Parton Distribution Functions and Benchmark Cross Sections at NNLO
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S. Moch | S. Alekhin | J. Blumlein | J. Blumlein | J. Blümlein | S. Moch | S. Alekhin
[1] J. Breitweg. ZEUS results on the measurement and phenomenology of F(2) at low x and low Q**2 , 1999 .
[2] J. Latorre,et al. Precision determination of alpha_s using an unbiased global NLO parton set , 2011, 1103.2369.
[3] M. Jamin,et al. New determination ofαsfrom hadronicτdecays , 2011, 1110.1127.
[4] M. Gluck,et al. The strange sea density and charm production in deep inelastic charged current processes , 1996, hep-ph/9603304.
[5] Michele Arneodo,et al. Quark and gluon distributions and αs from nucleon structure functions at low x , 1993 .
[6] G. Dissertori,et al. Precise determination of the strong coupling constant at NNLO in QCD from the three-jet rate in electron-positron annihilation at LEP. , 2009, Physical review letters.
[7] V. Braun,et al. Renormalization of twist-four operators in QCD , 2009, 0908.1684.
[8] Heavy-quark correlations in deep-inelastic electroproduction , 1995, hep-ph/9503484.
[9] S. Moch,et al. The third-order QCD corrections to deep-inelastic scattering by photon exchange , 2005, hep-ph/0504242.
[10] T. Tuuva,et al. Measurement of the lepton charge asymmetry in inclusive W production in pp collisions at $ \sqrt {s} = 7\;{\text{TeV}} $ , 2011 .
[11] P. Jimenez-Delgado,et al. Dynamical next-to-next-to-leading order parton distributions , 2009 .
[12] Z. Nagy,et al. Three-jet cross sections in hadron-hadron collisions at next-to-leading order. , 2002, Physical review letters.
[13] R. Petti,et al. Update of the global fit of PDFs including the low-Q DIS data , 2008, DIS 2008.
[14] N. Kidonakis,et al. Effects of higher-order threshold corrections in high-E T jet production , 2000, hep-ph/0007268.
[15] J. Rubin,et al. How well do we know the neutron structure function? , 2011, Physical review letters.
[16] R. Petti,et al. Determination of strange sea distributions from νN deep inelastic scattering , 2008, 0812.4448.
[17] Juan Rojo,et al. A Higher Order Perturbative Parton Evolution Toolkit (HOPPET) , 2008, Comput. Phys. Commun..
[18] Richard D. Ball,et al. Impact of Heavy Quark Masses on Parton Distributions and LHC Phenomenology , 2011, 1101.1300.
[19] E. al.,et al. Measurement of three-jet differential cross sections dσ3jet/dM3jet in pp¯ collisions at s=1.96 TeV , 2011, 1104.1986.
[21] A. Djouadi,et al. NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders , 2003, hep-ph/0307206.
[22] Z. Nagy,et al. Next-to-leading order calculation of three jet observables in hadron hadron collision , 2003 .
[23] L. Dixon,et al. High-precision QCD at hadron colliders: Electroweak gauge boson rapidity distributions at next-to-next-to leading order , 2003, hep-ph/0312266.
[24] J. Smith,et al. Charm electroproduction viewed in the variable-flavour number scheme versus fixed-order perturbation theory , 1996, hep-ph/9612398.
[25] Riccardo Abbate,et al. Thrust at N3LL with power corrections and a precision global fit for αs(mZ) , 2010, 1006.3080.
[26] A. Vogt,et al. The Three-loop splitting functions in QCD: The Singlet case , 2004, hep-ph/0404111.
[27] G. Watt. Parton distribution function dependence of benchmark Standard Model total cross sections at the 7 TeV LHC , 2011, 1106.5788.
[28] R. Harlander,et al. Next-to-next-to-leading order Higgs production at Hadron Colliders. , 2002, Physical review letters.
[29] Klein,et al. Nuclear dependence of dimuon production at 800 GeV. , 1990, Physical review letters.
