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Hadronic production of a Higgs boson in association with two jets at ...

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eplacemenB.2. Box Integral Functions 179tM 2 2F 1m3 F 2m3F 3m3M 2 3ssM 2 1Figure B.2: Conventions for labell<strong>in</strong>g the three scalar triangle <strong>in</strong>tegrals appear<strong>in</strong>g<strong>in</strong> the one-loop H plus parton amplitudes.(B.2.17)where,∆ =3∑−Mk 4 + 2M2 k M2 k+1k=1(B.2.18)δ k = M2 k − M2 k+1 − M2 k+2√ . (B.2.19)∆Altern<strong>at</strong>ive represent<strong>at</strong>ions for these <strong>in</strong>tegrals can be found <strong>in</strong> references [186,220,221].B.2.2Bubble basis <strong>in</strong>tegralsThe <strong>two</strong> po<strong>in</strong>t bubble <strong>in</strong>tegral <strong>in</strong>tegr<strong>at</strong>es to the follow<strong>in</strong>g,( )1 µ2 ǫI 2 (s) =. (B.2.20)ǫ(1 − 2ǫ) −s<strong>in</strong> this thesis we comb<strong>in</strong>e bubble <strong>in</strong>tegrals to produce the follow<strong>in</strong>g basis functions,L k (s, t) =log (s/t)(s − t) k , (B.2.21)which we then complete to avoid the presence <strong>of</strong> spurious (s → t) s<strong>in</strong>gularities.(L 3 (s, t) → ˆL 1 13 (s, t) = L 3 (s, t) −2(s − t) 2 s + 1 ),t

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