Franck-Condon Factors to High Vibrational Quantum Numbers IV: NO Band Systems

Abstract

Franck-Condon factor arrays have been computed numerically to highest known vibrational quantum numbers for the following NO band systems. $\beta :\left({\text{B}}^2\text{II}-{\text{X}}^2\text{II}\right)\text{Feast}1:\left({\text{D}}^2{\Sigma }^{+}-{\text{A}}^2{\Sigma }^{+}\right)\gamma :\left({\text{A}}^2{\Sigma }^{+}-{\text{X}}^2\text{II}\right)\text{Feast}2:\left({\text{E}}^2{\Sigma }^{+}-{\text{A}}^2{\Sigma }^{+}\right)\delta :\left({\text{C}}^2\text{II}-{\text{X}}^2\text{II}\right)\text{Ogawa}1:\left({\text{B}}^{\text{'}2}\text{Δ}-{\text{B}}^2\text{II}\right)ϵ:\left({\text{D}}^2{\Sigma }^{+}-{\text{X}}^2\text{II}\right)\text{Ogawa}2:\left(b^4{\Sigma }^{+}-a^4\text{II}\right){\beta }^{\text{'}}:\left({\text{B}}^{\text{'}2}\text{Δ}-{\text{X}}^2\text{II}\right)"\text{M}":\left(a^4\text{II}-{\text{X}}^2\text{II}\right){\gamma }^{\text{'}}:\left({\text{E}}^2{\Sigma }^{+}-{\text{X}}^2\text{II}\right)$.