[30] Z. A. Ibrahim,et al. Measurement of D*± production in deep inelastic scattering at HERA , 2003, 1303.6578.
[31] G. D'Agostini,et al. On the use of the covariance matrix to fit correlated data , 1994 .
[32] A. Bodek,et al. Determination of the strange quark content of the nucleon from a next-to-leading-order QCD analysis of neutrino charm production , 1994 .
[33] J. Latorre,et al. On the impact of NMC data on NLO and NNLO parton distributions and Higgs production at the Tevatron and the LHC , 2011, 1102.3182.
[34] W. Marsden. I and J , 2012 .
[35] Ye Li,et al. FEWZ 2.0: A code for hadronic Z production at next-to-next-to-leading order , 2010, Comput. Phys. Commun..
[36] R. Petti,et al. Modeling Lepton‐Nucleon Inelastic Scattering from High to Low Momentum Transfer , 2007, 0710.0124.
[37] U. Langenfeld,et al. Measuring the running top-quark mass , 2009, 0906.5273.
[38] K. Orginos,et al. Nucleon structure from mixed action calculations using 2+1 flavors of asqtad sea and domain wall valence fermions , 2010, 1001.3620.
[39] Measurement of high-Q2 neutral current deep inelastic e−p scattering cross sections with a longitudinally polarised electron beam at HERA , 2009, 0901.2385.
[40] W. Neerven,et al. Order αs2 correction to the structure function F3(x, Q2) in deep inelastic neutrino-hadron scattering , 1992 .
[41] Deep-inelastic structure functions at two loops , 1999, hep-ph/9912355.
[42] R. S. Thorne,et al. Parton distributions incorporating QED contributions , 2005 .
[43] K. Kanaya,et al. Precise determination of the strong coupling constant in N(f) = 2+1 lattice QCD with the Schrodinger functional scheme , 2009, 0906.3906.
[44] K. Chetyrkin,et al. New Four Loop Results in QCD , 2006 .
[45] Bruce J. West,et al. Measurement of high-Q 2 e - p neutral current cross sections at HERA and the extraction of xF 3 : The ZEUS collaboration , 2003 .
[46] R. Machleidt,et al. The Bonn Meson Exchange Model for the Nucleon Nucleon Interaction , 1987 .
[47] V. Velizhanin. Four loop anomalous dimension of the second moment of the non-singlet twist-2 operator in QCD , 2011, 1112.3954.
[48] J. Blumlein,et al. Update of the NNLO PDFs in the 3-, 4-, and 5-flavour scheme , 2010, 1007.3657.
[49] I. Bierenbaum,et al. The gluonic operator matrix elements at O(αs2) for DIS heavy flavor production , 2009, 0901.0669.
[50] M. Wobisch. Recent QCD results from the Tevatron , 2012, 1202.0205.
[51] H Severini,et al. Measurement of the inclusive jet cross section in pp[over] collisions at square root [s]=1.96 TeV. , 2008, Physical review letters.
[52] S. Alekhin. Impact of the three-loop corrections on the QCD analysis of the deep-inelastic scattering data , 2001 .
[53] J. Kuhn,et al. Complete QCD Corrections to Hadronic $Z$--Decays in Order $α_s^4$ , 2012, 1201.5804.
[54] A. Mitov,et al. Soft gluon resummation for heavy quark production in charged current deep inelastic scattering , 2003, hep-ph/0308105.
[55] B. Malaescu,et al. Evaluation of the strong coupling constant αS using the ATLAS inclusive jet cross-section data , 2012, 1203.5416.
[56] R. S. Thorne,et al. Uncertainties on αS in global PDF analyses and implications for predicted hadronic cross sections , 2009, 0905.3531.
[57] J. G. Contreras,et al. Measurement of inclusive jet production in deep-inelastic scattering at high Q2 and determination of the strong coupling , 2007 .
[58] T. Aaltonen,et al. Direct Measurement of the W Production Charge Asymmetry in p anti-p Collisions at s**(1/2) = 1.96-TeV , 2009, 0901.2169.
