Confronting Mueller-Navelet jets in NLL BFKL with LHC experiments at 7 TeV
暂无分享,去创建一个
[1] V. Gribov,et al. e+ e- pair annihilation and deep inelastic e p scattering in perturbation theory , 1972 .
[2] L. Lipatov. Parton model and perturbation theory , 1974 .
[3] L. Lipatov,et al. On the pomeranchuk singularity in asymptotically free theories , 1975 .
[4] L. Lipatov,et al. Multi - Reggeon Processes in the Yang-Mills Theory , 1976 .
[5] G. Parisi,et al. Asymptotic Freedom in Parton Language , 1977 .
[6] L. Lipatov,et al. The Pomeranchuk Singularity in Nonabelian Gauge Theories , 1977 .
[7] Y. Dokshitzer,et al. Calculation of the Structure Functions for Deep Inelastic Scattering and e+ e- Annihilation by Perturbation Theory in Quantum Chromodynamics. , 1977 .
[8] L. Lipatov,et al. The Pomeranchuk Singularity in Quantum Chromodynamics , 1978 .
[9] H. Navelet,et al. An inclusive minijet cross section and the bare pomeron in QCD , 1987 .
[10] L. Stanco,et al. HERWIG 5.1 - a Monte Carlo event generator for simulating hadron emission reactions with interfering gluons , 1992 .
[11] M. G. Ryskin,et al. DiffractiveJ/Ψ electroproduction in LLA QCD , 1993 .
[12] Higher-order corrections to jet cross sections in hadron colliders , 1993, hep-ph/9302225.
[13] A. Martin,et al. Implications of scaling violations of F2 at HERA for perturbative QCD , 1993, hep-ph/9311376.
[14] C. Schmidt,et al. BFKL versus O(\alpha_s^3) Corrections to Large-rapidity Dijet Production , 1994, hep-ph/9407359.
[15] Schmidt,et al. Dijet production at large rapidity intervals. , 1993, Physical review. D, Particles and fields.
[16] W. Stirling. Production of jet pairs at large relative rapidity in hadron-hadron collisions as a probe of the perturbative pomeron , 1994, hep-ph/9401266.
[17] V. Kim,et al. BFKL QCD Pomeron in High Energy Hadron Collisions and Inclusive Dijet Production 1 , 1995, hep-ph/9506381.
[18] Schmidt,et al. Balitsky-Fadin-Kuraev-Lipatov approximation versus O( alpha s3) corrections to large-rapidity dijet production. , 1995, Physical review. D, Particles and fields.
[19] Kim,et al. New effective Feynman-like rules for the multi-Regge QCD asymptotics of inclusive multijet production. , 1996, Physical review. D, Particles and fields.
[20] C. Royon,et al. Proton structure functions in the dipole picture of BFKL dynamics , 1996, hep-ph/9605389.
[21] A. Roeck,et al. The γ∗γ∗ total cross section and the BFKL Pomeron at e+e− colliders , 1996 .
[22] A. Białas,et al. Total gamma* gamma* cross-section and the BFKL pomeron , 1997, hep-ph/9705470.
[23] S. Brodsky,et al. Probing the QCD Pomeron in e + e − Collisions [Phys. Rev. Lett. 78, 803 (1997)] , 1997 .
[24] W. Stirling,et al. Dijet production at hadron-hadron colliders in the Balitskii-Fadin-Kuraev-Lipatov approach , 1997, hep-ph/9706529.
[25] A. Białas,et al. TOTAL γ ⋆ γ ⋆ CROSS SECTION AND THE BFKL POMERON 1 , 1997 .
[26] L. Lipatov,et al. BFKL pomeron in the next-to-leading approximation , 1998, hep-ph/9802290.
[27] G. Salam. A resummation of large sub-leading corrections at small x , 1998, hep-ph/9806482.
[28] M. Strikman,et al. Diffractive heavy quarkonium photoproduction and electroproduction in QCD , 1997, hep-ph/9702216.
[29] M. Ciafaloni,et al. Energy scale(s) and next-to-leading BFKL equation 1 Work supported in part by EU Network contract FM , 1998, hep-ph/9803389.
[30] Desy,et al. γ∗γ∗ total cross section in the dipole picture of BFKL dynamics , 1998, hep-ph/9812523.
[31] R. Peschanski,et al. High-energy factorization predictions for the charm structure function F2c at HERA , 1998, hep-ph/9802230.
[32] A. Białas,et al. Total $\gamma^{\star}\gamma^{\star}$ cross section and the QCD dipole picture , 1998 .
[33] M. Ciafaloni,et al. The BFKL Equation at Next-to-Leading Order and Beyond , 1998, hep-ph/9812366.
