Minkowski vacuum: Poincare invariant, quasi-free state

paweld
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Minkowski vacuum is Poincare invariant and quasi-free state.
I wonder if these two conditions fully define it or there are more
states which fulfill these conditions (or maybe Poincare
invariance alone is sufficinet). Thanks for answers.
 
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paweld said:
Minkowski vacuum is Poincare invariant and quasi-free state.
I wonder if these two conditions fully define it or there are more
states which fulfill these conditions (or maybe Poincare
invariance alone is sufficient).

I'm not entirely sure what you're asking. In advanced QFT, one attempts to
construct something called an "interacting representation" of the Poincare
group. (See Weinberg vol 1). The vacuum is still defined as the lowest-energy
eigenstate of the (full, interacting) Hamiltonian -- which often does not coincide
with the lowest-energy eigenstate of the free Hamiltonian.
 
My question is whether a state which fulfills two condition:
(1) its two point function is invariant under action of Poincare
group and
(2) all n-point function can be express in terms of two point function by
the sum over all parings (quasi-free state)
has to be Minkowski vacuum.
 
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
If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!

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