feynlag.vertices.bilinear¶
The fermion bilinear track.
Fermions never enter the commuting Poly extractor. A Yukawa or gauge-current term is written as:
coefficient(bosons, params) × Bilinear(ψ̄_a[i], Γ, χ_b[j])
where Γ is a Dirac structure built from feynlag.dirac objects
(diracPL, diracPR, DiracGamma(mu)*diracPL …) and [i], [j]
are flavor indices on IndexedBase components. The bilinear is an opaque
commuting atom (a spinor sandwich is a c-number).
A single bilinear per term is the FFS/FFV (Yukawa / gauge-current) track.
Two bilinears per term is the four-fermion (FFFF) track for dim-6 effective
operators like Fermi theory (ψ̄Γψ)(χ̄Γ′χ) — supported in the as-written
bilinear basis (no Fierz canonicalisation; a Fierz-rearranged operator is a
different input) and restricted to four distinct fermion components. When
a fermion component repeats among the four legs (e.g. (ēΓe)(ēΓ′e) or a
squared bilinear B²), extraction raises NotImplementedError: the
repeated leg generates cross-chain Wick contractions whose relative signs need
genuine spinor-index Fierz algebra the opaque-Bilinear design cannot
express. With distinct legs there are no exchange contractions, so the vertex
is simply i × coefficient × ∏(boson multiplicity)! with the two Dirac
structures (Γ, Γ′) carried alongside (four_fermion_feynman_rule()).
extract_fermion_vertices() groups terms by bilinear and peels the boson
legs off each coefficient with the bosonic extractor — this systematizes the
DLRSM1 IndexedBase coupling pattern.
Functions
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Distribute |
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Group a fermionic Lagrangian by bilinear(s) and extract boson legs. |
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Group a Majorana sector by |
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FFS/FFV rule: |
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Gauge-current terms of |
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Fermion mass matrix from the vacuum-evaluated fermionic sector. |
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FFFF rule: the scalar |
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Majorana FFS/FFSS rule: |
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Symmetric Majorana mass matrix from the vacuum-evaluated sector. |
Classes
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