Are Observables Only Quantities That Commute with Hamiltonian?

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Discussion Overview

The discussion revolves around the nature of observables in quantum mechanics, specifically whether observables are limited to quantities that commute with the Hamiltonian of a system. Participants explore definitions and implications of observables, including the role of position and the relationship between observables and measurement.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants argue that observables are not limited to quantities that commute with the Hamiltonian, as commuting indicates simultaneous measurability and conservation under certain conditions.
  • Position is presented as an observable, with references to the Heisenberg Uncertainty Principle highlighting the trade-off between knowledge of position and momentum.
  • There is a claim that any Hermitian operator corresponds to an observable, with the observable being the eigenvalues of that operator, although not all operators yield interesting observables.
  • Some participants assert that position could be considered the only observable, though this view is challenged as being overly simplistic and tied to outdated notions of measurement.
  • One participant discusses the definition of position observables in both non-relativistic and relativistic contexts, noting that for massless particles of higher spin, a position observable may not exist.
  • There is a contention regarding the nature of observations, with some arguing that all observations ultimately relate back to position, while others emphasize that the process of observation involves more than just positional data.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the definition and nature of observables, particularly concerning the role of position and the implications of commuting operators. The discussion remains unresolved with no clear consensus on these points.

Contextual Notes

Participants note that the definitions and implications of observables may depend on the specific physical system being considered, as well as the interpretations of quantum mechanics being applied.

audioloop
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are observables only those quantities which commute with system's Hamiltonian ?
 
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No. If it commutes with the Hamiltonian it simply means you can measure both it and energy simultaneously. It also means it probably will be conserved if the Hamiltonian has no specific time dependence - actually there is no probably about it - it will be conserved.

Thanks
Bill
 
Last edited:
As to your original question, position is an observable. Obviously from Heisenberg's Uncertainty Principle, the uncertainty in the momentum would then be infinite, so you have the classic statement of how if you know where a particle is, you have no idea where it's going or how fast. The converse statement is also true, you can know its momentum but consequently have no idea where it is.
 
As far as I know, in principle ANY Hermitian operator is associated with an observable, which are simply the eigenvalues of that operator. For the vast majority of such operators, the observable is not very interesting. For example, the Hamiltonian operator is associated with the observable "Energy". If the operators associated with two observables commute, then your system can be in a state where both observables can be simultaneously well defined.

Remember: just because a quantity is called an observable in QM doesn't mean we know how to build a machine to measure it, or that we even care about it.
 
also, it can (and I've seen it done) be argued that position is the only observable.
 
jfy4 said:
also, it can (and I've seen it done) be argued that position is the only observable.

Yes I have seen it argued as well - but its based on the silly idea the outcome of any observation is the position of a pointer or something like that. People like that are stuck in a time warp IMHO and are not in the computer age. Observations can be captured digitally not having anything to do with position at all.

Thanks
Bill
 
It depends on how you define "position" and which system to look at whether there is such a thing as a position observable.

In non-relativistic physics for (necessarily massive) particles of any spin, there always exists a position observable defined via the representation theory of the Poincare group, which gives you the 10 conserved quantities and their commutation relations (energy, momentum, angular momentum, center-of-momentum coordinates). Then you can define the position variable as that not explicitly time dependent observable which together with the momentum coordinates fulfills the Heisenberg algebra
[tex][\hat{x}_j,\hat{p}_k]=\mathrm{i} \hbar \delta_{jk}.[/tex]
In relativistic physics also for all massive particles there exists a position observable of this kind, for massless particles that's the case only for particles with spin 0 and spin 1/2. For all massless particles of higher spin, especially also for photons, there is no position observable in the strict sense. For details, see Arnold Neumaier's Theoretical Physics FAQ:

http://arnold-neumaier.at/physfaq/topics/position.html
 
Last edited:
bhobba said:
Yes I have seen it argued as well - but its based on the silly idea the outcome of any observation is the position of a pointer or something like that. People like that are stuck in a time warp IMHO and are not in the computer age. Observations can be captured digitally not having anything to do with position at all.
The issue is this: position is the primary way humans interact with the world. We see where objects are, we hear them, etc. Even if the information is stored digitally, we still have to acquire that information somehow, in a digital display for instance, and that involves sight. So the argument is that we only directly deal with position, and everything else we conclude about the world comes indirectly, from interpretation of the positional data of the senses.
 
  • #10
lugita15 said:
The issue is this: position is the primary way humans interact with the world. We see where objects are, we hear them, etc. Even if the information is stored digitally, we still have to acquire that information somehow, in a digital display for instance, and that involves sight. So the argument is that we only directly deal with position, and everything else we conclude about the world comes indirectly, from interpretation of the positional data of the senses.

Sight is not position but reception of the electromagnetic field. Position is reconstructed from what we see by a nontrivial process.
 
  • #11
A. Neumaier said:
Sight is not position but reception of the electromagnetic field. Position is reconstructed from what we see by a nontrivial process.

Exactly - scratching my head why anyone would think otherwise.

And reading information on a computer screen has nothing to do with the position of the screen or the position of whatever you use to present the information.

Thanks
Bill
 

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