[1]

F.D. Aaron and others. Combined Measurement and QCD Analysis of the Inclusive e+- p Scattering Cross Sections at HERA. JHEP, 1001:109, 2010. 61 pages, 21 figures.

[2]

H. Abramowicz and others. Combination and QCD Analysis of Charm Production Cross Section Measurements in Deep-Inelastic ep Scattering at HERA. Eur.Phys.J., C73:2311, 2013.

[3]

C. Adolph and others. Hadron Transverse Momentum Distributions in Muon Deep Inelastic Scattering at 160 GeV/c. Eur.Phys.J., C73:2531, 2013.

[4]

C.A. Aidala, B. Field, L.P. Gamberg, and T.C. Rogers. Limits on TMD Evolution From Semi-Inclusive Deep Inelastic Scattering at Moderate Q. Phys.Rev., D89:094002, 2014.

[5]

A. Airapetian and others. Multiplicities of charged pions and kaons from semi-inclusive deep-inelastic scattering by the proton and the deuteron. Phys.Rev., D87:074029, 2013.

[6]

Guido Altarelli and G. Parisi. Asymptotic Freedom in Parton Language. Nucl. Phys., B126:298, 1977.

[7]

M. Anselmino and others. Comparing extractions of Sivers functions. 2005.

[8]

M. Anselmino and others. Sivers Effect for Pion and Kaon Production in Semi- Inclusive Deep Inelastic Scattering. Eur. Phys. J., A39:89–100, 2009.

[9]

M. Anselmino, M. Boglione, J.O. Gonzalez H., S. Melis, and A. Prokudin. Unpolarised Transverse Momentum Dependent Distribution and Fragmentation Functions from SIDIS Multiplicities. JHEP, 1404:005, 2014.

[10]

Emil Avsar. On the Understanding and Use of 'Unintegrated' Parton Distributions in Small-x QCD. Int.J.Mod.Phys.Conf.Ser., 04:74–84, 2011.

[11]

Emil Avsar. TMD factorization and the gluon distribution in high energy QCD. 2012.

[12]

S. Mert Aybat and Ted C. Rogers. TMD Parton Distribution and Fragmentation Functions with QCD Evolution. Phys.Rev., D83:114042, 2011.

[13]

S. Mert Aybat, John C. Collins, Jian-Wei Qiu, and Ted C. Rogers. The QCD Evolution of the Sivers Function. Phys.Rev., D85:034043, 2012.

[14]

Alessandro Bacchetta, Markus Diehl, Klaus Goeke, Andreas Metz, Piet J. Mulders, and others. Semi-inclusive deep inelastic scattering at small transverse momentum. JHEP, 0702:093, 2007.

[15]

I. I. Balitsky and L. N. Lipatov. The Pomeranchuk Singularity in Quantum Chromodynamics. Sov. J. Nucl. Phys., 28:822–829, 1978.

[16]

A. Bermudez Martinez, P. Connor, F. Hautmann, H. Jung, A. Lelek, V. Radescu, and R. lebk. Collinear and TMD parton densities from fits to precision DIS measurements in the parton branching method. Phys. Rev., D99(7):074008, 2019.

[17]

E. Blanco, A. van Hameren, H. Jung, A. Kusina, and K. Kutak. Z boson production in proton-lead collisions at the LHC accounting for transverse momenta of initial partons. 2019.

[18]

Daniel Boer and Piet J. Mulders. Time reversal odd distribution functions in leptoproduction. Phys.Rev., D57:5780–5786, 1998.

[19]

Giuseppe Bozzi, Stefano Catani, Daniel de Florian, and Massimiliano Grazzini. Transverse-momentum resummation and the spectrum of the Higgs boson at the LHC. Nucl.Phys., B737:73–120, 2006.

[20]

R. Brun and F. Rademakers. ROOT: An object oriented data analysis framework. Nucl.Instrum.Meth., A389:81–86, 1997.

[21]

A. Buckley. New access to PDF data via LHAPDF6. In Les Houches 2013: Physics at TeV Colliders: Standard Model Working Group Report, 2014.

[22]

M.G.A. Buffing, A. Mukherjee, and Piet J. Mulders. Generalized Universality of Higher Transverse Moments of Quark TMD Correlators. Phys.Rev., D86:074030, 2012.

