation and the dependence of ##\langle A \rangle## on the state vector ##\mathbf{x}##, which may lead to confusion in the discussion.

Areas of Agreement / Disagreement

Participants express disagreement regarding the nature of ##\langle A \rangle## and its implications for commutation relations. There is no consensus on whether the proposed commutation relations hold true, and the discussion remains unresolved.

Contextual Notes

Participants highlight limitations in the definitions and assumptions regarding the operators involved, particularly the interpretation of ##\langle A \rangle## and its dependence on the state vector. The discussion also reflects potential confusion arising from standard notation in operator theory.

MisterX
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Suppose ##A## is a linear operator ##V\to V## and ##\mathbf{x} \in V##. We define a non-linear operator ##\langle A \rangle## as $$\langle A \rangle\mathbf{x} := <\mathbf{x}, A\mathbf{x}>\mathbf{x}$$

Can we say ## \langle A \rangle A = A\langle A \rangle ##? What about ## \langle A \rangle B = B\langle A \rangle ## ?

More generally if we have ##Q\mathbf{x} = q(\mathbf{x}) \mathbf{x}## with scalar function ##q##, when does ##AQ=QA ## ? I assert we can choose ##A, Q## such that this is false.
 
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MisterX said:
Can we say ## \langle A \rangle A = A\langle A \rangle ##? What about ## \langle A \rangle B = B\langle A \rangle ## ?
The way to test this is to expand ##(\langle A\rangle B)\mathbf x = \langle A \rangle (Bx)## and ##(B\langle A\rangle)\mathbf x = B( \langle A \rangle x)## using your definitions above to see whether they give exactly the same result.
 
I guess I am not sure about the use of the associative property here. But ignoring this it seems
## \langle A \rangle (B\mathbf {x}) = <B\mathbf {x}, AB\mathbf {x}>B\mathbf {x} ## and ##B( \langle A \rangle \mathbf {x})= <\mathbf {x}, A \mathbf {x}>B\mathbf {x}\neq \langle A \rangle (B\mathbf {x}) ##.

This is troubling to me because this step seems to be used in the proof of Heisenberg's uncertainty principle. Sources claim $$[A-\langle A \rangle, \, B- \langle B \rangle ] = [A,\,B] $$
I guess now am not sure if this is true and why.
 
That's because in that Heisenberg formula ##\langle A\rangle## is a scalar, not a nonlinear operator. The only similarity with this problem is the use of angle bracket symbols, but you have used them to mean something completely different from what Heisenberg means by them.

Where did you get the notion that ##\langle A\rangle## is a nonlinear operator?
 
andrewkirk said:
That's because in that Heisenberg formula ##\langle A\rangle## is a scalar, not a nonlinear operator. The only similarity with this problem is the use of angle bracket symbols, but you have used them to mean something completely different from what Heisenberg means by them.

Where did you get the notion that ##\langle A\rangle## is a nonlinear operator?
Are you asserting that ##\langle A\rangle## is not 2nd order in ##\mathbf{x}##? Doesn't the average of an operator depend on the state on which it acts?
 
MisterX said:
Doesn't the average of an operator depend on the state on which it acts?
That's right. To be precise, ##\langle A \rangle## denotes the scalar value ##\langle \mathbf x\ |\ A\ |\ \mathbf x\rangle## where ##\mathbf x## is the current state.

But ##\langle A \rangle## denotes the scalar result, not an operator. It is only an operator in the sense that scalar multiplication is a linear operation. If that is the meaning in your OP then the answers are, treating ##\langle A \rangle## as the linear operator that pre-multiplies any vector ##\mathbf y## by the scalar ##\langle A \rangle## (which is ##\langle \mathbf x\ |\ A \ |\ \mathbf x\rangle##), that both of the following are true:
  • ##\langle A\rangle A= A\langle A\rangle##
  • ##\langle A\rangle B= B\langle A\rangle##
since scalar multiplication commutes with any linear operator.

But we need to note that ##\langle A\rangle A \mathbf y## is
##\langle \mathbf x\ |\ A \ |\ \mathbf x\rangle A\mathbf y##
not
##\langle \mathbf y\ |\ A \ |\ \mathbf y\rangle A\mathbf y##

It has to be admitted, the standard notation is a little confusing because ##\langle A \rangle## depends on ##\mathbf x## even though that does not appear anywhere in the notation.
 
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