Can the 'mass' of bound states show up full propagator?

In summary, the Kallen-Lehmann spectral representation shows that the two point correlation and full propagator have a pole at the physical mass of the particle. According to Peskin and Schroeder, multiparticle states appear as a cut but bound states can also appear as poles. If we calculate the full propagator and find a pole for a certain momentum, we can conclude that it is the mass of the particle. However, there may not be a difference between the mass of the particle and the 'mass' of a bound state. This can be seen in an example of a proton moving in an electron gas where the interacting proton's ground state becomes the bound state of a hydrogen atom. Ultimately, for a single particle, the pole represents
  • #1
center o bass
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2
The result of the Kallen-Lehmann spectral representation is that the two point correlation (and thus also the full propagator) has a pole in the physical mass of the particle. In Peskin and Schroeder it is also argued that multiparticle states show up as a cut, but bound states can also show up as poles.

Let's then say that we calculate the full propagator to a certain order and we find that we have a pole for a certain mometum - how do we then conclude that this pole is actually the mass of the particle and not the 'mass' of the bound state?
 
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  • #2
center o bass said:
Let's then say that we calculate the full propagator to a certain order and we find that we have a pole for a certain mometum - how do we then conclude that this pole is actually the mass of the particle and not the 'mass' of the bound state?

The mass of the particle is what you start with in the Lagrangian. If a bound state appears then it'll look like something else.
 
  • #3
center o bass said:
How do we then conclude that this pole is actually the mass of the particle and not the 'mass' of the bound state?

I don't think there is a difference. You could for example consider a proton moving in an electron gas with chemical potential mu. When interaction is switched on, the ground state of the interacting proton will evolve into the ground state of a bound hydrogen atom.
 
  • #4
for a multiparticle state it is a bound state,for a single particle it is the physical mass.
 

1. What is a "bound state" in physics?

A bound state in physics refers to a state in which a particle or system of particles is confined within a potential energy well and is unable to escape. This can occur in systems such as atoms, molecules, and nuclei, where the particles are held together by attractive forces.

2. What is a propagator?

A propagator is a mathematical function used in quantum field theory to describe the probability amplitude for a particle to propagate from one point in spacetime to another. It takes into account the interactions between particles and their corresponding fields.

3. How is the mass of bound states related to their propagator?

The mass of a bound state is directly related to its propagator. The propagator for a bound state includes a term known as the "pole," which corresponds to the mass of the bound state. Therefore, the mass of the bound state is a key factor in determining its propagator.

4. Can the mass of bound states show up in the full propagator?

Yes, the mass of bound states can show up in the full propagator. As mentioned earlier, the mass of a bound state is directly related to its propagator, and therefore it is a crucial component of the full propagator.

5. Why is it important to understand the relationship between mass and propagator in bound states?

Understanding the relationship between mass and propagator in bound states is important in order to accurately describe and predict the behavior of particles and systems in quantum field theory. This knowledge can help to improve our understanding of fundamental particles and their interactions, and can also have practical applications in fields such as particle physics and cosmology.

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