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Berends, F.A., van Neerven, W.L., Burgers, G.J.H.: Higher order radiative corrections at LEP energies. Nucl. Phys. B
297, 429–478 (1988). [Erratum-ibid. B
304, 921 (1988)];Blümlein, J., De Freitas, A., van Neerven, W.: Two-loop QED operator matrix elements with massive external fermion lines. Nucl. Phys. B
855, 508–569 (2012). [arXiv:1107.4638 [hep-ph]];Hamberg, R., van Neerven, W.L., Matsuura, T.: A complete calculation of the order α
s 2 correction to the Drell-Yan K-factor. Nucl. Phys. B
359, 343–405 (1991). [Erratum-ibid. B
644, 403–404 (2002)];Zijlstra, E.B., van Neerven, W.L.: Contribution of the second order gluonic Wilson coefficient to the deep inelastic structure function. Phys. Lett. B
273, 476–482 (1991); O(α
s 2) contributions to the deep inelastic Wilson coefficient. Phys. Lett. B
272, 127–133 (1991); O(α
s 2) QCD corrections to the deep inelastic proton structure functions
F 2 and
F L . Nucl. Phys. B
383, 525–574 (1992); O(α
s 2) corrections to the polarized structure function
g 1(
x,
Q 2). Nucl. Phys. B
417, 61–100 (1994). [Erratum-ibid. B
426, 245 (1994)], [Erratum-ibid. B
773, 105–106 (2007)];Kazakov, D.I., Kotikov, A.V.: Totalas correction to deep-inelastic scattering cross section ratio
R = σ
L ∕σ
T in QCD. Calculation of the longitudinal structure function. Nucl. Phys. B
307, 721–762 (1988). [Erratum-ibid. B
345, 299 (1990)];Kazakov, D.I., Kotikov, A.V., Parente, G., Sampayo, O.A., Sanchez Guillen, J.: Complete quartic (α
s 2) correction to the deep inelastic longitudinal structure function
F L in QCD. Phys. Rev. Lett.
65, 1535–1538 (1990). [Erratum-ibid.
65, 2921 (1990)];Sanchez Guillen, J., Miramontes, J., Miramontes, M., Parente, G., Sampayo, O.A.: Next-toleading order analysis of the deep inelastic
R = σ
L ∕σ
total . Nucl. Phys. B
353, 337–345 (1991)