theorem 108.64 Appelquist–Carazzone
open in the book ·
parts/11-qft-standard-model/10-renormalization-group.tex:2353
· p. 2281
Rests on
- depends_on definition 108.17 Four schemes ¶
- depends_on equation 100.82 eq:qed-alpha-effective ¶
-
depends_on
proposition 100.33
Uehling's modification of the Coulomb potential
¶
- depends_on equation 100.50 eq:qed-pi2 ¶
-
depends_on
theorem 100.25
One-photon exchange is the Coulomb potential
¶
- depends_on equation 100.14 eq:qed-fourier ¶
- depends_on equation 100.17 eq:qed-photon-propagator ¶
-
depends_on
proposition 100.14
The Feynman rules of QED in SI form
¶
- depends_on equation 100.2 eq:qed-action ¶
-
depends_on
proposition 100.8
The photon propagator
¶
- depends_on equation 100.2 eq:qed-action ¶ ↺
- depends_on equation 100.16 eq:qed-gauge-fixing-term ¶
- depends_on equation 100.15 eq:qed-photon-kernel ¶
- proves proof ch:02-qed-renormalization@proof-4 ¶
-
depends_on
theorem 100.5
The gauge principle
¶
- depends_on equation 100.6 eq:qed-current ¶
- depends_on equation 100.5 eq:qed-free-dirac ¶
- proves proof ch:02-qed-renormalization@proof-1 ¶
- proves proof ch:02-qed-renormalization@proof-7 ¶
- proves proof ch:02-qed-renormalization@proof-14 ¶
- proves proof ch:02-qed-renormalization@proof-21 ¶
- proves proof ch:10-renormalization-group@proof-28 ¶
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Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
cites |
→ | Infrared singularities and massive fields | derived | parts/11-qft-standard-model/10-renormalization-group.tex:2360 |
depends_on |
→ | Four schemes | declared | parts/11-qft-standard-model/10-renormalization-group.tex:2361 |
depends_on |
→ | eq:qed-alpha-effective | declared | parts/11-qft-standard-model/10-renormalization-group.tex:2361 |
depends_on |
→ | Uehling's modification of the Coulomb potential | declared | parts/11-qft-standard-model/10-renormalization-group.tex:2361 |
proves |
← | ch:10-renormalization-group@proof-28 | declared | parts/11-qft-standard-model/10-renormalization-group.tex:2364 |