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Differential Cross-section of High Mass Muon Pairs Produced by a 194-{GeV}/$c \pi^-$ Beam on a Tungsten Target

The collaboration
Z.Phys. C28 (1985) 9, 1985

Abstract (data abstract)
PLAB=194 GEV/C. DATA FROM NA10 COLLABORATION AT CERN. MASS OF MUON PAIRS & gt; 4.07 GEV. UPDATE (04 DEC 2018): Added Tables 11-19 (194 GeV) and Tables 20-30 (286 GeV) containing re-analysed data by the NA10 experimenters using a better estimate of Fermi motion effects. These re-analysed data were obtained by private communication and previously published in W.J. Stirling and M.R. Whalley, "A compilation of Drell-Yan cross sections", J.Phys. G19 (1993) D1-D102 (https://doi.org/10.1088/0954-3899/19/D/001); numbers taken from http://hepdata.cedar.ac.uk/review/dy/na10.shtml . Thanks to Ivan Novikov for pointing out the omission from HEPData of these re-analysed data.

• #### Table 1

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t1

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 2

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t2

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 3

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t3

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 4

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t4

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 5

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t5

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 6

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t6

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 7

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t7

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 8

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t8

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 9

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t9

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 10

Data from Table 2 of paper

10.17182/hepdata.15988.v2/t10

The cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ integrated over each $\sqrt{\tau}$-$x_F$ cell as a function of $x_F$ for $\sqrt{\tau}$ =...

• #### Table 11

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t11

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.21-0.24 interval for...

• #### Table 12

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t12

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.24-0.27 interval for...

• #### Table 13

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t13

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.27-0.30 interval for...

• #### Table 14

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t14

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.30-0.33 interval for...

• #### Table 15

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t15

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.33-0.36 interval for...

• #### Table 16

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t16

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.36-0.39 interval for...

• #### Table 17

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t17

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.39-0.42 interval for...

• #### Table 18

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t18

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.54-0.63 interval for...

• #### Table 19

Data from Table 21 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t19

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.63-0.72 interval for...

• #### Table 20

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t20

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.18-0.21 interval for...

• #### Table 21

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t21

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.21-0.24 interval for...

• #### Table 22

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t22

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.24-0.27 interval for...

• #### Table 23

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t23

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.27-0.30 interval for...

• #### Table 24

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t24

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.30-0.33 interval for...

• #### Table 25

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t25

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.33-0.36 interval for...

• #### Table 26

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t26

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.45-0.48 interval for...

• #### Table 27

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t27

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.48-0.51 interval for...

• #### Table 28

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t28

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.51-0.54 interval for...

• #### Table 29

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t29

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.54-0.63 interval for...

• #### Table 30

Data from Table 22 of J.Phys. G19 (1993) D1-D102

10.17182/hepdata.15988.v2/t30

The differential cross section ${\rm d}^2\sigma/{\rm d}\sqrt{\tau}{\rm d}x$ as a function of $x$ in the $\sqrt{\tau}$ = 0.63-0.72 interval for...

Version 2 modifications: Added Tables 11-19 (194 GeV) and Tables 20-30 (286 GeV) containing re-analysed data by the NA10 experimenters using a better estimate of Fermi motion effects. Thanks to Ivan Novikov for pointing out the omission from HEPData of these re-analysed data.