[34] G. Salam,et al. Renormalization group improved small x equation , 1999, hep-ph/9905566.
[35] C. Royon. γ∗γ∗ total cross-section in the dipole picture of BFKL dynamics , 1999 .
[36] The QCD Pomeron with optimal renormalization , 1999, hep-ph/9901229.
[37] B. Cox,et al. Hard color singlet exchange at the Tevatron , 1999, hep-ph/9908464.
[38] L. Motyka,et al. The QCD pomeron in e+e- collisions , 1999, hep-ph/9904464.
[39] M. Ciafaloni,et al. The BFKL equation at next-to-leading level and beyond 1 Work supported in part by the E.U. QCDNET co , 1999 .
[40] J. S. Hoftun,et al. Probing Balitsky-Fadin-Kuraev-Lipatov dynamics in the dijet cross section at large rapidity intervals in pp collisions at sqrt[s]=1800 and 630 GeV. , 1999, Physical review letters.
[41] D. Ostrovsky. NLO correction to one-jet inclusive production at high energies , 1999, hep-ph/9912258.
[42] L. Lipatov,et al. NLO corrections to the BFKL equation in QCD and in supersymmetric gauge theories , 2000, hep-ph/0004008.
[43] M. Boonekamp. total cross-section in the dipole picture of BFKL dynamics , 2000 .
[44] E. al.,et al. Probing BFKL dynamics in the dijet cross section at large rapidity intervals , 2000 .
[45] A. Schäfer,et al. Erratum to: “Light vector meson photoproduction at large t” , 2001 .
[46] A. Martin,et al. Azimuthal decorrelation of forward and backward jets at the Tevatron , 2001, hep-ph/0105039.
[47] J. Guillet,et al. Is a large intrinsic $k_{\mathrm{T}}$ needed to describe photon + jet photoproduction at HERA? , 2001, hep-ph/0107262.
[48] J. Bartels,et al. The NLO jet vertex for Mueller-Navelet and forward jets: The quark part , 2001, hep-ph/0112283.
[49] W. Stirling,et al. Mueller-Navelet jets at hadron colliders , 2001, hep-ph/0101180.
[50] S. Brodsky,et al. High-energy QCD asymptotic behavior of photon-photon collisions , 2002, hep-ph/0207297.
[51] G. Poludniowski,et al. Diffractive heavy vector meson production from the BFKL equation , 2002, hep-ph/0207027.
[52] Hard colour singlet exchange and gaps between jets at the Tevatron , 2001, hep-ph/0111090.
[53] G. Salam,et al. Renormalization group improved small x Green's function , 2003, hep-ph/0307188.
[54] J. Bartels,et al. The NLO jet vertex for Mueller-Navelet and forward jets: the gluon part , 2002, hep-ph/0206290.
[55] Vector meson photoproduction from the BFKL equation. 1. Theory , 2003, hep-ph/0306232.
[56] A. Schaefer,et al. Exclusive photoproduction of a heavy vector meson in QCD , 2004, hep-ph/0401131.
[57] S. Wallon,et al. Double diffractive -production in collisions , 2005 .
[58] S. Wallon,et al. BFKL resummation effects in gamma* gamma* —g rho rho , 2005, hep-ph/0508134.
[59] A. Papa,et al. Electroproduction of two light vector mesons in next-to-leading BFKL: study of systematic effects , 2005, hep-ph/0510397.
[60] S. Wallon,et al. Double diffractive $\rho$-production in $\gamma^*\gamma^*$ collisions , 2005, hep-ph/0507038.
[61] Dimitri Bourilkov,et al. The Les Houches accord PDFs (LHAPDF) and LHAGLUE , 2005, hep-ph/0508110.
[62] A. Papa,et al. Electroproduction of two light vector mesons in the next-to-leading approximation , 2005, hep-ph/0508162.
[63] A. Vera. The effect of NLO conformal spins in azimuthal angle decorrelation of jet pairs , 2006, hep-ph/0602250.
[64] J. Bartels,et al. NLO inclusive jet production in $k_T$-factorization , 2006, hep-ph/0608154.
[65] S. Wallon,et al. BFKL resummation effects in γ*γ* → ρρ , 2006 .
[66] E. al.,et al. Minijet deformation and charge-independent angular correlations on momentum subspace (eta, phi) in Au-Au collisions at root S-NN=130 GeV , 2004, nucl-ex/0411003.
[67] S. Wallon,et al. Diffractive production of two ρ0L mesons in e+e- collisions , 2007, hep-ph/0703166.
[68] Florian Schwennsen,et al. The Azimuthal decorrelation of jets widely separated in rapidity as a test of the BFKL kernel , 2007, hep-ph/0702158.
