Renormalization Conditions
Quantum Field Theory · Part 6
213 KB10 sections4 key equationsLaTeX typeset
Table of Contents
- 1.4.1 The Ambiguity of Finite Parts
- 2.4.2 On-Shell Renormalization Scheme
- 3.4.3 On-Shell Scheme in QED
- 4.4.4 MS-bar Scheme
- 5.4.5 Running Parameters
- 6.4.6 Momentum Subtraction Schemes
- 7.4.7 Scheme Dependence and Independence
- 8.4.8 Comparison of Schemes
- 9.(a) Mass Renormalization Condition
- 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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