[59] C. Davies,et al. High-Precision c and b Masses, and QCD Coupling from Current-Current Correlators in Lattice and Continuum QCD , 2008, 1004.4285.
[60] Michele Arneodo,et al. Measurement of the proton and the deuteron structure functions, F2p and F2d , 1995 .
[61] Luk,et al. Dimuon production in proton-copper collisions at sqrt s =38.8 GeV. , 1991, Physical review. D, Particles and fields.
[62] S. Chekanov,et al. High Q**2 neutral current cross-sections in e+ p deep inelastic scattering at s**(1/2) = 318-GeV , 2004 .
[63] B. Kniehl,et al. Associated production of Higgs and Z bosons from gluon fusion in hadron collisions. , 1990, Physical review. D, Particles and fields.
[64] T. Riemann,et al. HECTOR 1.00: A program for the calculation of QED, QCD and electroweak corrections to ep and l± N deep inelastic neutral and charged current scattering☆ , 1995, hep-ph/9511434.
[65] Johannes Blumlein,et al. Mellin representation for the heavy flavor contributions to deep inelastic structure functions , 2004 .
[66] S. Dasu,et al. Precise measurements of the proton and deuteron structure functions from a global analysis of the SLAC deep inelastic electron scattering cross sections , 1992 .
[67] A. Vogt,et al. Threshold-improved predictions for charm production in deep-inelastic scattering , 2010, 1008.0951.
[68] W. L. van Neerven,et al. Contribution of the second order gluonic Wilson coefficient to the deep inelastic structure function , 1991 .
[69] M. L. Ferrer,et al. Measurement of inclusive jet and dijet production in pp collisions at root s=7 TeV using the ATLAS detector , 2012 .
[70] R. Petti,et al. Neutrino inclusive inelastic scattering off nuclei , 2007, hep-ph/0703033.
[71] Giulia Zanderighi,et al. NLO QCD corrections to five-jet production at LEP and the extraction of αs(MZ) , 2010, 1008.5313.
[72] A. Martin,et al. Parton distributions for the LHC , 2009, 0901.0002.
[73] V. Krivokhizhin,et al. QCD coupling constant at next-to-next-to-leading order from DIS data , 2010 .
[74] E. Bloom,et al. Ratio sigma/sub L//sigma/sub T/ from deep-inelastic electron scattering , 1983 .
[75] E. al.,et al. Applications of quark-hadron duality in the F-2 structure function , 2009, 0905.2374.
[76] T. Gottschalk. Chromodynamic corrections to neutrino production of heavy quarks , 1981 .
[77] J. Blümlein,et al. Higher-order constraints on the Higgs production rate from fixed-target DIS data , 2011, 1101.5261.
[78] W. L. van Neerven,et al. Heavy quark coefficient functions at asymptotic values Q2>>m2 , 1996, hep-ph/9601302.
[79] J. Blümlein,et al. Higher Twist contributions to the Structure Functions F_2(x,Q^2) and g_2(x,Q^2) , 2012 .
[80] Precise measurement of neutrino and anti-neutrino differential cross sections , 2006, hep-ex/0509010.
[81] S. Moch,et al. Running heavy-quark masses in DIS , 2011, 1107.0469.
[82] Alberto Guffanti,et al. Unbiased global determination of parton distributions and their uncertainties at NNLO and at LO , 2011, 1107.2652.
[83] J. Huston,et al. New parton distributions for collider physics , 2010, 1007.2241.
[84] Michele Arneodo,et al. Measurement of the proton and deuteron structure functions, F2p and F2d, and of the ratio sigmaL/sigmaT. , 1997 .
[85] Peter Uwer,et al. HATHOR - HAdronic Top and Heavy quarks crOss section calculatoR , 2011, Comput. Phys. Commun..
[86] Arnold,et al. Measurement of the A dependence of deep-inelastic electron scattering. , 1994, Physical review. D, Particles and fields.
[87] R. Kogler,et al. Precision jet measurements at HERA and determination of αs , 2011, 1112.5117.
