CMS-GEN-22-001 ; CERN-EP-2024-216 | ||
Energy-scaling behavior of intrinsic transverse momentum parameters in Drell-Yan simulation | ||
CMS Collaboration | ||
26 September 2024 | ||
Submitted to Phys. Rev. Lett. | ||
Abstract: We present an analysis based on models of the intrinsic transverse momentum of partons in nucleons by studying the dilepton transverse momentum in Drell-Yan events. Using parameter tuning in event generators and existing data from fixed-target experiments, from the Tevatron, and from the LHC, our investigation spans three orders of magnitude in center-of-mass energy and two orders of magnitude in dilepton invariant mass. The results show an energy-scaling behavior of the intrinsic transverse momentum parameters, independent of the dilepton invariant mass at a given center-of-mass energy. | ||
Links: e-print arXiv:2409.17770 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; CADI line (restricted) ; |
Figures | |
png pdf |
Figure 1:
Tuned parameter $ q $ values for DY measurements at different center-of-mass energies (points) for various PYTHIA and HERWIG setups (colors). The error bars on the points represent the tuning uncertainties. The tuned values are given in Appendix. For each generator setup, the function $ b \sqrt{s}^a $ is fitted to the points and shown as a line, assuming the same slope $ a $ for all the settings. The $ \chi^2_{\text{lin.}}/\text{NDF} $ and $ p $-value of the combined linear fit is given in the plot. The uncertainty in each fit is shown as a colored band and corresponds to the up and down variations of the fit parameters, propagated from the tune uncertainties. The CASCADE predictions (CAS3) [2,3] are also fitted separately with the function $ b \sqrt{s}^a $ for comparison with PYTHIA and HERWIG. |
png pdf |
Figure 2:
Tuned parameter $ q $ values for DY measurements at different center-of-mass energies (points) for various generator settings (lines and bands). The error bars on the points represent the tuning uncertainties. The tuned values are given in Appendix. For the PYTHIA CP5 setup, the parameter SPACESHOWER:PT0REF is set to 1 GeV (orange dashed) or its default value of 2 GeV (blue solid). For the HERWIG CH3 setup, the parameter SUDAKOVCOMMON:PTMIN is set to 0.7 GeV (green dotted) or its default value of 1.22 GeV (purple dash-dotted). The function $ b \sqrt{s}^a $ is fitted to the points of each generator setting and shown as a line, allowing free-floating slopes $ a $ and offsets $ \log_{10}(b) $. The uncertainty in each fit is shown as a colored band and corresponds to the up and down variations of the fit parameters, propagated from the tune uncertainties. |
png pdf |
Figure 3:
Tuned parameter values (points) for DY measurements at four different center-of-mass energies (panels) for the PYTHIA CP5 (blue) and HERWIG CH3 (green) setups. The error bars on the points represent the tuning uncertainties. The tuned values are given in Appendix. For each generator setup, a constant is fitted to the points and shown as a line. The uncertainty in each fit, propagated from the tune uncertainties, is shown as a colored band. |
png pdf |
Figure A1:
Effects of the variation of the UE parameters on the DY $ p_{\mathrm{T}}(\ell^+\ell^-) $ spectrum (upper), and of the variation of the intrinsic $ k_{\mathrm{T}} $ parameter on the density of the scalar sum of the charged-particle transverse momenta ($ p_{\mathrm{T}}^{\text{sum}} $) on the rapidity ($ \eta $) - azimuthal angle ($ \phi $) space as a function of the transverse momentum of the leading charged particle ($ p_{\mathrm{T}}^{\text{max}} $) in the transMAX region averaged over $ N_\text{events} $ generated events [28] in the minimum bias (MB) process (lower), which is one of the observables used for UE tuning. For each event, the transMAX region is defined by the direction of the leading charged particle in the space transverse to the proton beams. Assuming $ \phi $ as the azimuthal angle of the leading charged particle, the ranges of $ \phi_1 $ satisfying $ 60^{\circ} < |\phi-\phi_1| < 120^{\circ} $ define the two transverse regions, in which transMAX is the one with a higher activity. The red and violet shaded areas represent the predictions from the up and down variations of the UE tune and the intrinsic $ k_{\mathrm{T}} $ tune, respectively. In the upper distribution, both shaded areas are based on the prediction of tuned intrinsic $ k_{\mathrm{T}} $ parameter on top of PYTHIA CP5 (``int.