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PreprintCC BY-NC-SA 4.0arXiv

The chiral filter

Abstract

Thermal neutron capture on a proton, np→ dγ, is measured to a fraction of a percent; the impulse approximation misses nine percent of it. This article follows that gap through five decades of an idea of Mannque Rho's, the chiral filter. Chiral symmetry fixes the pion-exchange current that fills the gap, and power counting explains why nothing else competes. The missing nine percent becomes a prediction, correct within errors. On the unprotected side, one constant fixed by tritium beta decay predicted solar pp fusion and the {\it hep} process; gA* remains open.

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BibTeX
@misc{park2026chiral,
  title = {{The chiral filter}},
  author = {Tae-Sun Park},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.16543},
  eprint = {2609.16543},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.16543},
  note = {CC BY-NC-SA 4.0},
}
RIS
TY  - UNPB
TI  - The chiral filter
AU  - Tae-Sun Park
PY  - 2026
DA  - 2026/09/15
PB  - arXiv
DO  - 10.48550/arxiv.2609.16543
UR  - https://arxiv.org/abs/2609.16543
AB  - Thermal neutron capture on a proton, np→ dγ, is measured to a fraction of a percent; the impulse approximation misses nine percent of it. This article follows that gap through five decades of an idea of Mannque Rho's, the chiral filter. Chiral symmetry fixes the pion-exchange current that fills the gap, and power counting explains why nothing else competes. The missing nine percent becomes a prediction, correct within errors. On the unprotected side, one constant fixed by tritium beta decay predicted solar pp fusion and the {\it hep} process; g_A^* remains open.
ER  -