Name: Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV
Creator: LHCb Collaboration
Published: 2019

Abstract (data abstract)

CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections and ratios of cross-sections are measured as functions of the meson transverse momentum $p_T$ and rapidity $y$, for $p_T < 30$ GeV/$c$ and $2.0<y<4.5$. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode.

Table 1

Data from Fig2, (a); Table 2

10.17182/hepdata.82210.v1/t1

Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\Upsilon$(1S) (in pb). The first uncertainty...
Table 2

Data from Fig2, (b); Table 3

10.17182/hepdata.82210.v1/t2

Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\Upsilon$(2S) (in pb). The first uncertainty...
Table 3

Data from Fig2, (c); Table 4

10.17182/hepdata.82210.v1/t3

Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\Upsilon$(3S) (in pb). The first uncertainty...
Table 4

Data from Fig3 (top)

10.17182/hepdata.82210.v1/t4

Differential cross-sections multiplied by dimuon branching fractions for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) states versus $p_T$ integrated over $y$ between 2.0...
Table 5

Data from Fig3 (bottom)

10.17182/hepdata.82210.v1/t5

Differential cross-sections multiplied by dimuon branching fractions for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) states versus $y$ integrated over $p_T$ from 0...
Table 6

Data from Fig5, (a)

10.17182/hepdata.82210.v1/t6

Ratios of double-differential cross-sections times dimuon branching fractions for $\Upsilon$(2S) to $\Upsilon$(1S).
Table 7

Data from Fig5, (b)

10.17182/hepdata.82210.v1/t7

Ratios of double-differential cross-sections times dimuon branching fractions for $\Upsilon$(3S) to $\Upsilon$(1S).
Table 8

Data from Fig5, (c)

10.17182/hepdata.82210.v1/t8

Ratios of differential cross-sections times dimuon branching fractions versus $p_T$ over $y$ for $\Upsilon$(2S) to $\Upsilon$(1S) and $\Upsilon$(3S) to $\Upsilon$(1S).
Table 9

Data from Fig5, (d)

10.17182/hepdata.82210.v1/t9

Ratios of differential cross-sections times dimuon branching fractions versus $y$ over $p_T$ for $\Upsilon$(2S) to $\Upsilon$(1S) and $\Upsilon$(3S) to $\Upsilon$(1S).
Table 10

Data from Fig6, (a); Table 5

10.17182/hepdata.82210.v1/t10

The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\Upsilon$(1S).
Table 11

Data from Fig6, (b); Table 6

10.17182/hepdata.82210.v1/t11

The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\Upsilon$(2S).
Table 12

Data from Fig6, (c); Table 7

10.17182/hepdata.82210.v1/t12

The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\Upsilon$(3S).
Table 13

Data from Fig7 (top)

10.17182/hepdata.82210.v1/t13

Ratios of differential cross-sections between 13 TeV and 8 TeV measurements versus $p_T$ over $y$ for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S).
Table 14

Data from Fig7 (bottom)

10.17182/hepdata.82210.v1/t14

Ratios of differential cross-sections between 13 TeV and 8 TeV measurements versus $y$ over $p_T$ for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S).

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