Abstract
It is shown that a field is a free field as soon as the states generated by the Heisenberg field and the incoming field operators operating on the vacuum coincide [statement (i)]. Several conclusions are drawn from statement (i) concerning the strong convergence of the field for t tending to infinity [statement (ii)], the uselessness of the local clothed particle representation [statement (iii)], and the diagonalization of the Hamiltonian [statement (iv)], as well as the time behavior of the mathematical vacuum [statement (v)].
Full Text 
Sign-in/Register to access full text options
Sign-in/Register to access full text options 
Published version (
Free)
Free) 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a call
