Search for magnetic monopoles and stable particles with high electric charges in $\sqrt{s}=$13 TeV $pp$ collisions with the ATLAS detector

The ATLAS collaboration
JHEP 11 (2023) 112, 2023.

Abstract (data abstract)
CERN-LHC. We present a search for magnetic monopoles and high-electric-charge objects using LHC Run 2 $\sqrt{s}$ = 13 TeV proton–proton collisions recorded by the ATLAS detector. A total integrated luminosity of 138 fb$^{−1}$ was collected by a specialized trigger and analyzed.No highly ionizing particle candidate was observed. Considering the Drell-Yan and photon-fusion pair production mechanisms as benchmark models, lowest to-date cross-section upper limits are presented for spin-0 and spin-$\frac{1}{2}$ magnetic monopoles of charge 1$g_{D}$ and 2$g_{D}$ and high-electric-charge objects of charge $20\le|z|\le100$, for masses between 200 and 4000 GeV.

  • 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...

  • Table 2

    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...

  • Table 3

    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...

  • Table 4

    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...

  • Table 5

    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...

  • Table 6

    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...

  • Table 7

    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...

  • Table 8

    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...

  • Table 9

    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.

  • Table 10

    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.

  • Table 11

    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.

  • Table 12

    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.

  • Table 13

    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.

  • Table 14

    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.

  • Table 15

    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.

  • Table 16

    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.

  • Table 17

    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.

  • Table 18

    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.

  • Table 19

    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.

  • Table 20

    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.

  • Table 21

    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.

  • Table 22

    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.

  • Table 23

    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.

  • Table 24

    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.

  • Table 25

    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...

  • Table 26

    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...

  • Table 27

    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...

  • Table 28

    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...

  • Table 29

    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...

  • Table 30

    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...

  • Table 31

    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...

  • Table 32

    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...

  • Table 33

    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...

  • Table 34

    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...

  • Table 35

    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...

  • Table 36

    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...

  • Table 37

    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...

  • Table 38

    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...

  • Table 39

    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...

  • Table 40

    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...

  • Table 41

    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...

  • Table 42

    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...

  • Table 43

    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...

  • Table 44

    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...

  • Table 45

    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...

  • Table 46

    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...

  • Table 47

    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...

  • Table 48

    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...

  • Table 49

    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...

  • Table 50

    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...

  • Table 51

    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...

  • Table 52

    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...

  • Table 53

    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...

  • Table 54

    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...

  • Table 55

    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...

  • Table 56

    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...

  • Table 57

    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...

  • Table 58

    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...

  • Table 59

    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...

  • Table 60

    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...

  • Table 61

    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...

  • Table 62

    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...

  • Table 63

    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...

  • Table 64

    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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