[88] J. G. Contreras,et al. Measurement of D∗± meson production and determination of $F_{2}^{c\bar{c}}$ at low Q2 in deep-inelastic scattering at HERA , 2011, 1106.1028.
[89] H. Georgi,et al. Freedom at Moderate Energies: Masses in Color Dynamics , 1976 .
[90] Z. A. Ibrahim,et al. Measurement of charged current deep inelastic scattering cross sections with a longitudinally polarised electron beam at HERA , 2008, 0812.4620.
[91] Z. A. Ibrahim,et al. Measurement of charm and beauty production in deep inelastic ep scattering from decays into muons at , 2009 .
[92] M. Virchaux,et al. A measurement of αs and of higher twists from a QCD analysis of high statistics F2 data on hydrogen and deuterium targets , 1992 .
[93] S. Alekhin. Global fit to the charged leptons deep-inelastic-scattering data: α s , parton distributions, and high twists , 2001 .
[94] G. Luisoni,et al. Hadronisation effects in event-shape moments , 2009, 0911.2422.
[95] D. Bandurin. QCD measurements at the Tevatron , 2011, 1112.0051.
[96] J. Blumlein,et al. NNLO Benchmarks for Gauge and Higgs Boson Production at TeV Hadron Colliders , 2010, 1011.6259.
[97] R. Petti,et al. Global study of nuclear structure functions , 2004, hep-ph/0412425.
[98] E. Koffeman,et al. Measurement of D {* ±} production and the charm contribution to F 2 in deep inelastic scattering at HERA , 2000 .
[99] J. Kuhn,et al. Hadronic Z- and tau-Decays in Order alpha_s^4 , 2008, 0801.1821.
[100] J. G. Contreras,et al. Measurement of the inclusive e±p scattering cross section at high inelasticity y and of the structure function FL , 2010, 1012.4355.
[101] J. G. Contreras,et al. Measurement and QCD analysis of neutral and charged current cross-sections at HERA , 2003 .
[102] T. Okusawa,et al. Measurement of nucleon structure functions in neutrino scattering , 2006 .
[103] F. Maltoni,et al. Higgs boson production via vector-boson fusion at next-to-next-to-leading order in QCD. , 2010, Physical review letters.
[104] M. Grazzini,et al. W boson production at hadron colliders: the lepton charge asymmetry in NNLO QCD , 2010, DIS 2010.
[105] Takeshi Yamazaki,et al. Nucleon isovector structure functions in (2+1)-flavor QCD with domain wall fermions , 2010 .
[106] P. Boucaud,et al. Strong running coupling at τ and Z(0) mass scales from lattice QCD. , 2012, Physical review letters.
[107] A. Djouadi,et al. Predictions for Higgs production at the Tevatron and the associated uncertainties , 2010, 1009.1363.
[108] W. L. van Neerven,et al. Order α2S contributions to the deep inelastic Wilson coefficient , 1991 .
[109] P. Jimenez-Delgado,et al. On the role of heavy flavor parton distributions at high energy colliders , 2008, 0801.3618.
[110] S. Moch,et al. O ( a s ) heavy flavor corrections to charged current deep inelastic scattering in Mellin space , 2011, 1104.3449.
[111] S. Moch,et al. Heavy-quark deep-inelastic scattering with a running mass , 2010, 1011.5790.
[112] S. Alekhin,et al. Isospin dependence of power corrections in deep inelastic scattering , 2003, hep-ph/0304210.
[113] A. Gehrmann-De Ridder,et al. Double virtual corrections for gluon scattering at NNLO , 2012, 1211.2710.
[114] W. Lohmann,et al. A comparison of the structure functions F2 of the proton and the neutron from deep inelastic muon scattering at high Q2 , 1990 .
[115] S. Moch,et al. Higher order QCD corrections to charged-lepton deep-inelastic scattering and global fits of parton distributions , 2008, 0811.1412.
