Semi-inclusive deep inelastic scattering at small transverse momentum
By A. Bacchetta, M. Diehl, K. Goeke, A. Metz, P. Mulders, M. Schlegel. 2006
532 citations recorded by the source corpus.
We study the cross section for one-particle inclusive deep inelastic scattering off the nucleon for low transverse momentum of the detected hadron. We decompose the cross section in terms of structure functions and calculate them at tree level in terms of transverse-momentum-dependent parton distribution and fragmentation functions. Our results are complete in the one-photon exchange approximation at leading and first subleading twist accuracy, with both beam and target polarization.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/7a83cef6fb9cd946b43833fc8aaf9c72c77aeac7
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In Nuclear and High Energy Physics
Citations in the corpus
- Generalized parton correlation functions for a spin-0 hadron (2008, unknown): “Projection of GTMDs onto TMDs and GPDs 8 4.1 TMD-limit 8 4.2 GPD-limit 9 4.3 Relations between GPDs and TMDs 11”
- Transverse spin effects in hadron-pair production from semi-inclusive deep inelastic scattering (2009, methodology): “Among the five lepton-polarisation-independent TSAs that appear in SIDIS and DY, three are induced by the “twist-2” Sivers ( f⊥ 1T ), transversity (h1), pretzelosity (h ⊥ 1T ) TMD PDFs, while the other two are related to various “twist-3” objects [22, 23].”
- Effects of transversity in deep-inelastic scattering by polarized protons (2010, unknown): “2 T) , (2) where Ph⊥ ≡ |Ph − (Ph·q)q |q|2 | is the transverse momentum of the produced hadron, and Dq→h 1 is the polarizationaveragedquarkfragmentationfunction. The notation C denotes the convolution [9] C ... = x X q e2 q Z d2p Td 2k δ(2) p −k − Ph⊥ z ... , (3) where the sum runs over the quark fl”
- Semi-inclusive processes at low and high transverse momentum (2008, background): “The lepton-hadron cross section can then be parameterized as [14]”