Abstract
Using methods from effective field theory, we develop a novel, systematic framework for the calculation of the cross sections for electroweak gauge-boson production at small and very small transverse momentum q T , in which large logarithms of the scale ratio M V /q T are resummed to all orders. These cross sections receive logarithmically enhanced corrections from two sources: the running of the hard matching coefficient and the collinear factorization anomaly. The anomaly leads to the dynamical generation of a non-perturbative scale \( {q_* } \sim {M_V}{e^{ - {\text{const}}/{\alpha_s}\left( {{M_V}} \right)}} \), which protects the processes from receiving large long-distance hadronic contributions. Expanding the cross sections in either α s or q T generates strongly divergent series, which must be resummed. As a by-product, we obtain an explicit non-perturbative expression for the intercept of the cross sections at q T = 0, including the normalization and first-order α s (q ∗ ) correction. We perform a detailed numerical comparison of our predictions with the available data on the transverse-momentum distribution in Z-boson production at the Tevatron and LHC.
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ArXiv ePrint: 1109.6027
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Becher, T., Neubert, M. & Wilhelm, D. Electroweak gauge-boson production at small q T : Infrared safety from the collinear anomaly. J. High Energ. Phys. 2012, 124 (2012). https://doi.org/10.1007/JHEP02(2012)124
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DOI: https://doi.org/10.1007/JHEP02(2012)124