Manuscript Em02-D@4 · Em02-D-v4.tex · section · fcf2fac7

Six-row coefficients

Integrated-vertex jets and the known six rows › Six-row coefficients · lines 1432–1455

Em02-D@4#eq:C47, Em02-D@4#eq:C5a, Em02-D@4#eq:Cresp

Define

C_{47} (Φ) C_{5 a} (Φ) C_{resp} (Φ) = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) [\partial_{r^{0}} Q ϕ_{2} (a, s, r)]_{r = s - t}, = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) f (a + s) [\partial_{r^{0}}^{2} Q ϕ_{2} (a, s, r)]_{r = - t}, = - \frac{i κ}{16 π} \int d^{4} a d R (s) f (a + s) Q ϕ_{2} (a, s, 0) .

Displayed formulas in this passage

Em02-D@4#eq:C47 · line 1435
$C_{47} (Φ) C_{5 a} (Φ) C_{resp} (Φ) = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) [\partial_{r^{0}} Q ϕ_{2} (a, s, r)]_{r = s - t}, = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) f (a + s) [\partial_{r^{0}}^{2} Q ϕ_{2} (a, s, r)]_{r = - t}, = - \frac{i κ}{16 π} \int d^{4} a d R (s) f (a + s) Q ϕ_{2} (a, s, 0) .$
Em02-D@4#eq:C5a · line 1435
$C_{47} (Φ) C_{5 a} (Φ) C_{resp} (Φ) = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) [\partial_{r^{0}} Q ϕ_{2} (a, s, r)]_{r = s - t}, = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) f (a + s) [\partial_{r^{0}}^{2} Q ϕ_{2} (a, s, r)]_{r = - t}, = - \frac{i κ}{16 π} \int d^{4} a d R (s) f (a + s) Q ϕ_{2} (a, s, 0) .$
Em02-D@4#eq:Cresp · line 1435
$C_{47} (Φ) C_{5 a} (Φ) C_{resp} (Φ) = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) [\partial_{r^{0}} Q ϕ_{2} (a, s, r)]_{r = s - t}, = \frac{i κ}{16 π} \int d^{4} a d R (s) d R (t) f (a + s) [\partial_{r^{0}}^{2} Q ϕ_{2} (a, s, r)]_{r = - t}, = - \frac{i κ}{16 π} \int d^{4} a d R (s) f (a + s) Q ϕ_{2} (a, s, 0) .$