Renormalization Conditions

Quantum Field Theory · Part 6

213 KB10 sections4 key equationsLaTeX typeset

Table of Contents

  1. 1.4.1 The Ambiguity of Finite Parts
  2. 2.4.2 On-Shell Renormalization Scheme
  3. 3.4.3 On-Shell Scheme in QED
  4. 4.4.4 MS-bar Scheme
  5. 5.4.5 Running Parameters
  6. 6.4.6 Momentum Subtraction Schemes
  7. 7.4.7 Scheme Dependence and Independence
  8. 8.4.8 Comparison of Schemes
  9. 9.(a) Mass Renormalization Condition
  10. 10.(b) Field Renormalization Condition

Key Equations

$$\delta m^2 = \frac{C}{\epsilon} + (\text{finite part})$$
$$\left.\frac{d\Sigma(p^2)}{dp^2}\right|_{p^2=m^2} = 0$$
$$\Sigma(\not{p} = m_e) = 0$$
$$\delta X = -\frac{C_X}{\epsilon} - C_X(\ln 4\pi - \gamma_E) + 0$$

Equations are rendered with MathJax in the PDF with professional LaTeX typesetting.

Course Context

This PDF is part of the Quantum Field Theory course on CoursesHub.World. A comprehensive graduate-level course in quantum field theory. Covers classical field theory, canonical quantization, path integrals, gauge theories, renormalization, the Standard Model, and advanced ...

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