[116] E. al.,et al. Determination of the pole and MS̄ masses of the top quark from the tt̄ cross section , 2011, 1104.2887.
[117] F. Maltoni,et al. Vector boson fusion at next-to-next-to-leading order in QCD: Standard model Higgs boson and beyond , 2012 .
[118] R. Thorne,et al. PDF dependence of Higgs cross sections at the Tevatron and LHC: response to recent criticism , 2011, 1106.5789.
[119] M. Grazzini,et al. Vector boson production at hadron colliders: a fully exclusive QCD calculation at next-to-next-to-leading order. , 2009, Physical review letters.
[120] Kirill Melnikov,et al. Dilepton rapidity distribution in the Drell-Yan process at next-to-next-to-leading order in QCD. , 2003, Physical review letters.
[121] A. Vogt,et al. Next-to-next-to-leading order QCD corrections to the photon's parton structure , 2001, hep-ph/0110331.
[122] S. Chekanov,et al. Inclusive-jet and dijet cross-sections in deep inelastic scattering at HERA , 2007 .
[123] O. Nachtmann. Positivity constraints for anomalous dimensions , 1973 .
[124] Lord,et al. Proton and deuteron structure functions in muon scattering at 470 GeV. , 1995, Physical review. D, Particles and fields.
[125] Jaap Velthuis,et al. Measurement of the neutral current cross section and F-2 structure function for deep inelastic e(+)p scattering at HERA , 2001 .
[126] R. Harlander,et al. Top-quark mediated effects in hadronic Higgs-Strahlung , 2011, 1111.0761.
[127] T. Aaltonen,et al. Measurement of dσ/dy of Drell–Yan e+e− pairs in the Z mass region from collisions at , 2009, 0908.3914.
[128] K. Melnikov,et al. Fixed target Drell-Yan data and NNLO QCD fits of parton distribution functions , 2006, hep-ph/0606237.
[129] S. Moch,et al. Higher-order soft corrections to lepton pair and Higgs boson production , 2005 .
[130] A. Bodek,et al. A precise extraction of R=σL/σT from a global analysis of the SLAC deep inelastic e-p and e-d scattering cross sections , 1990 .
[131] C. Collaboration,et al. Measurement of the Inclusive Jet Cross Section in pp Collisions at sqrt(s) = 7 TeV , 2011, 1106.0208.
[132] A. Bodek,et al. Experimental studies of the neutron and proton electromagnetic structure functions , 1979 .
[133] V. Cerný,et al. Jet production in ep collisions at low Q2 and determination of αs , 2009, 0911.5678.
[134] E. al.,et al. Measurement of the muon charge asymmetry from W boson decays , 2007, 0709.4254.
[135] Z. Trocsanyi,et al. A subtraction scheme for computing QCD jet cross sections at NNLO: integrating the iterated singly-unresolved subtraction terms , 2010, 1011.1909.
[136] M. Grazzini,et al. Associated Higgs-W-boson production at hadron colliders: a fully exclusive QCD calculation at NNLO. , 2011, Physical review letters.
[137] A. Vogt,et al. Efficient evolution of unpolarized and polarized parton distributions with QCD-Pegasus , 2004, Comput. Phys. Commun..
[138] Johannes Blumlein,et al. Two-Loop Massive Operator Matrix Elements and Unpolarized Heavy Flavor Production at Asymptotic Values Q^2 >> m^2 , 2007 .
[139] A. V. Sidorov,et al. Test of QCD and a measurement of Λ from scaling violations in the proton structure function F2(x, Q2) at high Q2 , 1989 .
[140] Z. A. Ibrahim,et al. Measurement of D± and D0 production in deep inelastic scattering using a lifetime tag at HERA , 2008, 0812.3775.
[141] Bruce J. West,et al. Inclusive jet cross sections in the Breit frame in neutral current deep inelastic scattering at HERA and determination of alpha(s) , 2002 .
[142] G. Smadja,et al. A High Statistics Measurement of the Proton Structure Functions F(2) (x, Q**2) and R from Deep Inelastic Muon Scattering at High Q**2 , 1989 .
