]>The Phenomenology of Iron Pnictides Superconductors Explained in the Framework of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>s</mml:mi></mml:math>-Wave Three-Band Eliashberg Theory : Table 1
Table 1: The effect of the intraband terms and Coulomb interaction on the gap values.
Pure interband 𝜆 𝑖 𝑖 = 0 . 𝜇 ∗ 𝑖 𝑗 = 0 Ω 0 = 1 0  meV
Free parameters 𝜆 3 1 = 4 . 2 6 7 𝜆 3 2 = 1 . 1 3 8 —
Results Δ 1 = 1 0 . 2 9  meV Δ 2 = 5 . 5 6  meV | Δ 3 | = 1 0 . 2 2  meV
Intraband 𝜆 𝑖 𝑖 = 0 . 4 𝜇 ∗ 𝑖 𝑗 = 0 Ω 0 = 1 0  meV
Free parameters 𝜆 3 1 = 3 . 8 6 6 𝜆 3 2 = 0 . 4 7 1 —
Results Δ 1 = 1 0 . 3 0  meV Δ 2 = 5 . 6 2  meV | Δ 3 | = 1 0 . 2 4  meV
Intraband and Coulomb 𝜆 𝑖 𝑖 = 0 . 4 𝜇 ∗ 𝑖 𝑗 = 0 . 1 Ω 0 = 1 0  meV
Free parameters 𝜆 3 1 = 2 . 7 3 0 𝜆 3 2 = 0 . 7 5 8 —
Results Δ 1 = 7 . 4 9  meV Δ 2 = 5 . 7 2  meV | Δ 3 | = 7 . 9 8  meV