phenomenon 105.5 The charged pion is pseudoscalar
open in the book ·
parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:397
· p. 2115
- phenomenon-tested: no experiment declares a \tests edge to it and it is not listed in untested.txt
Rests on
- depends_on equation 105.4 eq:cpt-ylm-parity ¶
- proves proof ch:07-discrete-symmetries-cpt@proof-4 ¶
Supports
-
depends_on
proposition 105.15
Parity of an $n$-pion state
¶
- depends_on proposition 101.24 The parities of the two final states are opposite ¶
- depends_on proposition 107.19 The pion has odd intrinsic parity ¶
- depends_on proposition 101.24 The parities of the two final states are opposite ¶ ↺
Neighborhood
Every logical edge within two steps of this node.
- declared and complete
- partly declared
- a check failed
- not graded
- declared in the source
- inferred from structure
Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
cites |
→ | The Gamma-Ray Spectrum Resulting from Capture of Negative$\pi$-Mesons in Hydrogen and Deuterium | derived | parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:402 |
depends_on |
→ | eq:cpt-ylm-parity | declared | parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:405 |
depends_on |
← | Parity of an $n$-pion state | declared | parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:1016 |
depends_on |
← | The pion has odd intrinsic parity | declared | parts/11-qft-standard-model/09-nuclear-physics.tex:795 |
depends_on |
← | The parities of the two final states are opposite | declared | parts/11-qft-standard-model/03-weak-interactions.tex:1180 |
proves |
← | ch:07-discrete-symmetries-cpt@proof-4 | declared | parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:408 |