New herwig7 underlying event tune: From RHIC to LHC energies

We present parameter sets corresponding to new underlying event tunes for the erwig7.3 Monte Carlo event generator. The existing erwig tunes are in good agreement with LHC data, however, they are not typically designed for center-of-mass energies below <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msqrt> <a:mi>s</a:mi> </a:msqrt> <a:mo>=</a:mo> <a:mn>300</a:mn> <a:mtext> </a:mtext> <a:mtext> </a:mtext> <a:mi>GeV</a:mi> </a:math> . The tunes presented in this study can describe midrapidity data collected at the nominal RHIC energy of <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msqrt> <c:mi>s</c:mi> </c:msqrt> <c:mo>=</c:mo> <c:mn>200</c:mn> <c:mtext> </c:mtext> <c:mtext> </c:mtext> <c:mi>GeV</c:mi> </c:math> as well as higher center-of-mass energies utilized by experiments at the LHC and Tevatron. The base “New Haven” tune is developed by fitting minimum-bias simulations of proton-proton ( <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mi>p</e:mi> <e:mi>p</e:mi> </e:math> ) collisions to midrapidity identified hadron and jet data from the STAR experiment. The “Nashville” tune includes a separate set of parameters developed by tuning to Tevatron proton-antiproton ( <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mi>p</g:mi> <g:mover accent="true"> <g:mi>p</g:mi> <g:mo stretchy="false">¯</g:mo> </g:mover> </g:math> ) data at <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msqrt> <k:mi>s</k:mi> </k:msqrt> <k:mo>=</k:mo> <k:mn>300</k:mn> </k:math> , 900 and 1960 GeV from CDF, and LHC <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"> <m:mi>p</m:mi> <m:mi>p</m:mi> </m:math> measurements from CMS at <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"> <o:msqrt> <o:mi>s</o:mi> </o:msqrt> <o:mo>=</o:mo> <o:mn>7</o:mn> <o:mtext> </o:mtext> <o:mtext> </o:mtext> <o:mi>TeV</o:mi> </o:math> , in addition to the STAR measurements. Both new tunes demonstrate significant improvements over the recommended default tune currently included in the latest version of erwig for minimum bias production. As such, we advocate using these tunes for future simulation studies at midrapidity by experimental collaborations at RHIC (STAR and sPHENIX) and the LHC (ALICE, ATLAS, and CMS).

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Journal
Physical review. D/Physical review. D.
Published
2025-11-06
DOI
https://doi.org/10.1103/cnck-wtbh
Primary Topic
High-Energy Particle Collisions Research
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article
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article

New herwig7 underlying event tune: From RHIC to LHC energies

Karl J. Friston
Physical review. D/Physical review. D.
High-Energy Particle Collisions Research
article

New herwig7 underlying event tune: From RHIC to LHC energies

Karl J. Friston
article en

Abstract

We present parameter sets corresponding to new underlying event tunes for the erwig7.3 Monte Carlo event generator. The existing erwig tunes are in good agreement with LHC data, however, they are not typically designed for center-of-mass energies below <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msqrt> <a:mi>s</a:mi> </a:msqrt> <a:mo>=</a:mo> <a:mn>300</a:mn> <a:mtext> </a:mtext> <a:mtext> </a:mtext> <a:mi>GeV</a:mi> </a:math> . The tunes presented in this study can describe midrapidity data collected at the nominal RHIC energy of <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msqrt> <c:mi>s</c:mi> </c:msqrt> <c:mo>=</c:mo> <c:mn>200</c:mn> <c:mtext> </c:mtext> <c:mtext> </c:mtext> <c:mi>GeV</c:mi> </c:math> as well as higher center-of-mass energies utilized by experiments at the LHC and Tevatron. The base “New Haven” tune is developed by fitting minimum-bias simulations of proton-proton ( <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mi>p</e:mi> <e:mi>p</e:mi> </e:math> ) collisions to midrapidity identified hadron and jet data from the STAR experiment. The “Nashville” tune includes a separate set of parameters developed by tuning to Tevatron proton-antiproton ( <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mi>p</g:mi> <g:mover accent="true"> <g:mi>p</g:mi> <g:mo stretchy="false">¯</g:mo> </g:mover> </g:math> ) data at <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msqrt> <k:mi>s</k:mi> </k:msqrt> <k:mo>=</k:mo> <k:mn>300</k:mn> </k:math> , 900 and 1960 GeV from CDF, and LHC <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"> <m:mi>p</m:mi> <m:mi>p</m:mi> </m:math> measurements from CMS at <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"> <o:msqrt> <o:mi>s</o:mi> </o:msqrt> <o:mo>=</o:mo> <o:mn>7</o:mn> <o:mtext> </o:mtext> <o:mtext> </o:mtext> <o:mi>TeV</o:mi> </o:math> , in addition to the STAR measurements. Both new tunes demonstrate significant improvements over the recommended default tune currently included in the latest version of erwig for minimum bias production. As such, we advocate using these tunes for future simulation studies at midrapidity by experimental collaborations at RHIC (STAR and sPHENIX) and the LHC (ALICE, ATLAS, and CMS).

Physical review. D/Physical review. D.Vol. 112(11)
Vanderbilt University (US), Brookhaven National Laboratory (US), Yale University (US), Columbia University (US), Stanford University (US)
Openalex Percentile: Top 82%
High-Energy Particle Collisions Research
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