[1]

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

[2]

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

[3]

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

[4]

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

[5]

M.G.A. Buffing, A. Mukherjee, and P.J. Mulders. Generalized Universality of Definite Rank Gluon Transverse Momentum Dependent Correlators. Phys.Rev., D88:054027, 2013.

[6]

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

[7]

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

[8]

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

[9]

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

[10]

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

[11]

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

[12]

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

[13]

Marcello Ciafaloni. Coherence Effects in Initial Jets at Small q**2 / s. Nucl. Phys., B296:49, 1988.

[14]

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

[15]

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

[16]

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

[17]

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.

[18]

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

[19]

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

[20]

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

[21]

A.A. Grinyuk, A.V. Lipatov, G.I. Lykasov, and N.P. Zotov. Transition between soft physics at the LHC and low-x physics at HERA. Phys.Rev., D87(7):074017, 2013.

[22]

M. Hansson and H. Jung. Status of CCFM: Un-integrated gluon densities. 2003.

[23]

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

[24]

F. Hautmann and H. Jung. Transverse momentum dependent gluon density from DIS precision data. Nucl. Phys., B883:1 – 19, 2014.

[25]

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

[26]

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

[27]

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

[28]

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

[29]

F. James. Monte Carlo Theory and Practice. Rept.Prog.Phys., 43:1145, 1980.

[30]

Hannes Jung and Francesco Hautmann. Determination of transverse momentum dependent gluon density from HERA structure function measurements. 2012.

[31]

H. Jung and G. P. Salam. Hadronic final state predictions from CCFM: The hadron- level Monte Carlo generator CASCADE. Eur. Phys. J., C19:351–360, 2001.

[32]

H. Jung, S. Baranov, M. Deak, A. Grebenyuk, F. Hautmann, and others. The CCFM Monte Carlo generator CASCADE version 2.2.03. Eur.Phys.J., C70:1237, 2010.

[33]

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

[34]

G. Marchesini and B. Webber. Simulation of qcd inital state radiation at small x. Nucl. Phys. B, 349:617, 1991.

[35]

G. Marchesini and B. Webber. Final states in heavy quark leptoproduction at small x. Nucl. Phys. B, 386:215, 1992.

[36]

Giuseppe Marchesini. QCD coherence in the structure function and associated distributions at small x. Nucl. Phys., B445:49–80, 1995.

[37]

H. Jung et al. . TMDlib and TMDplotter. DESY-14-059.

[38]

P.J. Mulders. Non-collinearity in high energy processes. Pramana, 72:83–95, 2009.