Peskin and Schroeder problem 3.5(a): Figuring out the cancellation

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SUMMARY

The discussion centers on resolving a sign discrepancy in Peskin and Schroeder's problem 3.5(a) related to the variation of fields in quantum field theory. The terms in question involve the variations of the fields ##\phi## and ##\chi##, specifically the expressions involving Grassmann numbers. The user initially struggles with the minus sign in the first term but later recognizes that complex conjugation alters the order of Grassmann numbers, which clarifies the issue. This realization confirms that the terms can indeed combine to form a total derivative as expected.

PREREQUISITES
  • Understanding of quantum field theory concepts, particularly variations of fields.
  • Familiarity with Grassmann numbers and their properties.
  • Knowledge of complex conjugation and its effects on mathematical expressions.
  • Experience with Peskin and Schroeder's "An Introduction to Quantum Field Theory" as a reference text.
NEXT STEPS
  • Study the properties of Grassmann numbers in detail.
  • Review the derivation of total derivatives in quantum field theory contexts.
  • Examine complex conjugation rules in the context of quantum fields.
  • Explore additional problems in Peskin and Schroeder to reinforce understanding of field variations.
USEFUL FOR

This discussion is beneficial for graduate students in physics, particularly those studying quantum field theory, as well as researchers looking to deepen their understanding of field variations and Grassmann algebra.

Adgorn
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Homework Statement
Given the Lagrangian:
##L=\partial_\mu \phi \partial \phi^* +\chi^\dagger i \bar{\sigma}^\mu \partial_\mu \chi +F^*F##

Where ##\phi## is a complex vector field, ##\chi## is a free Weyl Fermion and ##F## is an auxiliary complex scalar field, show that the Lagrangian is symmetric under the transformation:

##\delta \phi = -i \epsilon^T \sigma^2 \chi##
##\delta \chi = \epsilon F +\sigma^\mu \partial_\mu \phi \sigma^2 \epsilon^*##
##\delta F = -i \epsilon^\dagger \bar{\sigma}^\mu \partial_\mu \chi##

where ##\epsilon## is a two component spinor of Grassmann numbers.
Relevant Equations
##\chi^T \sigma^2 \epsilon = \epsilon^T \sigma^2 \chi##
##\sigma^2 \sigma^\mu \sigma^2 = (\bar{\sigma}^\mu)^T##
##(\sigma^\mu \cdot \partial) (\bar{\sigma}^\mu \cdot \partial) = \partial^\mu \partial_\mu##
I've managed to account for all the terms except for two, which seem to have a minus sign I cannot get rid of. When expanding the variation, one of them comes from the ##\phi## variation:

$$-i \partial^\mu \phi \epsilon^\dagger \sigma^2 \partial_\mu \chi^* =-i \partial^\mu \phi \partial_\mu \chi^\dagger \sigma^2 \epsilon^*.$$

The other comes from the ##\chi## term and is:

$$i {\sigma}^\mu \bar{\sigma}^\nu \partial_\mu \partial_\nu\phi \chi^\dagger \sigma^2 \epsilon^*=i \partial_\mu \partial^\mu \phi \chi^\dagger \sigma^2 \epsilon^*.$$

If all is right in the world, these two terms should combine to make a total derivative, but they differ by a sign. The online solution manual writes the first term without the minus sign, but I don't see how that can be the case. Is there some rule with Grassmann numbers that I'm not aware of here?
 
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Never mind, I immediately realized upon hitting "post" that complex conjugation switches the order of Grassmann numbers. Better late then never.
 
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Hitting the post button is one of the absolutely best ways of realizing things …
 
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