For a list of pub­li­ca­tions or­dered by date with ci­ta­tion in­for­ma­tions see IN­SPIRE-HEP

N3LO QCD pre­dic­tions for W & Z bo­son pro­duc­tion

  • J. Camp¬≠bell, T. Neu¬≠mann, Third or¬≠der QCD pre¬≠dic¬≠tions for fidu¬≠cial W-¬≠bo¬≠son pro¬≠duc¬≠tion,
    arX­iv:2308.15382, JHEP 11 (2023) 127
  • T. Neu¬≠mann, J. Camp¬≠bell, Fidu¬≠cial Drel¬≠l-Yan pro¬≠duc¬≠tion at the LHC im¬≠proved by trans¬≠verse-¬≠mo¬≠men¬≠tum re¬≠sum¬≠ma¬≠tion at N4LLp+N3LO, arX¬≠iv:2207.07056, Phys.Rev.D 107 (2023) 1, L011506

Bo­son and di­bo­son processes with trans­verse-­mo­men­tum and jet-veto re­sum­ma­tion

  • J. Camp¬≠bell, R.K. El¬≠lis, T. Neu¬≠mann, S. Seth, Jet-veto re¬≠sum¬≠ma¬≠tion at N3LLp+NNLO in bo¬≠son pro¬≠duc¬≠tion process¬≠es, arX¬≠iv:2301.11768, JHEP 04 (2023) 106
  • J. Camp¬≠bell, R.K. El¬≠lis, T. Neu¬≠mann, S.Seth, Trans¬≠verse mo¬≠men¬≠tum re¬≠sum¬≠ma¬≠tion at N3LL+NNLO for di¬≠bo¬≠son process¬≠es, arX¬≠iv:2210.10724, JHEP 03 (2023) 080
  • T. Neu¬≠mann, The dipho¬≠ton qT spec¬≠turm at N3LL‚Ä≤+NNLO EPJC 81 (2021) 10, 905, arX¬≠iv:2107.12478
  • T. Becher, T. Neu¬≠mann, Fidu¬≠cial qT re¬≠sum¬≠ma¬≠tion of col¬≠or-s¬≠in¬≠glet processes at N3LL+NNLO, JHEP 03 (2021) 199, arX¬≠iv:2009.11437. Pub¬≠lic re¬≠lease of CuTe-M¬≠CFM and MCFM 10.0.

US Snow­mass Whitepa­per

  • F.F. Cordero, A. von Man¬≠teuf¬≠fel, T. Neu¬≠mann, Com¬≠pu¬≠ta¬≠tional Chal¬≠lenges for Mul¬≠ti¬≠-loop Col¬≠lider Phe¬≠nom¬≠e¬≠nol¬≠o¬≠gy: A Snow¬≠mass 2021 White Pa¬≠per, arX¬≠iv:2204.04200, Com¬≠put.¬≠Soft¬≠w.Big Sci. 6 (2022) 1, 14
  • signee and con¬≠trib¬≠u¬≠tor of other whitepa¬≠pers, see IN¬≠SPIRE-HEP


  • J. Camp¬≠bell, T. Neu¬≠mann, Pre¬≠ci¬≠sion Phe¬≠nom¬≠e¬≠nol¬≠ogy with MCFM, JHEP 1912 (2019) 034, arX¬≠iv:1909.09117. Re¬≠lease pub¬≠li¬≠ca¬≠tion of MCFM-9.0. We ad¬≠dress in gen¬≠eral the is¬≠sues for reach¬≠ing high pre¬≠ci¬≠sion in Monte Carlo in¬≠te¬≠gra¬≠tion for higher or¬≠der cal¬≠cu¬≠la¬≠tions, slic¬≠ing pa¬≠ra¬≠me¬≠ter de¬≠pen¬≠dence of higher or¬≠der cal¬≠cu¬≠la¬≠tions and in pre¬≠ci¬≠sion physics like Drel¬≠l-Yan, and the ef¬≠fi¬≠cient cal¬≠cu¬≠la¬≠tion of PDF un¬≠cer¬≠tain¬≠ties at NN¬≠LO.

