Pith. sign in

(C27) In momentum space the propagator leads to the integral ~I5(k;m) = ∫ d4p (2π)4 ∫ d4q (2π)4 (2π)4δ4(p +q −k) [ −p ·q +m2] × [ p2 −m2 +iǫ ] −1[ q2 −m2 +iǫ ] −1

Pseudoscalar Diquarks The spectral representation of the Diquark Feynman propagato r is i(∆F )5,ab(x′ −x) = (0 |T [ χa 5(x′)χb† 5 (x) ] |0) = i ∫ ∞ s0 ds (∆F )ab(x′ −x), s) ρ(s)

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
browse 1 citing papers

citation-role summary

method 1

citation-polarity summary

use method 1

fields

nucl-th 1

years

2025 1

verdicts

CONDITIONAL 1

roles

method 1

polarities

use method 1

representative citing papers

Nucleon-Quark Diquark-exchange Interaction

nucl-th · 2025-06-27 · conditional · novelty 4.0

A QFT calculation yields an effective axial-vector diquark propagator with a sign opposite to meson exchange, giving a repulsive nucleon-quark potential.

citing papers explorer

Showing 1 of 1 citing paper.

  • Nucleon-Quark Diquark-exchange Interaction nucl-th · 2025-06-27 · conditional · none · ref 2

    A QFT calculation yields an effective axial-vector diquark propagator with a sign opposite to meson exchange, giving a repulsive nucleon-quark potential.