[23]

M.G.A. Buffing, Piet J. Mulders, and A. Mukherjee. Universality of Quark and Gluon TMD Correlators. Int.J.Mod.Phys.Conf.Ser., 25:1460003, 2014.

[24]

Marcin Bury, Andreas van Hameren, Hannes Jung, Krzysztof Kutak, Sebastian Sapeta, and Mirko Serino. Calculations with off-shell matrix elements, TMD parton densities and TMD parton showers. Eur. Phys. J., C78(2):137, 2018.

[25]

S. Catani and F. Hautmann. Quark anomalous dimensions at small x. Phys.Lett., B315:157–163, 1993.

[26]

S. Catani and F. Hautmann. High-energy factorization and small x deep inelastic scattering beyond leading order. Nucl. Phys., B427:475–524, 1994.

[27]

S. Catani, M. Ciafaloni, and F. Hautmann. GLUON CONTRIBUTIONS TO SMALL x HEAVY FLAVOR PRODUCTION. Phys. Lett., B242:97, 1990.

[28]

S. Catani, F. Fiorani, and G. Marchesini. Qcd coherence in initial state radiation. Phys. Lett. B, 234:339, 1990.

[29]

S. Catani, F. Fiorani, and G. Marchesini. Small x Behavior of Initial State Radiation in Perturbative QCD. Nucl. Phys., B336:18, 1990.

[30]

S. Catani, M. Ciafaloni, and F. Hautmann. High-energy factorization and small x heavy flavor production. Nucl. Phys., B366:135–188, 1991.

[31]

S. Catani, M. Ciafaloni, and F. Hautmann. High-energy factorization in QCD and minimal subtraction scheme. Phys. Lett., B307:147–153, 1993.

[32]

I.O. Cherednikov and N.G. Stefanis. Wilson lines and transverse-momentum dependent parton distribution functions: A Renormalization-group analysis. Nucl.Phys., B802:146–179, 2008.

[33]

I.O. Cherednikov and N.G. Stefanis. Renormalization-group properties of transverse-momentum dependent parton distribution functions in the light-cone gauge with the Mandelstam-Leibbrandt prescription. Phys.Rev., D80:054008, 2009.

[34]

Jui-Yu Chiu, Ambar Jain, Duff Neill, and Ira Z. Rothstein. A Formalism for the Systematic Treatment of Rapidity Logarithms in Quantum Field Theory. JHEP, 1205:084, 2012.

[35]

Jui-yu Chiu, Ambar Jain, Duff Neill, and Ira Z. Rothstein. The Rapidity Renormalization Group. Phys.Rev.Lett., 108:151601, 2012.

[36]

Marcello Ciafaloni and Gianni Camici. Energy scale(s) and next-to-leading BFKL equation. Phys.Lett., B430:349–354, 1998.

[37]

M. Ciafaloni. Coherence effects in initial jets at small q²/s. Nucl. Phys. B, 296:49, 1988.

[38]

John C. Collins and R. Keith Ellis. Heavy quark production in very high-energy hadron collisions. Nucl. Phys., B360:3–30, 1991.

[39]

John C. Collins and F. Hautmann. Infrared divergences and nonlightlike eikonal lines in Sudakov processes. Phys.Lett., B472:129–134, 2000.

[40]

John C. Collins and Andreas Metz. Universality of soft and collinear factors in hard-scattering factorization. Phys.Rev.Lett., 93:252001, 2004.

[41]

J. C. Collins and others. Sivers effect in Drell Yan at RHIC. Phys. Rev., D73:094023, 2006.

[42]

J. C. Collins and others. Sivers effect in semi-inclusive deeply inelastic scattering. Phys. Rev., D73:014021, 2006.

[43]

John C. Collins and Davison E. Soper. Back-To-Back Jets in QCD. Nucl.Phys., B193:381, 1981.

[44]

John C. Collins and Davison E. Soper. Parton Distribution and Decay Functions. Nucl.Phys., B194:445, 1982.

[45]

John C. Collins, Davison E. Soper, and George F. Sterman. Does the Drell-Yan Cross-section Factorize? Phys.Lett., B109:388, 1982.

[46]

John C. Collins, Davison E. Soper, and George F. Sterman. Factorization for One Loop Corrections in the Drell-Yan Process. Nucl.Phys., B223:381, 1983.

