Table 1
Figure 8a
10.17182/hepdata.141286.v1/t1
Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-0 monopoles production as...
Figure 8a
10.17182/hepdata.141286.v1/t1
Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-0 monopoles production as...
Figure 8b
10.17182/hepdata.141286.v1/t2
Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-1/2 monopoles production as...
Figure 8c
10.17182/hepdata.141286.v1/t3
Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-0 monopoles as...
Figure 8d
10.17182/hepdata.141286.v1/t4
Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-1/2 monopoles as...
Figure 9a
10.17182/hepdata.141286.v1/t5
Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-0 HECOs production as...
Figure 9b
10.17182/hepdata.141286.v1/t6
Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-1/2 HECOs production as...
Figure 9c
10.17182/hepdata.141286.v1/t7
Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-0 HECOs as...
Figure 9d
10.17182/hepdata.141286.v1/t8
Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-1/2 HECOs as...
Data from Figure 1a of auxiliary material
10.17182/hepdata.141286.v1/t9
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 200 GeV.
Data from Figure 1b of auxiliary material
10.17182/hepdata.141286.v1/t10
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 500 GeV.
Data from Figure 1c of auxiliary material
10.17182/hepdata.141286.v1/t11
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 1000 GeV.
Data from Figure 1d of auxiliary material
10.17182/hepdata.141286.v1/t12
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 1500 GeV.
Data from Figure 1e of auxiliary material
10.17182/hepdata.141286.v1/t13
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 2000 GeV.
Data from Figure 1f of auxiliary material
10.17182/hepdata.141286.v1/t14
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 2500 GeV.
Data from Figure 1g of auxiliary material
10.17182/hepdata.141286.v1/t15
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 3000 GeV.
Data from Figure 1h of auxiliary material
10.17182/hepdata.141286.v1/t16
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=1g_\textrm{D}$ monopoles of mass 4000 GeV.
Data from Figure 2a of auxiliary material
10.17182/hepdata.141286.v1/t17
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 200 GeV.
Data from Figure 2b of auxiliary material
10.17182/hepdata.141286.v1/t18
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 500 GeV.
Data from Figure 2c of auxiliary material
10.17182/hepdata.141286.v1/t19
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 1000 GeV.
Data from Figure 2d of auxiliary material
10.17182/hepdata.141286.v1/t20
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 1500 GeV.
Data from Figure 2e of auxiliary material
10.17182/hepdata.141286.v1/t21
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 2000 GeV.
Data from Figure 2f of auxiliary material
10.17182/hepdata.141286.v1/t22
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 2500 GeV.
Data from Figure 2g of auxiliary material
10.17182/hepdata.141286.v1/t23
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 3000 GeV.
Data from Figure 2h of auxiliary material
10.17182/hepdata.141286.v1/t24
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 4000 GeV.
Data from Figure 3a of auxiliary material
10.17182/hepdata.141286.v1/t25
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3b of auxiliary material
10.17182/hepdata.141286.v1/t26
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3c of auxiliary material
10.17182/hepdata.141286.v1/t27
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3d of auxiliary material
10.17182/hepdata.141286.v1/t28
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3e of auxiliary material
10.17182/hepdata.141286.v1/t29
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3f of auxiliary material
10.17182/hepdata.141286.v1/t30
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3g of auxiliary material
10.17182/hepdata.141286.v1/t31
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 3h of auxiliary material
10.17182/hepdata.141286.v1/t32
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=20$ of mass...
Data from Figure 4a of auxiliary material
10.17182/hepdata.141286.v1/t33
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4b of auxiliary material
10.17182/hepdata.141286.v1/t34
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4c of auxiliary material
10.17182/hepdata.141286.v1/t35
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4d of auxiliary material
10.17182/hepdata.141286.v1/t36
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4e of auxiliary material
10.17182/hepdata.141286.v1/t37
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4f of auxiliary material
10.17182/hepdata.141286.v1/t38
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4g of auxiliary material
10.17182/hepdata.141286.v1/t39
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 4h of auxiliary material
10.17182/hepdata.141286.v1/t40
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=40$ of mass...
Data from Figure 5a of auxiliary material
10.17182/hepdata.141286.v1/t41
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5b of auxiliary material
10.17182/hepdata.141286.v1/t42
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5c of auxiliary material
10.17182/hepdata.141286.v1/t43
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5d of auxiliary material
10.17182/hepdata.141286.v1/t44
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5e of auxiliary material
10.17182/hepdata.141286.v1/t45
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5f of auxiliary material
10.17182/hepdata.141286.v1/t46
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5g of auxiliary material
10.17182/hepdata.141286.v1/t47
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 5h of auxiliary material
10.17182/hepdata.141286.v1/t48
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=60$ of mass...
Data from Figure 6a of auxiliary material
10.17182/hepdata.141286.v1/t49
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6b of auxiliary material
10.17182/hepdata.141286.v1/t50
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6c of auxiliary material
10.17182/hepdata.141286.v1/t51
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6d of auxiliary material
10.17182/hepdata.141286.v1/t52
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6e of auxiliary material
10.17182/hepdata.141286.v1/t53
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6f of auxiliary material
10.17182/hepdata.141286.v1/t54
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6g of auxiliary material
10.17182/hepdata.141286.v1/t55
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 6h of auxiliary material
10.17182/hepdata.141286.v1/t56
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=80$ of mass...
Data from Figure 7a of auxiliary material
10.17182/hepdata.141286.v1/t57
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7b of auxiliary material
10.17182/hepdata.141286.v1/t58
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7c of auxiliary material
10.17182/hepdata.141286.v1/t59
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7d of auxiliary material
10.17182/hepdata.141286.v1/t60
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7e of auxiliary material
10.17182/hepdata.141286.v1/t61
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7f of auxiliary material
10.17182/hepdata.141286.v1/t62
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7g of auxiliary material
10.17182/hepdata.141286.v1/t63
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
Data from Figure 7h of auxiliary material
10.17182/hepdata.141286.v1/t64
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for HECOs of charge $|z|=100$ of mass...
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