Search for dark matter produced in association with a single top quark and an energetic $W$ boson in $\sqrt{s}=$ 13 TeV $pp$ collisions with the ATLAS detector

The ATLAS collaboration
Eur.Phys.J.C 83 (2023) 603, 2023.

Abstract (data abstract)
Version of twMeT HEPData record as of 09.12.2022.

  • Overview

    10.17182/hepdata.136029.v1/t1

    - - - - - - - - Overview of HEPData Record - - - - - - - -...

  • highst_mamh_obs

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t2

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • highst_mamh_exp

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t3

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • highst_mhtb_lowma_obs

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t4

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • highst_mhtb_lowma_exp

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t5

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • highst_mhtb_highma_obs

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t6

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • highst_mhtb_highma_exp

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t7

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • highst_dmtt_mamh_obs

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t8

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • highst_dmtt_mamh_exp

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t9

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • highst_dmtt_mhtb_lowma_obs

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t10

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • highst_dmtt_mhtb_lowma_exp

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t11

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • highst_dmtt_mhtb_highma_obs

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t12

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • highst_dmtt_mhtb_highma_exp

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t13

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • lowst_mamh_obs

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t14

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • lowst_mamh_exp

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t15

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • lowst_mhtb_lowma_obs

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t16

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • lowst_mhtb_lowma_exp

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t17

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • lowst_mhtb_highma_obs

    Data from figaux. 1e.

    10.17182/hepdata.136029.v1/t18

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • lowst_mhtb_highma_exp

    Data from figaux. 1e.

    10.17182/hepdata.136029.v1/t19

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • lowst_dmtt_mamh_obs

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t20

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • lowst_dmtt_mamh_exp

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t21

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • lowst_dmtt_mhtb_lowma_obs

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t22

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • lowst_dmtt_mhtb_lowma_exp

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t23

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • lowst_dmtt_mhtb_highma_obs

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t24

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • lowst_dmtt_mhtb_highma_exp

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t25

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_highst_mamh_obs

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t26

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_highst_mamh_exp

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t27

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_highst_mhtb_lowma_obs

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t28

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_highst_mhtb_lowma_exp

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t29

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_highst_mhtb_highma_obs

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t30

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_highst_mhtb_highma_exp

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t31

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_highst_dmtt_mamh_obs

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t32

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_highst_dmtt_mamh_exp

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t33

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_highst_dmtt_mhtb_lowma_obs

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t34

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_highst_dmtt_mhtb_lowma_exp

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t35

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_highst_dmtt_mhtb_highma_obs

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t36

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_highst_dmtt_mhtb_highma_exp

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t37

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_lowst_mamh_obs

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t38

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_lowst_mamh_exp

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t39

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_lowst_mhtb_lowma_obs

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t40

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_lowst_mhtb_lowma_exp

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t41

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_lowst_mhtb_highma_obs

    Data from figaux. 1e.

    10.17182/hepdata.136029.v1/t42

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_lowst_mhtb_highma_exp

    Data from figaux. 1e.

    10.17182/hepdata.136029.v1/t43

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_lowst_dmtt_mamh_obs

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t44

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_lowst_dmtt_mamh_exp

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t45

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 0LBoosted_lowst_dmtt_mhtb_lowma_obs

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t46

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_lowst_dmtt_mhtb_lowma_exp

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t47

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 0LBoosted_lowst_dmtt_mhtb_highma_obs

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t48

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 0LBoosted_lowst_dmtt_mhtb_highma_exp

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t49

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_highst_mamh_obs

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t50

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_highst_mamh_exp

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t51

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_highst_mhtb_lowma_obs

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t52

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_highst_mhtb_lowma_exp

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t53

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_highst_mhtb_highma_obs

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t54

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_highst_mhtb_highma_exp

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t55

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_highst_dmtt_mamh_obs

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t56

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_highst_dmtt_mamh_exp

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t57

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_highst_dmtt_mhtb_lowma_obs

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t58

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_highst_dmtt_mhtb_lowma_exp

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t59

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_highst_dmtt_mhtb_highma_obs

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t60

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_highst_dmtt_mhtb_highma_exp

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t61

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_lowst_mamh_obs

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t62

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_lowst_mamh_exp

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t63

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_lowst_mhtb_lowma_obs

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t64

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_lowst_mhtb_lowma_exp

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t65

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_lowst_mhtb_highma_exp

    Data from figaux. 1e.

