A theory describing the effects of a DC magnetic field on a 3 ⌺ ϩ Ϫ 1 ⌸ complex includes the influence on the energy positions of the 3 ⌺ ϩ rovibrational levels, the change of their lifetimes as well as the strength of the 3 ⌺ ϩ ← 1 ⌺ ϩ intercombination transitions. This is measured on the aЈ 3 ⌺ ϩ (vϭ14)←X 1 ⌺ ϩ (vϭ0) transition in CO where strong zero field mixing of the aЈ 3 ⌺ ϩ (v ϭ14) state with the A 1 ⌸(vϭ4) state occurs through spin-orbit coupling. aЈ←X excitation spectra are taken under fields of up to 1 Tesla. Lifetimes of various aЈ(vϭ14),N,F i rotational levels are measured as a function of a magnetic field, where changes as large as 30% reveal a strong influence of the field on the mixing with the A 1 ⌸(vϭ4) state. A change in the singlet character of the aЈ 3 ⌺ ϩ (vϭ14),N,F i rovibrational levels alters the line intensities of their forbidden aЈ←X transition which arises due to intensity borrowing from the allowed A←X transition. From the measured lifetime values at 1 Tesla the changes in line intensities as well as absolute oscillator strengths for several aЈ(vϭ14)←X(vϭ0) rotational lines are derived. An increase in population transfer from X 1 ⌺ ϩ (vϭ0),J to aЈ 3 ⌺ ϩ (vϭ14),N,F i of up to 51% is deduced. Finally, the energy levels and the lifetimes of the aЈ(vϭ14),N,F i rotational levels in the high field regime beyond 4 Tesla are discussed.