Weinberg QFT I: Lorentz Transformation with interaction

[SeySchW]

Hi,

a few lines below equation (3.1.5) Weinberg writes:
"The transformation rule (3.1.1) is only possible for particles that for one reason or another are not interacting."

I thought a lot about it, but don't see any possible reason. Can you help please?

After a few lines he defines the states \Phi_{\alpha}
then these one should transform like (3.1.1). But why?

Thanks a lot

 

[Bill_K]

I believe he gives a reason for this in the very next sentence: "Eq (3.1.1) requires among other things that the state has an energy equal to the sum of the one-particle energies with no interaction terms that would involve more than one particle at a time."

 

[SeySchW]

"Eq (3.1.1) requires among other things that the state has an energy equal to the sum of the one-particle energies ... and with no interaction terms, terms that would involve more than one particle at a time."

Thank you for the answer, I'm not quite sure, if I understand this argument. So I will rephrase it. In a theory with no interactions we expect that the energy of a multiparticle state is the sum of the single energies. Whereas in an interacting theory this should be different. But I don't understand why this should be the case?

Thanks

 

[meopemuk]

In a theory with no interactions we expect that the energy of a multiparticle state is the sum of the single energies. Whereas in an interacting theory this should be different. But I don't understand why this should be the case?

But this is the *definition* of interaction! In an interacting theory the Hamiltonian has the form (3.1.8), where H_0 is the sum of single particle energies and V is the interaction potential energy.

Eugene.

 

[SeySchW]

Ok this makes sense. But then \Psi_{\alpha}^{\pm} is not a direct product state of one particle states otherwise it would transform like (3.1.1). How can we then define something like the index \alpha for \Psi_{\alpha}^{\pm}?

Beside: Where can I read more about this? I am completely confused.

Thanks

 

[meopemuk]

SeySchW,

In interacting theory the total boost operator (3.3.20) is different from the non-interacting boost operator K_0. Therefore, boost transformation laws of n-particle states are different from (3.1.1) in the interacting case. For example, a 1-particle state may transform into a n-particle state under interacting boost.

Eugene.

 

[weejee]

Ok this makes sense. But then \Psi_{\alpha}^{\pm} is not a direct product state of one particle states otherwise it would transform like (3.1.1). How can we then define something like the index \alpha for \Psi_{\alpha}^{\pm}?

Beside: Where can I read more about this? I am completely confused.

Thanks

I think you can view (3.1.13) as the definition of in/out states.