$ k_{\mathrm{T}} $ tune''). In the lower distribution, the red shaded area is based on the prediction of the intrinsic $ k_{\mathrm{T}} $ parameter set to the default 1.8 and the UE tune set to PYTHIA CP5 (``Default int.$ k_{\mathrm{T}} $''), while the violet shaded area is based on the ``int.$ k_{\mathrm{T}} $ tune'' prediction. The error bars represent the statistical uncertainty in the simulated events. The upper distribution also includes the UE prediction of the combined tune of the intrinsic $ k_{\mathrm{T}} $ and the ISR cutoff scale to the DY $ p_{\mathrm{T}}(\ell^+\ell^-) $ distribution (``int.$ k_{\mathrm{T}} $+ISR $ p_{\text{T0Ref}} $ tune''). |
png pdf |
Figure A1-a:
Effects of the variation of the UE parameters on the DY $ p_{\mathrm{T}}(\ell^+\ell^-) $ spectrum (upper), and of the variation of the intrinsic $ k_{\mathrm{T}} $ parameter on the density of the scalar sum of the charged-particle transverse momenta ($ p_{\mathrm{T}}^{\text{sum}} $) on the rapidity ($ \eta $) - azimuthal angle ($ \phi $) space as a function of the transverse momentum of the leading charged particle ($ p_{\mathrm{T}}^{\text{max}} $) in the transMAX region averaged over $ N_\text{events} $ generated events [28] in the minimum bias (MB) process (lower), which is one of the observables used for UE tuning. For each event, the transMAX region is defined by the direction of the leading charged particle in the space transverse to the proton beams. Assuming $ \phi $ as the azimuthal angle of the leading charged particle, the ranges of $ \phi_1 $ satisfying $ 60^{\circ} < |\phi-\phi_1| < 120^{\circ} $ define the two transverse regions, in which transMAX is the one with a higher activity. The red and violet shaded areas represent the predictions from the up and down variations of the UE tune and the intrinsic $ k_{\mathrm{T}} $ tune, respectively. In the upper distribution, both shaded areas are based on the prediction of tuned intrinsic $ k_{\mathrm{T}} $ parameter on top of PYTHIA CP5 (``int.$ k_{\mathrm{T}} $ tune''). In the lower distribution, the red shaded area is based on the prediction of the intrinsic $ k_{\mathrm{T}} $ parameter set to the default 1.8 and the UE tune set to PYTHIA CP5 (``Default int.$ k_{\mathrm{T}} $''), while the violet shaded area is based on the ``int.$ k_{\mathrm{T}} $ tune'' prediction. The error bars represent the statistical uncertainty in the simulated events. The upper distribution also includes the UE prediction of the combined tune of the intrinsic $ k_{\mathrm{T}} $ and the ISR cutoff scale to the DY $ p_{\mathrm{T}}(\ell^+\ell^-) $ distribution (``int.$ k_{\mathrm{T}} $+ISR $ p_{\text{T0Ref}} $ tune''). |
png pdf |
Figure A1-b:
Effects of the variation of the UE parameters on the DY $ p_{\mathrm{T}}(\ell^+\ell^-) $ spectrum (upper), and of the variation of the intrinsic $ k_{\mathrm{T}} $ parameter on the density of the scalar sum of the charged-particle transverse momenta ($ p_{\mathrm{T}}^{\text{sum}} $) on the rapidity ($ \eta $) - azimuthal angle ($ \phi $) space as a function of the transverse momentum of the leading charged particle ($ p_{\mathrm{T}}^{\text{max}} $) in the transMAX region averaged over $ N_\text{events} $ generated events [28] in the minimum bias (MB) process (lower), which is one of the observables used for UE tuning. For each event, the transMAX region is defined by the direction of the leading charged particle in the space transverse to the proton beams. Assuming $ \phi $ as the azimuthal angle of the leading charged particle, the ranges of $ \phi_1 $ satisfying $ 60^{\circ} < |\phi-\phi_1| < 120^{\circ} $ define the two transverse regions, in which transMAX is the one with a higher activity. The red and violet shaded areas represent the predictions from the up and down variations of the UE tune and the intrinsic $ k_{\mathrm{T}} $ tune, respectively. In the upper distribution, both shaded areas are based on the prediction of tuned intrinsic $ k_{\mathrm{T}} $ parameter on top of PYTHIA CP5 (``int.