[143] W. Lohmann,et al. A high statistics measurement of the deuteron structure functions F2(x, Q2) and R from deep inelastic muon scattering at high Q2 , 1990 .
[144] M. Lacombe,et al. Parametrization of the Paris N-N potential , 1980 .
[145] Lang,et al. Measurement of kinematic and nuclear dependence of R= sigma L/ sigma T in deep inelastic electron scattering. , 1994, Physical review. D, Particles and fields.
[146] S. Bethke. EPJ manuscript No. (will be inserted by the editor) The 2009 World Average of αs , 2022 .
[147] G. G. Stokes. "J." , 1890, The New Yale Book of Quotations.
[148] K. Jansen,et al. Moments of nucleon generalized parton distributions from lattice QCD simulations at physical pion mass , 2011, Physical Review D.
[149] V. Ravindran,et al. NNLO corrections to the total cross section for Higgs boson production in hadron-hadron collisions , 2003, hep-ph/0302135.
[150] A. Vogt,et al. The longitudinal structure function at the third order , 2004, hep-ph/0411112.
[151] J. Blümlein,et al. Higher twist contributions to the structure functions F 2 p (x ,Q 2 ) and F 2 d (x ,Q 2 ) at large x at higher orders , 2008 .
[152] E. Bloom,et al. Inelastic electron scattering from hydrogen at 50° and 60°☆ , 1976 .
[153] A. Vogt,et al. Third-order QCD corrections to the charged-current structure function F 3 , 2008, 0812.4168.
[154] P. Jimenez-Delgado,et al. Variable flavor number parton distributions and weak gauge and Higgs boson production at hadron colliders at next-to-next-to-leading order of QCD , 2009, 0909.1711.
[155] K. Rabbertz,et al. Theory-Data Comparisons for Jet Measurements in Hadron-Induced Processes , 2011, 1109.1310.
[156] Johannes Blümlein,et al. 3-, 4-, and 5-flavor next-to-next-to-leading order parton distribution functions from deep-inelastic-scattering data and at hadron colliders , 2010 .
[157] O. Sampayo,et al. Next-to-leading order analysis of the deep inelastic R = σL/σT , 1991 .
[158] C. Schneider,et al. The O(αs3) massive operator matrix elements of O(nf) for the structure function F2(x,Q2) and transversity , 2010, Nuclear physics. B.
[159] C. Adloff. Deep inelastic inclusive e p scattering at low x and a determination of alpha(s) , 2001 .
[160] R. Petti,et al. Structure functions for light nuclei , 2010, 1004.3062.
[161] Zeus Collaborations. Combined Measurement and QCD Analysis of the Inclusive ep Scattering Cross Sections at HERA , 2009 .
[162] V. Ravindran,et al. Two-loop corrections to Higgs boson production , 2004, hep-ph/0408315.
[163] W. L. van Neerven,et al. Order-αs2 QCD corrections to the deep inelastic proton structure functions F2 and FL , 1992 .
[164] J. Smith,et al. Complete O(αS) corrections to heavy-flavour structure functions in electroproduction , 1993 .
[165] E. Shuryak,et al. Theory of power corrections to deep inelastic scattering in quantum chromodynamics (I). Q -2 effects , 1982 .
[166] S. Bethke,et al. O ct 2 01 1 Workshop on Precision Measurements of α s MPI , 2011 .
[167] Roelof Hamberg,et al. A complete calculation of the order αs2 correction to the Drell-Yan K-factor , 1991 .
[168] Strong coupling constant with flavor thresholds at four loops in the MS scheme , 1997, hep-ph/9706430.
[169] C. Anastasiou,et al. Higgs Boson Production at Hadron Colliders in NNLO QCD , 2002, hep-ph/0207004.
[170] Johannes Blumlein,et al. Mellin moments of the O(αs3) heavy flavor contributions to unpolarized deep-inelastic scattering at Q2≫m2 and anomalous dimensions , 2009, 0904.3563.