| Average prompt D-meson, Jpsi and HFe self normalised yields vs relative charged-particle multiplicity at central rapidity in pp at 13 TeV (D mesons for 8 < pT < 12 GeV/c)
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| Average prompt D-meson, Jpsi and HFe self normalised yields vs relative charged-particle multiplicity at central rapidity in pp at 13 TeV (D mesons for 2 < pT < 4 GeV/c)
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| Comparison of data with models: Average D-meson double ratios vs charged-particle multiplicity in pp 13 TeV
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| Average D-meson double ratios vs relative charged-particle multiplicity in pp at 13 TeV
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| Comparison of data with models: Average D-meson self normalised yields vs charged-particle multiplicity in pp 13 TeV
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| Comparison of average D-meson self nomalised yields vs relative charged-particle multiplicity in pp 13 TeV with pp 7 TeV
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| Average D-meson self normalised yields vs relative charged-particle multiplicity in pp at 13 TeV
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K0s-Antip correlation function Kyoto + AJ 1 model
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-p + K0s-Antip correlation function Kyoto + AJ 1 model
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-p + K0s-Antip correlation function Kyoto + AJ 2 model
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-Antip correlation function Kyoto + AJ 2 model
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-p correlation function Kyoto + AJ 2 model
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-p correlation function Kyoto + AJ 1 model
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-Antip correlation function Lednicky
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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K0s-p correlation function Lednicky
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System p-p
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| Cross section ratio for e+ <- W+ and e- <-W- as a function of pT in mid rapidity in pp collisions at 13 TeV
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| Cross section for e- <- W- in 30<pT,e<60 GeV/c in mid rapidity in pp collisions at 13 TeV
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| Cross section for e+ <- W+ in 30<pT,e<60 GeV/c in mid rapidity in pp collisions at 13 TeV
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| pT differential cross section for e- <- W- in mid-rapidity in pp collisions at 13 TeV
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| pT differential cross section for e+ <- W+ in mid-rapidity in pp collisions at 13 TeV
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the percentile estimator
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity as a function of the percentile estimator
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the percentile estimator
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity as a function of the percentile estimator
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the charged particle multiplicity at midrapidity
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity as a function of the charged particle multiplicity at midrapidity
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity self-normalised to INEL>0 as a function of the charged particle multiplicity at midrapidity
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity as a function of the particle multiplicity
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| Ratio $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields to multiplicity (self-normalised to INEL>0) as a function of the percentile selection
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| Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields to multiplicity (self-normalised to INEL>0) as a function of the average charged particle multiplicity
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| $\Xi^{-}$ + $\bar{\Xi}^{+}$ $p_{\text{T}}$-spectra in ($\sqrt{s}$ - ZDC) and V0M classes in pp collisions at $\sqrt{s}$ = 13 TeV
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| Nuclear modification factor of $\pi^0$ meson and charged hadron spectra in p-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ and $8.16$ TeV and in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ TeV
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| 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
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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 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
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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 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
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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 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 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 $\sqrt{s} = 7\;\text{TeV}$
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from pp collisions at $\sqrt{s} = 7\;\text{TeV}$
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| Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
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| Azimuthal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
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| Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projections of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from p--Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
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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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| 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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
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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 $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$
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