A Position is no more an operator in QFT

Heidi
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In quantum mechanics there is no operator for time (problem with unbounded energy).
position is no more an operator in field theory. was there still a problem in QM?
 
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Say there are many particles of same kind, position lose its meaning and number density takes its palce.
 
In general there is no position operator in relativistic quantum theory, at least not within the only kind of relativistic QT that's successful in describing the real world in terms of the Standard Model, which is local relativistic QFT.

However, for all massive particles you can define a position operator having the usual properties. Since only massive particles have a useful non-relativistic limit, there is no contradiction between having a position operator in non-relativistic quantum theory and local relativistic QFT.

The representations of the Galilei group for massless particles doesn't lead to a physically interpretable quantum theory. See also my comment on this here:

https://www.physicsforums.com/threa...r-the-gravitational-field.997062/post-6433476
 
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Is there a position operator in QFT? The question does not make sense until one defines what exactly one means by "position operator". There is operator that satisfies some properties one would expect from a decent position operator, but not all. In particular, the Newton-Wigner position operator does not transform as a Lorentz vector.
 
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I was referring to the usual definition of position operators, as explained in

https://arnold-neumaier.at/physfaq/topics/position.html

It's of course not part of Lorentz four-vector operator, because otherwise time would be an operator too, but that cannot be by construction, because the energy spectrum is bounded from below.
 
Demystifier said:
Is there a position operator in QFT? The question does not make sense until one defines what exactly one means by "position operator". There is operator that satisfies some properties one would expect from a decent position operator, but not all. In particular, the Newton-Wigner position operator does not transform as a Lorentz vector.
Position in relativistic physics is an interesting thing. It happens that the classical position operator IS a Newton-Wigner operator and, also, does-not transform as a 4-vector (can't give a reference, is still in peer review).

Moreover, I think the Newton-Wigner position function (https://arxiv.org/abs/2004.09723) of Hamiltonian mechanics has the same property, though I'm not sure, I haven't read the article in full details.
 
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Not an expert in QM. AFAIK, Schrödinger's equation is quite different from the classical wave equation. The former is an equation for the dynamics of the state of a (quantum?) system, the latter is an equation for the dynamics of a (classical) degree of freedom. As a matter of fact, Schrödinger's equation is first order in time derivatives, while the classical wave equation is second order. But, AFAIK, Schrödinger's equation is a wave equation; only its interpretation makes it non-classical...
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA
Is it possible, and fruitful, to use certain conceptual and technical tools from effective field theory (coarse-graining/integrating-out, power-counting, matching, RG) to think about the relationship between the fundamental (quantum) and the emergent (classical), both to account for the quasi-autonomy of the classical level and to quantify residual quantum corrections? By “emergent,” I mean the following: after integrating out fast/irrelevant quantum degrees of freedom (high-energy modes...

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