Sin­gle-­top-quark pro­duc­tion at NNLO and in SMEFT

  • J. Camp¬≠bell, T. Neu¬≠mann, Z. Sul¬≠li¬≠van, Test¬≠ing par¬≠ton dis¬≠tri¬≠b¬≠u¬≠tion func¬≠tions with t-chan¬≠nel sin¬≠gle-¬≠top-quark pro¬≠duc¬≠tion arX¬≠iv:2109.10448, Phys.Rev.D 104 (2021) 9, 094042
  • J. Camp¬≠bell, T. Neu¬≠mann, Z. Sul¬≠li¬≠van, Sin¬≠gle-¬≠top-quark pro¬≠duc¬≠tion in the t-chan¬≠nel at NNLO, arX¬≠iv:2012.01574, JHEP 02 (2021) 040. Pub¬≠licly avail¬≠able since MCFM-9.1.
  • T. Neu¬≠mann, Z.E. Sul¬≠li¬≠van, Of¬≠f-shell sin¬≠gle-¬≠top-quark pro¬≠duc¬≠tion in the Stan¬≠dard Model Ef¬≠fec¬≠tive Field The¬≠o¬≠ry, JHEP 1906 (2019) 022, arX¬≠iv:1903.11023. Pub¬≠licly avail¬≠able since MCFM-8.3.

The per­tur­ba­tive QCD gra­di­ent flow

  • R.V. Har¬≠lan¬≠der, F. Lange, T. Neu¬≠mann, Hadronic vac¬≠uum po¬≠lar¬≠iza¬≠tion us¬≠ing gra¬≠di¬≠ent flow arX¬≠iv:2007.01057.
  • J. Artz, R.V. Har¬≠lan¬≠der, F. Lange, T. Neu¬≠mann, M. Prausa, Re¬≠sults and tech¬≠niques for higher or¬≠der cal¬≠cu¬≠la¬≠tions within the gra¬≠di¬≠ent flow for¬≠mal¬≠ism, JHEP 1906 (2019) 121, arX¬≠iv:1905.00882.
  • R.V. Har¬≠lan¬≠der, T. Neu¬≠mann, The per¬≠tur¬≠ba¬≠tive QCD gra¬≠di¬≠ent flow to three loops, JHEP 1606 (2016) 161, arX¬≠iv:1606.03756.

Ző≥ pro¬≠duc¬≠tion

  • J.M. Camp¬≠bell, T. Neu¬≠mann, C. Williams, Ző≥ Pro¬≠duc¬≠tion at NNLO In¬≠clud¬≠ing Anom¬≠alous Cou¬≠plings, JHEP 11 (2017) 150, arX¬≠iv:1708.02925. Pub¬≠licly avail¬≠able since MCFM-8.1.
    This study has been used in the AT­LAS study in ref. [1] for a uni­fied SM and anom­alous cou­plings study at NN­LO.

