Momentum four vector for ground state.

In summary, the concept of ground state in Quantum Field Theory refers to the state with zero momentum, which is necessary for Poincare symmetry. For massless particles, such as photons, the ground state can have zero energy, but for massive particles, the ground state actually means there is no particle present at all. The potential V(x) does not affect the four momentum of the ground state. For supersymmetric ground states, the momentum four vector would also be zero, as it is the only state that preserves supersymmetry.
  • #1
arroy_0205
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I am confused about the definition of ground state and its characteristics. For a field in spacetime do we mean the ground state to be the minimum of the potential or minimum of the total energy? Specifically what is the momentum four vector of the ground state ([tex] p^{\mu}=(...) [/tex]) for a massive and for a massless field? In my opinion, for massless case, [tex] p^{\mu}=(0,0,0,0) [/tex] and for massive case, [tex] p^{\mu}=(m,0,0,0) [/tex] . Is that correct? How does the potential [tex] V(x) [/tex] enter in the four momentum? In my expression for the four momentum, I have not included the potential in the four momentum.

Finally what is the momentum four vector for a supersymmetric ground state?
 
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  • #2
I think you are confusing the ground state of the theory with the lowest energy state of a given particle. The ground state of a QFT should have zero momentum as this is the only state that does not violate Poincare symmetry; that fixes it to be [tex] p^{\mu}=(E,0,0,0) [/tex]. In the massless case (photons) you can reduce the photon energy towards zero by making its wavelength longer and longer. But that means you still have a one photon in your state.

In the massive case you see that the true ground state of the theory with [tex] p^{\mu}=(0,0,0,0) [/tex] means that there is no electron at all. And this is the ground state of the QFT (not the lowest energy state of one electron, but of no electron). In addition, a state like [tex] p^{\mu}=(m,0,0,0) [/tex] would still carry spin, whereas [tex] p^{\mu}=(0,0,0,0) [/tex] does not. This applies to the photon case as well; a photon with infinite wavelength would still carry spin 1, that means you should consider a state w/o photon as the true ground state.
 

1. What is the momentum four vector for ground state?

The momentum four vector for ground state is a mathematical representation of the momentum and energy of a particle in its lowest energy state, also known as its ground state. It is a four-dimensional vector that includes the particle's momentum in the three spatial dimensions and its energy in the fourth dimension.

2. How is the momentum four vector related to special relativity?

The momentum four vector is a fundamental concept in special relativity, which is a theory that describes the relationship between space and time. It is used to describe the momentum and energy of particles in a way that is consistent with the principles of special relativity, such as the invariance of the speed of light.

3. What is the significance of the ground state in quantum mechanics?

The ground state is the lowest energy state of a particle or system, and it plays a crucial role in quantum mechanics. It is the starting point for analyzing the behavior of particles and systems, and many important concepts, such as the uncertainty principle and the Schrödinger equation, are based on the ground state.

4. How does the momentum four vector for ground state differ from that of excited states?

The momentum four vector for ground state is unique in that it represents the lowest energy state of a particle, while the momentum four vector for excited states represents higher energy states. This means that the values of momentum and energy in the four-dimensional vector will be different for ground state and excited states.

5. What are some applications of the momentum four vector for ground state?

The momentum four vector for ground state has many applications in physics, including in particle physics, quantum field theory, and special relativity. It is used in calculations and equations to describe the behavior of particles and systems, such as in the calculation of scattering amplitudes and decay rates.

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