I read a saying as follows:

In a theory with no particles which decay and no bound states, the turning on and off of the interactions merely serves to limit the effective range of forces. In this case, turning the interactions on and off adiabatically will not significantly affect the evolution of any state, so the initial energy and the final energy as determined by the full Hamiltonian $H$ will equal to that determined by the free Hamiltonian $H_0$, so we find that scattering preserves the $H_0$-energy of the states: $$\left[H_0,S \right]=0.$$

I didn't prove this saying, but I think for infinite past the state is asymptotically free, for example $|p_1 p_2\rangle$, and because the full Hamiltonian in the infinte past is equal to free Hamiltonian in adiabatically switching off, in the infinte past the energy of full Hamiltonian is equal to free Hamiltonain $E_1+E_2$. While the whole process must be conservation of energy, the energy of full Hamiltonian is equal to free one, $E_1+E_2$, in any time.

While according to Gell-Mann and Low theorem, the energy of free Hamiltonian $H_0$ is different from the full Hamiltonian $H$:

$$E = E_0 + \langle\Psi_0 | H_\epsilon-H_0 | \Psi_\epsilon\rangle$$

This also seems to be right. Because in adiabatic process, energy crossing will not occur, that is, some energy level $E_n(t_1)$ of $H(t_1)=H_0+H_I(t_1)$ will become corresponding energy level $E_n(t_2)$ of $H(t_2)=H_0+H_I(t_2)$. Therefore the energy will different in different time. But it also seems to be weird, since energy is not conserved in interacting QFT.

How to resolve this feud?


1 Answer 1


In non-relativistic scattering theory much effort has been put into a formulation avoiding adiabatic switching. Thus the existence and completeness of the Moller wave operators is proven allowing a definition of a unitary scattering operator commuting with the free Hamiltonian. But in field-theoretic situations the situation is not that simple. In fact the Hilbert spaces for free and interacting systems are different (Haag's theorem). This may account for the differences you noted. See also: Are the Møller wave operators $\Omega_\pm$ related to $\lim_{t\rightarrow\infty}U(t)$ from field theory?

  • $\begingroup$ It seems that the Haag's theorem was regarded as obsolete? physics.stackexchange.com/q/3983 $\endgroup$
    – user26143
    Commented Apr 28, 2014 at 12:38
  • $\begingroup$ Indeed, there is much discussion about the relevance of Haag's theorem. Secondly, it seems that your statement "the energy of full Hamiltonian is equal to free one, E1+E2, in any time" cannot be derived from the wave operator approach I mentioned. $\endgroup$
    – Urgje
    Commented Apr 28, 2014 at 13:00
  • 1
    $\begingroup$ Thank you for your comment. Just a side note, I am not the author of op, user34669. "the energy of full Hamiltonian is equal to free one, E1+E2, in any time" is not my statement.... $\endgroup$
    – user26143
    Commented Apr 28, 2014 at 13:25
  • $\begingroup$ I'm sorry, point taken. $\endgroup$
    – Urgje
    Commented Apr 28, 2014 at 19:03
  • $\begingroup$ I've corrected the question here, have any comment? Thanks physics.stackexchange.com/q/272854 $\endgroup$
    – 346699
    Commented Apr 1, 2017 at 4:42

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