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000192622 0247_ $$2doi$$a10.1103/PhysRevD.90.094005
000192622 0247_ $$2ISSN$$a0556-2821
000192622 0247_ $$2ISSN$$a1089-4918
000192622 0247_ $$2ISSN$$a1550-2368
000192622 0247_ $$2ISSN$$a1550-7998
000192622 0247_ $$2arXiv$$aarXiv:1409.0514
000192622 0247_ $$2altmetric$$aaltmetric:2875458
000192622 0247_ $$2inspire$$ainspire:1313154
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000192622 0881_ $$aDESY-14-197; arXiv:1409.0514
000192622 088__ $$2DESY$$aDESY-14-197
000192622 088__ $$2arXiv$$aarXiv:1409.0514
000192622 1001_ $$0P:(DE-H253)PIP1006346$$aLipatov, Artem$$b0$$eCorresponding Author
000192622 245__ $$aTMD parton densities in associated real and virtual photon and jet production at LHC
000192622 260__ $$a[S.l.]$$bSoc.$$c2014
000192622 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2014-11-10
000192622 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2014-11-01
000192622 3367_ $$00$$2EndNote$$aJournal Article
000192622 3367_ $$2DRIVER$$aarticle
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000192622 500__ $$aOA
000192622 520__ $$aWe study the associated production of real (isolated) or virtual photons (with their subsequent leptonic decay) and hadronic jets in proton-proton collisions at the LHC using the ${k}_{T}$-factorization approach of QCD. The consideration is based on the off-shell quark-gluon QCD Compton scattering subprocesses. In the case of virtual photon production, the contributions from $Z$ boson exchange as well as ${\gamma }^{*}-Z$ interference with the full spin correlations are included. The transversemomentum-dependent (TMD) quark and gluon densities in a proton are determined from the Kimber-Martin-Ryskin prescription or Catani-Ciafoloni-Fiorani-Marchesini (CCFM) equation. In the latter, we restrict to the case where the gluon-to-quark splitting occurs at the last evolution step and calculate the sea quark density as a convolution of the CCFM-evolved gluon distribution and the TMD gluon-to-quark splitting function. Our numerical predictions are compared with the recent experimental data taken by the ATLAS Collaboration. We discuss the theoretical uncertainties of our calculations and argue that further studies are capable of constraining the TMD parton densities in the proton.
000192622 536__ $$0G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405$$aExperiments at LHC (CMS) (POF2-512)$$cPOF2-512$$fPOF II$$x0
000192622 542__ $$2Crossref$$i2014-11-10$$uhttp://link.aps.org/licenses/aps-default-license
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000192622 650_7 $$2autogen$$aphoton: virtual
000192622 650_7 $$2autogen$$aparton: density
000192622 650_7 $$2autogen$$agluon: density
000192622 650_7 $$2autogen$$aquark: density
000192622 650_7 $$2autogen$$aphoton: production
000192622 650_7 $$2autogen$$ajet: production
000192622 650_7 $$2autogen$$aspin: correlation
000192622 650_7 $$2autogen$$ajet: hadronic
000192622 650_7 $$2autogen$$aZ0: exchange
000192622 650_7 $$2autogen$$aquark: sea
000192622 650_7 $$2autogen$$atransverse momentum: factorization
000192622 650_7 $$2autogen$$ap p: scattering
000192622 650_7 $$2autogen$$atransverse momentum dependence
000192622 650_7 $$2autogen$$aquantum chromodynamics
000192622 650_7 $$2autogen$$aCERN LHC Coll
000192622 650_7 $$2autogen$$aassociated production
000192622 650_7 $$2autogen$$aevolution equation
000192622 650_7 $$2autogen$$aCompton scattering
000192622 650_7 $$2autogen$$asplitting function
000192622 650_7 $$2autogen$$aleptonic decay
000192622 650_7 $$2autogen$$aCCFM equation
000192622 650_7 $$2autogen$$ainterference
000192622 650_7 $$2autogen$$aquark gluon
000192622 650_7 $$2autogen$$asplitting
000192622 650_7 $$2autogen$$aoff-shell
000192622 650_7 $$2autogen$$aATLAS
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000192622 7001_ $$0P:(DE-H253)PIP1001174$$aZotov, Nikolai$$b1
000192622 77318 $$2Crossref$$3journal-article$$a10.1103/physrevd.90.094005$$b : American Physical Society (APS), 2014-11-10$$n9$$p094005$$tPhysical Review D$$v90$$x1550-7998$$y2014
000192622 773__ $$0PERI:(DE-600)2844732-3$$a10.1103/PhysRevD.90.094005$$gVol. D90, no. 9, p. 094005$$n9$$p094005$$tPhysical review / D$$v90$$x1550-7998$$y2014
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