AbstractAbstract
[en] We compare the results of the fixed-flavor scheme calculation of Laenen, Riemersma, Smith, and van Neerven with the variable-flavor scheme calculation of Aivazis, Collins, Olness, and Tung for the case of neutral-current (photon-mediated) heavy-flavor (charm and bottom) production. Specifically, we examine the features of both calculations throughout phase space and compare the structure function F2(x,Q2). We also analyze the dependence of F2 on the mass factorization scale μ. We find that the former is most applicable near threshold, while the latter works well for asymptotic Q2. The validity of each calculation in the intermediate region is dependent upon the x and Q2 values chosen
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Agrawal, P.; Tung, Wu-Ki; Olness, F.I.; Riemersma, S.T.
'95 QCD and high energy hadronic interactions1995
'95 QCD and high energy hadronic interactions1995
AbstractAbstract
[en] Two existing calculation methods are compared. As expected from physical grounds, the next-to-leading-order fixed-flavor scheme calculation yields good results near threshold, while the leading-order variable-flavor scheme calculation works well for asymptotic Q2. The quality of the calculations in the intermediate region is dependent upon the x and Q2 values chosen. An accurate self-consistent QCD calculation over the entire range can be obtained by extending the variable-flavor scheme to next-to-leading-order. Recent work to carry out this calculation is described. Preliminary numerical results of this calculation are also presented for comparison. (author)
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Tran Thanh Van, J. (ed.); [669 p.]; ISBN 2-86332-184-6; ; 1995; p. 353-359; 30. Moriond particle physics meeting; Les Arcs, Savoie (France); 18-25 Mar 1995; 16 refs.
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