Trace of the fundamental commutation relation

Click For Summary

Discussion Overview

The discussion centers around the trace of the fundamental commutation relation between the position operator \(x\) and the momentum operator \(p\). Participants explore the implications of the trace operation in the context of unbounded operators in quantum mechanics, comparing it to the trace of finite-dimensional matrices and discussing the validity of certain proofs related to the trace operation.

Discussion Character

  • Technical explanation, Conceptual clarification, Debate/contested

Main Points Raised

  • One participant notes that the trace of the commutator \(\text{Tr}(xp) - \text{Tr}(px) = 0\) seems contradictory since the commutator \([x, p] = i\hbar\) has a non-zero trace.
  • Another participant suggests that the issue arises because \(x\) and \(p\) are unbounded operators on an infinite-dimensional Hilbert space, which affects the validity of certain trace relations known from finite-dimensional matrices.
  • A participant presents a proof of the trace property \(\text{Tr}(AB) = \text{Tr}(BA)\) but questions its applicability to unbounded operators.
  • Another participant responds that while the proof itself is valid, the traces of \(AB\) and \(BA\) are undefined for the operators \(x\) and \(p\), and that the trace's value can depend on the chosen basis.
  • One participant reflects on their interest in commutation relations for spin, noting that the trace of the Pauli matrices is zero and expressing curiosity about whether similar results could be obtained for \(x\) and \(p\).

Areas of Agreement / Disagreement

Participants generally agree that the trace operation behaves differently for unbounded operators compared to bounded operators, but multiple views remain regarding the implications and validity of specific proofs. The discussion does not reach a consensus on the applicability of the trace properties to the operators in question.

Contextual Notes

Limitations include the dependence on the definitions of bounded and unbounded operators, as well as the specific conditions under which the trace is defined or finite. The discussion also highlights the complexity of operator theory in quantum mechanics.

daudaudaudau
Messages
297
Reaction score
0
Hi.

So I have learned that this holds for the trace if A and B are two operators: [itex]\text{Tr}(AB)=\text{Tr}(BA)[/itex]. Now I take the trace of the commutator between [itex]x[/itex] and [itex]p[/itex]: [itex]\text{Tr}(xp)-\text{Tr}(px)=\text{Tr}(xp)-\text{Tr}(xp)=0[/itex]. But the commutator of x and p is [itex]i\hbar[/itex]. Certainly the trace of [itex]i\hbar[/itex] is not zero. What is wrong here?
 
Physics news on Phys.org
The problem is that x and p are unbounded operators on an infinite-dimensional Hilbert space; therefore certain relations known from finite-dimensional matrices do no-longer hold.
 
So what's wrong with this "proof":

[tex]\text{Tr}(AB)=\sum_n \langle n|AB|n\rangle = \sum_n\sum_m\langle n|A|m\rangle\langle m|B|n\rangle=\sum_n\sum_m\langle m|B|n\rangle\langle n|A|m\rangle=\sum_m \langle m|BA|m\rangle=\text{Tr}(BA)[/tex]
 
Nothing is wrong with your proof, only that for the operators A=x and B=p Tr(AB) and Tr(BA) are undefined or the value of the trace depends on the basis chosen. As tom.stoer said, the class of operators for which the trace is finite and independent of the basis chosen is only a small subset of the bounded operators (so called trace class operators) while most operators we are interested in in quantum mechanics are unbounded.
 
Okay I see. I was just considering this question because I was looking at the commutation relations for spin. In that case the trace of the Pauli matrices is actually zero. Just from writing up the commutation relations I obtained a set of equations that I could solve and determine the Pauli matrices... I just wanted to see if a similar thing was possible with x and p.
 

Similar threads

  • · Replies 31 ·
2
Replies
31
Views
3K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 32 ·
2
Replies
32
Views
4K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 38 ·
2
Replies
38
Views
12K
  • · Replies 77 ·
3
Replies
77
Views
9K