Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV

The ALICE collaboration
CERN-EP-2023-264, 2023.

Abstract (data abstract)
The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| < 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.

  • Figure 1 (top)

    Data from Figure 1 (top)

    10.17182/hepdata.153919.v1/t1

    Mean number of charged particles ($\langle N_{\mathrm{ch}} \rangle$) within leading charged-particle jets as a function of $p_{T}^{\mathrm{jet, ch}}$ for minimum-bias...

  • Figure 1 (bottom)

    Data from Figure 1 (bottom)

    10.17182/hepdata.153919.v1/t2

    Mean number of charged particles ($\langle N_{\mathrm{ch}} \rangle$) within leading charged-particle jets as a function of $p_{T}^{\mathrm{jet, ch}}$ for high-multiplicity...

  • Figure 2

    Data from Figure 2

    10.17182/hepdata.153919.v1/t3

    The ratio of $\langle N_{\mathrm{ch}} \rangle$ between high-multiplicity (HM) and minimum-bias (MB) events as a function of $p_{T}^{\mathrm{jet, ch}}$ for...

  • Figure 3 (top left)

    Data from Figure 3 (top left)

    10.17182/hepdata.153919.v1/t4

    $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$)...

  • Figure 3 (top middle)

    Data from Figure 3 (top middle)

    10.17182/hepdata.153919.v1/t5

    $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$)...

  • Figure 3 (top right)

    Data from Figure 3 (top right)

    10.17182/hepdata.153919.v1/t6

    $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$)...

  • Figure 3 (bottom left)

    Data from Figure 3 (bottom left)

    10.17182/hepdata.153919.v1/t7

    $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in high-multiplicity (HM) pp collisions for jet resolution parameter ($R$)...

  • Figure 3 (bottom middle)

    Data from Figure 3 (bottom middle)

    10.17182/hepdata.153919.v1/t8

    $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in high-multiplicity (HM) pp collisions for jet resolution parameter ($R$)...

  • Figure 3 (bottom right)

    Data from Figure 3 (bottom right)

    10.17182/hepdata.153919.v1/t9

    $z^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in high-multiplicity (HM) pp collisions for jet resolution parameter ($R$)...

  • Figure 5 (top)

    Data from Figure 5 (top)

    10.17182/hepdata.153919.v1/t10

    The ratio of $z^{\mathrm{ch}}$ distributions for $10 < p_{\mathrm{T}}^{\mathrm{jet, ch}} < 20$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events...

  • Figure 5 (middle)

    Data from Figure 5 (middle)

    10.17182/hepdata.153919.v1/t11

    The ratio of $z^{\mathrm{ch}}$ distributions for $30 < p_{\mathrm{T}}^{\mathrm{jet, ch}} < 40$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events...

  • Figure 5 (bottom)

    Data from Figure 5 (bottom)

    10.17182/hepdata.153919.v1/t12

    The ratio of $z^{\mathrm{ch}}$ distributions for $60 < p_{\mathrm{T}}^{\mathrm{jet, ch}} < 80$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events...

  • Figure 7 (top left)

    Data from Figure 7 (top left)

    10.17182/hepdata.153919.v1/t13

    $\xi^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$)...

  • Figure 7 (top middle)

    Data from Figure 7 (top middle)

    10.17182/hepdata.153919.v1/t14

    $\xi^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$)...

  • Figure 7 (top right)

    Data from Figure 7 (top right)

    10.17182/hepdata.153919.v1/t15

    $\xi^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in minimum-bias (MB) pp collisions for jet resolution parameter ($R$)...

  • Figure 7 (bottom left)

    Data from Figure 7 (bottom left)

    10.17182/hepdata.153919.v1/t16

    $\xi^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in high-multiplicity (HM) pp collisions for jet resolution parameter ($R$)...

  • Figure 7 (bottom middle)

    Data from Figure 7 (bottom middle)

    10.17182/hepdata.153919.v1/t17

    $\xi^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in high-multiplicity (HM) pp collisions for jet resolution parameter ($R$)...

  • Figure 7 (bottom right)

    Data from Figure 7 (bottom right)

    10.17182/hepdata.153919.v1/t18

    $\xi^{\mathrm{ch}}$ distributions in leading jets for different $p_{T}^{\mathrm{jet, ch}}$ intervals in high-multiplicity (HM) pp collisions for jet resolution parameter ($R$)...

  • Figure 9 (top)

    Data from Figure 9 (top)

    10.17182/hepdata.153919.v1/t19

    The ratio of $\xi^{\mathrm{ch}}$ distributions for $10 < p_{\mathrm{T}}^{\mathrm{jet, ch}} < 20$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events...

  • Figure 9 (middle)

    Data from Figure 9 (middle)

    10.17182/hepdata.153919.v1/t20

    The ratio of $\xi^{\mathrm{ch}}$ distributions for $30 < p_{\mathrm{T}}^{\mathrm{jet, ch}} < 40$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events...

  • Figure 9 (bottom)

    Data from Figure 9 (bottom)

    10.17182/hepdata.153919.v1/t21

    The ratio of $\xi^{\mathrm{ch}}$ distributions for $60 < p_{\mathrm{T}}^{\mathrm{jet, ch}} < 80$ GeV/c between high-multiplicity (HM) and minimum-bias (MB) events...

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