| Lund plane density unfolded/raw distribution
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| The unfolded Lund plane in pp collisions
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| Momentum splitting scale projection ln(kT) for narrow angle splittings
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| Momentum splitting scale projection ln(kT) for wide angle splittings
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| Momentum splitting scale projection ln(kT)
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| Angular splitting scale projection ln(R/dR) for mostly perturbative splittings
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| Angular splitting scale projection ln(R/dR) for mostly non-perturbative splittings
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| Angular splitting scale projection ln(R/dR)
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| Efficiency, purity, and subjet matching purity for the momentum splitting scale ln(kT)
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| Efficiency, purity, and subjet matching purity for the angular splitting scale ln(R/dR)
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| Response in momentum splitting scale ln(kt)
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| Response in angular scale ln(R/dR)
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| Near-side and away-side jet fragments as a function of multiplicity class with the Pythia8 description.
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| Near-side jet fragments as a function of multiplicity class with model descriptions
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| Near-side $\Delta\eta$ projections for various transverse momentum ranges in high-multiplicity and minimum bias pp collisions at 13 TeV with model descriptions,
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| v3 as a function of event-scale selection in high-multiplicity(0--0.1%) pp collisions at 13 TeV using template fit
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| v2 as a function of event-scale selection in high-multiplicity(0--0.1%) pp collisions at 13 TeV using template fit
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| v2 and v3 as a function of transverse momentum in high-multiplicity(0--0.1%) pp collisions at 13 TeV using template fit
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| Flow extraction using the template fit in high-multiplicity(0--0.1%) pp collisions at 13 TeV for 1$~<p_{\rm{T}}<~$2 GeV/$c$
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| Centrality dependence of the flow angle and magnitude fluctuations from v2{2}/v2[2]
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| Lower and upper limits of flow angle and flow magnitude fluctuations of v2{2}/v2[2] with etagap > 0.0 in centralities 0-5%, 10-20% and 30-40%
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| Lower and upper limits of flow angle and flow magnitude fluctuations of v2{2}/v2[2] with etagap > 0.0 in centralities 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%
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| <v2(pt)^2 v2^2>/<v2(pt)^2><v2^2> with etagap > 0.0 in centralities 0-5%, 10-20% and 30-40%
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| <v2(pt)^2 v2^2>/<v2(pt)^2><v2^2> with etagap > 0.0 in centralities 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%
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| F(Psi_2^a,\Psi_2) with etagap > 0.0 in centralities 0-5%, 10-20% and 30-40%
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| F(Psi_2^a,\Psi_2) with etagap > 0.0 in centralities 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%
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| Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
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| Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
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| Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
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| Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$ compared to models
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|
| Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
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| Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
|
|
| Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
|
|
| Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
|
|
| Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
|
|
| Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
|
|
| Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
|
|
| Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
|
|
| Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb 70--80% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb 30--40% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb 0--5% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb 70--80% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb 30--40% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
|
|
| Two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb 0--5% multiplicity class collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
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|