$ k_{\mathrm{T}} $ tune''). In the lower distribution, the red shaded area is based on the prediction of the intrinsic $ k_{\mathrm{T}} $ parameter set to the default 1.8 and the UE tune set to PYTHIA CP5 (``Default int.$ k_{\mathrm{T}} $''), while the violet shaded area is based on the ``int.$ k_{\mathrm{T}} $ tune'' prediction. The error bars represent the statistical uncertainty in the simulated events. The upper distribution also includes the UE prediction of the combined tune of the intrinsic $ k_{\mathrm{T}} $ and the ISR cutoff scale to the DY $ p_{\mathrm{T}}(\ell^+\ell^-) $ distribution (``int.$ k_{\mathrm{T}} $+ISR $ p_{\text{T0Ref}} $ tune''). |
Tables | |
png pdf |
Table 1:
Measurements of the Drell-Yan differential cross section as a function of $ p_{\mathrm{T}}(\ell^+\ell^-) $ at various center-of-mass energies $ \sqrt{s} $ from different hadron-collision processes used as inputs for the intrinsic $ k_{\mathrm{T}} $ tunes. The $ \sqrt{s} $ in $ \mathrm{p}\mathrm{Pb} $ collisions represents the nucleon-nucleon center-of-mass energy. The variable $ Q $ represents the energy scale of the hard scattering, approximated by the dilepton invariant mass. The Z boson mass is denoted as $ m(\mathrm{Z}) $. |
png pdf |
Table B1:
Tune results for the BEAMREMNANTS:PRIMORDIALKTHARD parameter in PYTHIA 8 and the SHOWERHANDLER:INTRINSICPTGAUSSIAN parameter in HERWIG 7, taking into account the uncertainty from tune ranges (range) and the functions for interpolation (int.). |
png pdf |
Table B2:
Tune results for the BEAMREMNANTS:PRIMORDIALKTHARD parameter in PYTHIA8 with the CP5 tune setup. The parameter SPACESHOWER:PT0REF was set to 1 GeV. |
png pdf |
Table B3:
Tune results for the SHOWERHANDLER:INTRINSICPTGAUSSIAN parameter in HERWIG 7 with the CH3 tune setup. The parameter SUDAKOVCOMMON:PTMIN was set to 0.7 GeV. |
png pdf |
Table B4:
Results of the tune to various ranges of the $ m(\ell^+\ell^-) $ for values of $ \sqrt{s} $ of 38.8 GeV and 8, 8.16, and 13 TeV. |
Summary |
In summary, the study assesses the mutual impacts of the variation of the intrinsic $ k_{\mathrm{T}}$ tune on the UE, and that of the UE tune on the DY transverse momentum, and concludes that the impacts are negligible, which supports our approach of tuning the intrinsic $ k_{\mathrm{T}}$ parameters with fixed UE parameters. |
References | ||||
1 | A. Bermudez Martinez et al. | The transverse momentum spectrum of low mass Drell-Yan production at next-to-leading order in the parton branching method | EPJC 80 (2020) 598 | 2001.06488 |
2 | I. Bubanja et al. | The small $ k_{\textrm{T}} $ region in Drell-Yan production at next-to-leading order with the parton branching method | EPJC 84 (2024) 154 | 2312.08655 |
3 | M. Mendizabal, F. Guzman, H. Jung, and S. Taheri Monfared | On the role of soft gluons in collinear parton densities and parton shower event generators | 2309.11802 | |
4 | P. Hägler, B. U. Musch, J. W. Negele, and A. Schäfer | Intrinsic quark transverse momentum in the nucleon from lattice QCD | Euro. Phys. Lett. 88 (2009) 61001 | 0908.1283 |
5 | B. U. Musch et al. | Transverse-momentum distribution of quarks in the nucleon from lattice QCD | in Proceedings of LIGHT CONE 2008 Relativistic Nuclear and Particle Physics, 2008 link |
|
6 | B. U. Musch, P. Hägler, J. W. Negele, and A. Schäfer | Exploring quark transverse momentum distributions with lattice QCD | PRD 83 (2011) 094507 | 1011.1213 |
7 | C. Bierlich et al. | A comprehensive guide to the physics and usage of PYTHIA 8.3 | SciPost Phys. Codeb. 2022 (2022) 8 | 2203.11601 |
8 | T. Sjöstrand and P. Z. Skands | Multiple interactions and the structure of beam remnants | JHEP 03 (2004) 053 | hep-ph/0402078 |
9 | J. Bellm et al. | Herwig 7.0/Herwig++ 3.0 release note | EPJC 76 (2016) 196 | 1512.01178 |
10 | Sherpa Collaboration | Event generation with Sherpa 2.2 | SciPost Phys. 7 (2019) 034 | 1905.09127 |
11 | NuSea Collaboration | Absolute Drell-Yan dimuon cross-sections in 800 GeV/$ c $ pp and pd collisions | hep-ex/0302019 | |