Hig­gs+­jet pro­duc­tion

  • T. Neu¬≠mann, Nex¬≠t-¬≠to-lead¬≠ing or¬≠der Hig¬≠gs+¬≠jet pro¬≠duc¬≠tion at large trans¬≠verse mo¬≠menta in¬≠clud¬≠ing top quark mass ef¬≠fects, J. Phys. Comm. 2 (2018) 095017, arX¬≠iv:1802.02981.
    This study uses a high en­ergy as­ymp­totic ex­pan­sion of the two-loop vir­tual cor­rec­tions and com­bines them with pre­vi­ous re­sults. Re­sults are top-quark-­mass ac­cu­rate at low and high pT apart from the 2mt thresh­old re­gion. Pub­licly avail­able in MCFM-8.2.
  • T. Neu¬≠mann, C. Williams, The Higgs bo¬≠son at high pT, Phys. Rev.¬†D95 (2017) 014004, arX¬≠iv:1609.00367.
    Com¬≠pu¬≠ta¬≠tion of full top-quark-loop Hig¬≠gs+2¬≠jet am¬≠pli¬≠tudes in com¬≠bi¬≠na¬≠tion with low-en¬≠ergy as¬≠ymp¬≠totic ex¬≠pan¬≠sion of two-loop vir¬≠tual cor¬≠rec¬≠tions and im¬≠ple¬≠men¬≠ta¬≠tion in MCFM. Used in the CMS study for the search for boosted Higgs bosons to bŐĄb [2]. Pub¬≠licly avail¬≠able in MCFM-8.1.
  • T. Neu¬≠mann, M. Wiese¬≠mann, Fi¬≠nite top-¬≠mass ef¬≠fects in glu¬≠on-in¬≠duced Higgs pro¬≠duc¬≠tion with a jet-veto at NNLO, JHEP 11 (2014) 150, arX¬≠iv:1408.6836.
    We com­bine the pre­vi­ous re­sults with a NNLO cal­cu­la­tion of in­clu­sive Higgs pro­duc­tion.
  • R.V. Har¬≠lan¬≠der, T. Neu¬≠mann, Prob¬≠ing the na¬≠ture of the Hig¬≠gs-gluon cou¬≠pling, Phys. Rev.¬†D88 (2013) 074015, arX¬≠iv:1308.2225.
    Study on the im­pact of di­men­sion five and seven op­er­a­tors that mod­ify the Hig­gs-gluon cou­pling in Hig­gs+­jet pro­duc­tion.
  • R.V. Har¬≠lan¬≠der, T. Neu¬≠mann, K.J. Oz¬≠eren, M. Wiese¬≠mann, Top-¬≠mass ef¬≠fects in dif¬≠fer¬≠en¬≠tial Higgs pro¬≠duc¬≠tion through gluon fu¬≠sion at or¬≠der őĪs4, JHEP 08 (2012) 139, arX¬≠iv:1206.0157.
    This first study fo­cuses on a low en­ergy as­ymp­totic ex­pan­sion of the two-loop vir­tual cor­rec­tions.


  • T.Neu¬≠mann, Tools for per¬≠tur¬≠ba¬≠tive high¬≠-¬≠pre¬≠ci¬≠sion cal¬≠cu¬≠la¬≠tions, con¬≠tri¬≠bu¬≠tion to LHCP 2021, PoS LHCP2021 (2021) 295
  • T. Neu¬≠mann, Re¬≠cent De¬≠vel¬≠op¬≠ments in Gluon Fu¬≠sion Higgs Cal¬≠cu¬≠la¬≠tions, con¬≠tri¬≠bu¬≠tion to the 13th Con¬≠fer¬≠ence on the In¬≠ter¬≠sec¬≠tions of Par¬≠ti¬≠cle and Nu¬≠clear Physics (CI¬≠PANP 2018) Palm Springs, Cal¬≠i¬≠for¬≠nia, USA arX¬≠iv:1810.01800.
  • T. Neu¬≠mann, C. Williams, The Higgs bo¬≠son at high pT: Fi¬≠nite top-¬≠mass im¬≠proved re¬≠sults, PoS LL2016 (2016) 027



[1] M. Aaboud, oth¬≠ers, Mea¬≠sure¬≠ment of the Ző≥‚ÄĄ‚Üí‚ÄĄőĹőĹŐĄő≥ pro¬≠duc¬≠tion cross sec¬≠tion in pp col¬≠li¬≠sions at $\sqrt{s}=13$ TeV with the AT¬≠LAS de¬≠tec¬≠tor and lim¬≠its on anom¬≠alous triple gauge-¬≠bo¬≠son cou¬≠plings, JHEP. 12 (2018) 010, doi:10.1007/JHEP¬≠12(2018)010, http://arx¬≠¬≠s/1810.04995.

[2] A.M. Sirun­yan, oth­ers, In­clu­sive search for a highly boosted Higgs bo­son de­cay­ing to a bot­tom quark-an­ti­quark pair, Phys. Rev. Lett. 120 (2018) 071802, doi:10.1103/­Phys­RevLet­t.120.071802, http://arx­­s/1709.05543.