[47]

John C. Collins, Davison E. Soper, and George F. Sterman. Transverse Momentum Distribution in Drell-Yan Pair and W and Z Boson Production. Nucl.Phys., B250:199, 1985.

[48]

John C. Collins. Foundations of perturbative QCD, volume 32. Cambridge monographs on particle physics, nuclear physics and cosmology., 2011.

[49]

M. Deak, F. Hautmann, H. Jung, and K. Kutak. Forward-Central Jet Correlations at the Large Hadron Collider, 2010.

[50]

M. Deak, F. Hautmann, H. Jung, and K. Kutak. Forward Jets and Energy Flow in Hadronic Collisions. Eur.Phys.J., C72:1982, 2012.

[51]

Yuri L. Dokshitzer. Calculation of the Structure Functions for Deep Inelastic Scattering and e+ e- Annihilation by Perturbation Theory in Quantum Chromodynamics. Sov. Phys. JETP, 46:641–653, 1977.

[52]

Fabio Dominguez, A.H. Mueller, Stephane Munier, and Bo-Wen Xiao. On the small-x evolution of the color quadrupole and the Weizsácker-Williams gluon distribution. Phys.Lett., B705:106–111, 2011.

[53]

Fabio Dominguez, Jian-Wei Qiu, Bo-Wen Xiao, and Feng Yuan. On the linearly polarized gluon distributions in the color dipole model. Phys.Rev., D85:045003, 2012.

[54]

Fabio Dominguez. Unintegrated Gluon Distributions at Small-x. 10022/AC:P:11293, 2011.

[55]

Miguel G. Echevarria, Ahmad Idilbi, and Ignazio Scimemi. Factorization Theorem For Drell-Yan At Low q_T And Transverse Momentum Distributions On-The-Light-Cone. JHEP, 1207:002, 2012.

[56]

Miguel G. Echevarria, Ahmad Idilbi, Andreas Schaefer, and Ignazio Scimemi. Model-Independent Evolution of Transverse Momentum Dependent Distribution Functions (TMDs) at NNLL. Eur.Phys.J., C73:2636, 2013.

[57]

Miguel G. Echevarria, Ahmad Idilbi, and Ignazio Scimemi. A Unified Treatment of the QCD Evolution of All (Un-)Polarized TMD Functions: Collins Function as a Study Case. Phys.Rev., D90:014003, 2014.

[58]

Miguel G. Echevarria, Tomas Kasemets, Piet J. Mulders, and Cristian Pisano. QCD evolution of (un)polarized gluon TMDPDFs and the Higgs q_T-distribution. JHEP, 07:158, 2015.

[59]

Victor S. Fadin and L.N. Lipatov. BFKL pomeron in the next-to-leading approximation. Phys.Lett., B429:127–134, 1998.

[60]

Victor S. Fadin, E.A. Kuraev, and L.N. Lipatov. On the Pomeranchuk Singularity in Asymptotically Free Theories. Phys.Lett., B60:50–52, 1975.

[61]

K. Golec-Biernat and M. Wusthoff. Saturation in diffractive deep inelastic scattering. Phys. Rev. D, 60:114023, 1999.

[62]

V. N. Gribov and L. N. Lipatov. Deep inelastic e p scattering in perturbation theory. Sov. J. Nucl. Phys., 15:438–450, 1972.

[63]

Marco Guzzi, Pavel M. Nadolsky, and Bowen Wang. Nonperturbative contributions to a resummed leptonic angular distribution in inclusive neutral vector boson production. Phys.Rev., D90:014030, 2014.

[64]

M. Hansson and H. Jung. The status of CCFM unintegrated gluon densities, 23-27 April 2003. DIS 2003, St. Petersburg, Russia, hep-ph/0309009.

[65]

F. Hautmann and H. Jung. Recent results on unintegrated parton distributions. Nucl.Phys.Proc.Suppl., 184:64–72, 2008.

[66]

F. Hautmann and H. Jung. Transverse momentum dependent gluon density from DIS precision data. Nucl. Phys. B, 883:1 – 19, 2014.