[69] F. Schwennsen. Phenomenology of jet physics in the BFKL formalism at NLO , 2007, hep-ph/0703198.
[70] P. Aurenche,et al. Jet–jet and hadron–jet correlations in hadro- and electroproduction , 2008, 0807.2133.
[71] A. Vera,et al. Collinear improvement of the BFKL kernel in the electroproduction of two light vector mesons , 2007, 0707.4100.
[72] O. Kepka,et al. Gaps between jets at hadron colliders in the next-to-leading BFKL framework , 2009, 0903.4598.
[73] E. Levin,et al. Two Parton Shower Background for Associate W Higgs Production , 2008, 0803.0646.
[74] et al,et al. Long range rapidity correlations and jet production in high energy nuclear collisions , 2009, 0909.0191.
[75] C. Royon,et al. Azimuthal decorrelation of Mueller-Navelet jets at the Tevatron and the LHC , 2007, 0704.3409.
[76] A. Martin,et al. Parton distributions for the LHC , 2009, 0901.0002.
[77] D. Volyanskyy,et al. Observation of long-range, near-side angular correlations in proton-proton collisions at the LHC , 2010, 1009.4122.
[78] S. Wallon,et al. First complete NLL BFKL calculation of Mueller Navelet jets at LHC , 2010, 1010.0160.
[79] G. I. Veres,et al. System size dependence of cluster properties from two-particle angular correlations in Cu+Cu and Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV , 2010 .
[80] S. Wallon,et al. Mueller Navelet jets at LHC - complete NLL BFKL calculation , 2010 .
[81] I Sedykh,et al. High transverse momentum triggered correlations over a large pseudorapidity acceptance in Au+Au collisions at s(NN)**1/2 = 200 GeV , 2009, 0903.2811.
[82] S. Wallon,et al. Mueller Navelet jets at LHC — complete next-to-leading BFKL calculation , 2010, 1002.1365.
[83] T. Tuuva,et al. Long-range and short-range dihadron angular correlations in central PbPb collisions at a nucleon-nucleon center of mass energy of 2.76 TeV , 2011, 1105.2438.
[84] Francois Gelis,et al. The ridge in proton-proton collisions at the LHC , 2010, 1009.5295.
[85] J. Bartels,et al. Recombination within multi-chain contributions in pp scattering , 2011, 1105.1638.
[86] A. Schäfer,et al. Elements of a theory for multiparton interactions in QCD , 2011, 1111.0910.
[87] A. Kovner,et al. Angular correlations in gluon production at high energy , 2010, 1012.3398.
[88] A. Rezaeian,et al. Ridge from the BFKL evolution and beyond , 2011, 1105.3275.
[89] Pavel Strachota,et al. Measurement of the azimuthal anisotropy for charged particle production in √ sNN = 2.76 TeV lead-lead collisions with the ATLAS detector , 2012 .
[90] D. Ivanov,et al. The next-to-leading order jet vertex for Mueller-Navelet and forward jets revisited , 2011, 1112.3752.
[91] Raju Venugopalan,et al. Explanation of systematics of CMS p+Pb high multiplicity di-hadron data at $\sqrt{s}_{\rm NN} = 5.02$ TeV , 2012, 1211.3701.
[92] D. Ivanov,et al. The next-to-leading order forward jet vertex in the small-cone approximation , 2012, 1202.1082.
[93] Jr.,et al. Anomalous centrality evolution of two-particle angular correlations from Au-Au collisions at √sNN=62 and 200 GeV , 2011, 1109.4380.
[94] R. Venugopalan,et al. Azimuthal collimation of long range rapidity correlations by strong color fields in high multiplicity hadron-hadron collisions. , 2012, Physical review letters.
[95] T. Tuuva,et al. Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\sqrt{s_{NN}}= 2.76\ \mbox{TeV}$ , 2012 .
[96] T. B. Skaali,et al. Anisotropic flow of charged hadrons, pions and (anti-)protons measured at high transverse momentum in Pb-Pb collisions at root S-NN=2.76 TeV , 2013 .
[97] Matthias Rudolph Richter,et al. Long-range angular correlations on the near and away side in p-Pb collisions at root S-NN=5.02 TeV , 2012, 1212.2001.
[98] G. Bruno,et al. Observation of long-range, near-side angular correlations in pPb collisions at the LHC , 2013 .
[99] R. Venugopalan,et al. Evidence for BFKL and saturation dynamics from dihadron spectra at the LHC , 2012, 1210.3890.
[100] D. Ivanov,et al. Mueller-Navelet small-cone jets at LHC in next-to-leading BFKL , 2012, 1211.7225.
[101] Raju Venugopalan,et al. Comparison of the color glass condensate to dihadron correlations in proton-proton and proton-nucleus collisions , 2013, 1302.7018.