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The Lippman-Schwinger equation for two-nucleon scattering

We wrote the Lippman-Schwinger equation as ϕm|ˆT|ϕn=ϕm|ˆV|ϕn+kϕm|ˆV|ϕk1(Enωk)ϕk|ˆT|ϕn. How do we rewrite it in a partial wave expansion with momenta k?