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PDF Transverse Momentum Dependent Factorization for Radiative

functions is from 0 to ∞ in the heavy quark limit. Actually, from the momentum conservation, it is from 0 to P = mbv kb kq . Under the limit mb → ∞ we have P → ∞. As discussed in [10], if we set P to be ∞ at the beginning, it may resultin some ill-dened distributions.

(PDF) An unfitted finite element method for two-phase Stokes problems...

kq . hk2.


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