12 | J. C. Webb | Measurement of continuum dimuon production in 800-GeV/$ c $ proton nucleon collisions | PhD thesis, New Mexico State U, 2003 link |
hep-ex/0301031 |
13 | D. Antreasyan et al. | Dimuon scaling comparison at 44 GeV and 62 GeV | PRL 48 (1982) 302 | |
14 | PHENIX Collaboration | Measurements of $ \mu\mu $ pairs from open heavy flavor and Drell-Yan in $ \text{p}+\text{p} $ collisions at $ \sqrt{s}= $ 200 GeV | PRD 99 (2019) 072003 | 1805.02448 |
15 | D0 Collaboration | Measurement of the inclusive differential cross section for Z bosons as a function of transverse momentum in $ \overline{\text{p}}\text{p} $ collisions at $ \sqrt{s}= $ 1.8 TeV | PRD 61 (2000) 032004 | hep-ex/9907009 |
16 | CDF Collaboration | The transverse momentum and total cross section of $ \text{e}^+\text{e}^- $ pairs in the Z boson region from $ \text{p}\overline{\text{p}} $ collisions at $ \sqrt{s}= $ 1.8 TeV | PRL 84 (2000) 845 | hep-ex/0001021 |
17 | D0 Collaboration | Measurement of the normalized Z/$ \gamma^* \rightarrow \mu^+\mu^- $ transverse momentum distribution in $ \text{p}\overline{\text{p}} $ collisions at $ \sqrt{s}= $ 1.96 TeV | PLB 693 (2010) 522 | 1006.0618 |
18 | CDF Collaboration | Transverse momentum cross section of $ \text{e}^+\text{e}^- $ pairs in the Z-boson region from $ \text{p}\overline{\text{p}} $ collisions at $ \sqrt{s}= $ 1.96 TeV | PRD 86 (2012) 052010 | 1207.7138 |
19 | CMS Collaboration | Study of Z production in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}= $ 2.76 TeV in the dimuon and dielectron decay channels | JHEP 03 (2015) 022 | CMS-HIN-13-004 1410.4825 |
20 | ATLAS Collaboration | Measurement of the transverse momentum and $ \phi^*_{\eta} $ distributions of Drell-Yan lepton pairs in proton-proton collisions at $ \sqrt{s}= $ 8 TeV with the ATLAS detector | EPJC 76 (2016) 291 | 1512.02192 |
21 | CMS Collaboration | Study of Drell-Yan dimuon production in proton-lead collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}} = $ 8.16 TeV | JHEP 05 (2021) 182 | CMS-HIN-18-003 2102.13648 |
22 | CMS Collaboration | Measurement of the mass dependence of the transverse momentum of lepton pairs in Drell-Yan production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | EPJC 83 (2023) 628 | CMS-SMP-20-003 2205.04897 |
23 | LHCb Collaboration | Precision measurement of forward Z boson production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JHEP 07 (2022) 026 | 2112.07458 |
24 | C. T. H. Davies, B. R. Webber, and W. J. Stirling | Drell-Yan cross-sections at small transverse momentum | NPB 256 (1985) 413 | |
25 | M. Guzzi, P. M. Nadolsky, and B. Wang | Nonperturbative contributions to a resummed leptonic angular distribution in inclusive neutral vector boson production | PRD 90 (2014) 014030 | 1309.1393 |
26 | S.-Y. Wei | Exploring the non-perturbative Sudakov factor via $ \text{Z}^0 $-boson production in pp collisions | PLB 817 (2021) 136356 | 2009.06514 |
27 | S. Baranov et al. | CASCADE3 a Monte Carlo event generator based on TMDs | EPJC 81 (2021) 425 | 2101.10221 |
28 | CMS Collaboration | Underlying event measurements with leading particles and jets in pp collisions at $ \sqrt{s}= $ 13 TeV | CMS Physics Analysis Summary, 2015 link |
CMS-PAS-FSQ-15-007 |
29 | CMS Collaboration | Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements | EPJC 80 (2020) 4 | CMS-GEN-17-001 1903.12179 |
30 | CMS Collaboration | Development and validation of HERWIG 7 tunes from CMS underlying-event measurements | EPJC 81 (2021) 312 | CMS-GEN-19-001 2011.03422 |
31 | CMS Collaboration | HEPData record for this analysis | link | |
32 | J. Alwall et al. | The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations | JHEP 07 (2014) 079 | 1405.0301 |
33 | CMS Collaboration | Placeholder for journal reference to appendices | ||
34 | A. Buckley et al. | Systematic event generator tuning for the LHC | EPJC 65 (2010) 331 | 0907.2973 |
35 | E. Gross and O. Vitells | Trial factors for the look elsewhere effect in high energy physics | EPJC 70 (2010) 525 | 1005.1891 |
36 | C. Balázs and C.-P. Yuan | Soft gluon effects on lepton pairs at hadron colliders | PRD 56 (1997) 5558 | hep-ph/9704258 |
Compact Muon Solenoid LHC, CERN |