A question about symmetry in the phi^4 theory

In summary, the symmetry ##\phi\rightarrow-\phi## ensures that the amplitude can be written as ##\alpha + \beta p^2 + \gamma p^4 + ...## without the odd terms in ##p## and that any diagram in ##\phi^4## must have an even number of external legs.
  • #1
gobbles
17
1

Homework Statement


Why does the symmetry ##\phi\rightarrow-\phi## mean that an amplitude can be written as
##\alpha + \beta p^2 + \gamma p^4 + ...##
without the odd terms in ##p##?

Homework Equations


I understand that, due to this symmetry, any diagram in ##\phi^4## has an even number of external legs, because otherwise the correlation function of the external fields is zero. So any diagram can be written in the form
##V(p^2)\left(\frac{i}{p^2-m^2}\right)^{n}##
where ##n## is even and ##V(p^2)## is the expression for the amplitude without the external legs. Expanding ##V(p^2)## in ##p## will, of course, give only even powers of ##p##, as will the expansion of ##\left(\frac{i}{p^2-m^2}\right)^n##, but that is true also for ##n## odd, corresponding to an odd number of external legs. So where does this symmetry play a role here?

The Attempt at a Solution


Outlined in (2).
 
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  • #2


Hello,

The symmetry ##\phi\rightarrow-\phi## plays a crucial role in the form of the amplitude ##V(p^2)##. This is because the symmetry implies that the amplitude must be an even function of ##\phi##. This means that the terms in the amplitude must be of the form ##\alpha + \beta p^2 + \gamma p^4 + ...##, where ##\alpha, \beta, \gamma, ...## are constants. If the amplitude had odd terms in ##p##, then the symmetry would be broken, as the odd terms would change sign under the transformation ##\phi\rightarrow-\phi##. Therefore, the symmetry ensures that the amplitude can only have even powers of ##p##, resulting in the form ##V(p^2)## without the odd terms in ##p##.

Additionally, as you mentioned, the symmetry also plays a role in the number of external legs in a diagram. Since the correlation function of the external fields is zero for an odd number of external legs, the symmetry ensures that any diagram in ##\phi^4## must have an even number of external legs. This is because the symmetry would be broken if there were an odd number of external legs, resulting in a non-zero correlation function.

I hope this helps clarify the role of the symmetry in the form of the amplitude and the number of external legs in a diagram. Let me know if you have any further questions.
 

What is the phi^4 theory and why is symmetry important in it?

The phi^4 theory is a mathematical model used in particle physics to describe the behavior of elementary particles. It involves a scalar field called phi and its interactions with itself. Symmetry is important in this theory because it helps to simplify calculations and make predictions about the behavior of particles.

What is symmetry breaking in the context of the phi^4 theory?

Symmetry breaking occurs when the symmetry of a system is lost due to certain conditions or interactions. In the context of the phi^4 theory, symmetry breaking can occur when the scalar field phi takes on a non-zero value, breaking the symmetry of the system.

What is spontaneous symmetry breaking and how is it related to the phi^4 theory?

Spontaneous symmetry breaking is a phenomenon in which a system exhibits symmetry at a fundamental level, but not at an observable level. In the phi^4 theory, spontaneous symmetry breaking can occur when the potential energy of the system is minimized at a non-zero value of phi, resulting in a broken symmetry.

What is the significance of Goldstone bosons in the phi^4 theory?

Goldstone bosons are particles that arise as a result of spontaneous symmetry breaking in the phi^4 theory. They are known as "massless" particles because they have no mass and are associated with the broken symmetry of the system. Goldstone bosons play an important role in predicting the behavior of particles in the phi^4 theory.

What are some practical applications of the phi^4 theory and its understanding of symmetry?

The phi^4 theory has many practical applications in particle physics, such as in the study of phase transitions and the behavior of quarks and gluons in quantum chromodynamics. Understanding symmetry in this theory also has implications for other areas of physics, such as condensed matter physics and cosmology.

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