[67]

F. Hautmann, M. Hentschinski, and H. Jung. TMD PDFs: A Monte Carlo implementation for the sea quark distribution. 2012.

[68]

F. Hautmann, H. Jung, and S. Taheri Monfared. The CCFM uPDF evolution uPDFevolv, 2014.

[69]

F. Hautmann. Heavy top limit and double-logarithmic contributions to higgs production at m(h)²/s ll 1. Phys. Lett., B535:159–162, 2002.

[70]

F. Hautmann. Endpoint singularities in unintegrated parton distributions. Phys.Lett., B655:26–31, 2007.

[71]

F. Hautmann. Unintegrated parton distributions and applications to jet physics. Acta Phys.Polon., B40:2139–2163, 2009.

[72]

S. Jadach and M. Skrzypek. QCD evolution in the fully unintegrated form. Acta Phys.Polon., B40:2071–2096, 2009.

[73]

H. Jung. Unintegrated parton density functions in CCFM, April 2004. DIS 2004, Strbské Pleso, Slovakia, hep-ph/0411287.

[74]

Anton V. Konychev and Pavel M. Nadolsky. Universality of the Collins-Soper-Sterman nonperturbative function in gauge boson production. Phys.Lett., B633:710–714, 2006.

[75]

Krzysztof Kutak and Sebastian Sapeta. Gluon saturation in dijet production in p-Pb collisions at Large Hadron Collider. Phys.Rev., D86:094043, 2012.

[76]

Krzysztof Kutak. Hard scale dependent gluon density, saturation and forward-forward dijet production at the LHC. Phys.Rev., D91(3):034021, 2015.

[77]

F. Landry, R. Brock, Pavel M. Nadolsky, and C. P. Yuan. Tevatron Run-1 Z boson data and Collins-Soper-Sterman resummation formalism. Phys. Rev., D67:073016, 2003.

[78]

E.M. Levin, M.G. Ryskin, Yu.M. Shabelski, and A.G. Shuvaev. Heavy quark production in semihard nucleon interactions. Sov.J.Nucl.Phys., 53:657, 1991.

[79]

L.N. Lipatov. Small x physics in perturbative QCD. Phys.Rept., 286:131–198, 1997.

[80]

G. Marchesini. Qcd coherence in the structure function and associated distributions at small x. Nucl. Phys. B, 445:49, 1995.

[81]

Xiang-dong Ji, Jian-ping Ma, and Feng Yuan. Qcd factorization for spin-dependent cross sections in dis and drell-yan processes at low transverse momentum. Phys. Lett., B597:299–308, 2004.

[82]

Xiang-dong Ji, Jian-ping Ma, and Feng Yuan. Qcd factorization for semi-inclusive deep-inelastic scattering at low transverse momentum. Phys. Rev., D71:034005, 2005.

[83]

Ruibin Meng, Fredrick I. Olness, and Davison E. Soper. Semi-Inclusive Deeply Inelastic Scattering at Small q_T. Phys. Rev., D54:1919–1935, 1996.

[84]

Piet J. Mulders and R.D. Tangerman. The Complete tree level result up to order 1/Q for polarized deep inelastic leptoproduction. Nucl.Phys., B461:197–237, 1996.

[85]

Pavel M. Nadolsky, D.R. Stump, and C.P. Yuan. Semiinclusive hadron production at HERA: The Effect of QCD gluon resummation. Phys.Rev., D61:014003, 2000.

[86]

Pavel M. Nadolsky, D.R. Stump, and C.P. Yuan. Phenomenology of multiple parton radiation in semiinclusive deep inelastic scattering. Phys.Rev., D64:114011, 2001.

[87]

P. Schweitzer, T. Teckentrup, and A. Metz. Intrinsic transverse parton momenta in deeply inelastic reactions. Phys.Rev., D81:094019, 2010.

[88]

Andrea Signori, Alessandro Bacchetta, Marco Radici, and Gunar Schnell. Investigations into the flavor dependence of partonic transverse momentum. JHEP, 1311:194, 2013.

[89]

Peng Sun, Joshua Isaacson, C. P. Yuan, and Feng Yuan. Universal Non-perturbative Functions for SIDIS and Drell-Yan Processes. 2014.

[weba]

http://root.cern.ch/http://root.cern.ch/.

[webb]

https://lhapdf.hepforge.org/lhapdf.hepforge.org/.