    10.17182/hepdata.136029.v1/t66

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_lowst_dmtt_mamh_obs

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t67

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_lowst_dmtt_mamh_exp

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t68

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 1LBoosted_lowst_dmtt_mhtb_lowma_obs

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t69

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_lowst_dmtt_mhtb_lowma_exp

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t70

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 1LBoosted_lowst_dmtt_mhtb_highma_obs

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t71

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 1LBoosted_lowst_dmtt_mhtb_highma_exp

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t72

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_highst_mamh_obs

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t73

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 2L_highst_mamh_exp

    Data from fig. 10a.

    10.17182/hepdata.136029.v1/t74

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 2L_highst_mhtb_lowma_obs

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t75

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_highst_mhtb_lowma_exp

    Data from fig. 10c.

    10.17182/hepdata.136029.v1/t76

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_highst_mhtb_highma_obs

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t77

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_highst_mhtb_highma_exp

    Data from fig. 10e.

    10.17182/hepdata.136029.v1/t78

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_highst_dmtt_mamh_obs

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t79

    The observed exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 2L_highst_dmtt_mamh_exp

    Data from fig. 10b.

    10.17182/hepdata.136029.v1/t80

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 2L_highst_dmtt_mhtb_lowma_obs

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t81

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_highst_dmtt_mhtb_lowma_exp

    Data from fig. 10d.

    10.17182/hepdata.136029.v1/t82

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_highst_dmtt_mhtb_highma_obs

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t83

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_highst_dmtt_mhtb_highma_exp

    Data from fig. 10f.

    10.17182/hepdata.136029.v1/t84

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_lowst_mamh_exp

    Data from figaux. 1a.

    10.17182/hepdata.136029.v1/t85

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 2L_lowst_mhtb_lowma_exp

    Data from figaux. 1c.

    10.17182/hepdata.136029.v1/t86

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_lowst_mhtb_highma_exp

    Data from figaux. 1e.

    10.17182/hepdata.136029.v1/t87

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_lowst_dmtt_mamh_exp

    Data from figaux. 1b.

    10.17182/hepdata.136029.v1/t88

    The expected exclusion contour at 95% CL as a function of the $m_a$ vs. $m_{H^{\pm}}$ and assuming tan$\beta$ = 1,...

  • 2L_lowst_dmtt_mhtb_lowma_obs

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t89

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_lowst_dmtt_mhtb_lowma_exp

    Data from figaux. 1d.

    10.17182/hepdata.136029.v1/t90

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 150...

  • 2L_lowst_dmtt_mhtb_highma_obs

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t91

    The observed exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • 2L_lowst_dmtt_mhtb_highma_exp

    Data from figaux. 1f.

    10.17182/hepdata.136029.v1/t92

    The expected exclusion contour at 95% CL as a function of the $m_{H^{\pm}}$ vs. tan$\beta$ and assuming $m_a$ = 250...

  • mamH_xSecUpperLimit_Comb_st0p7

    Data from figaux. 02a.

    10.17182/hepdata.136029.v1/t93

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_Comb_st0p7

    Data from figaux. 02c.

    10.17182/hepdata.136029.v1/t94

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_Comb_st0p7

    Data from figaux. 02e.

    10.17182/hepdata.136029.v1/t95

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_Comb_st0p7_DMtt

    Data from figaux. 02b.

    10.17182/hepdata.136029.v1/t96

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_Comb_st0p7_DMtt

    Data from figaux. 02d.

    10.17182/hepdata.136029.v1/t97

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_Comb_st0p7_DMtt

    Data from figaux. 02f.

    10.17182/hepdata.136029.v1/t98

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_Comb_st0p35

    Data from figaux. 03a.

    10.17182/hepdata.136029.v1/t99

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_Comb_st0p35

    Data from figaux. 03c.

    10.17182/hepdata.136029.v1/t100

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_Comb_st0p35

    Data from figaux. 03e.

    10.17182/hepdata.136029.v1/t101

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_Comb_st0p35_DMtt

    Data from figaux. 03b.

    10.17182/hepdata.136029.v1/t102

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_Comb_st0p35_DMtt

    Data from figaux. 03d.

    10.17182/hepdata.136029.v1/t103

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_Comb_st0p35_DMtt

    Data from figaux. 03f.

    10.17182/hepdata.136029.v1/t104

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_0L_st0p7

    Data from figaux. 04a.

    10.17182/hepdata.136029.v1/t105

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_0L_st0p7

    Data from figaux. 04c.

    10.17182/hepdata.136029.v1/t106

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_0L_st0p7

    Data from figaux. 04e.

    10.17182/hepdata.136029.v1/t107

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_0L_st0p7_DMtt

    Data from figaux. 04b.

    10.17182/hepdata.136029.v1/t108

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_0L_st0p7_DMtt

    Data from figaux. 04d.

    10.17182/hepdata.136029.v1/t109

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_0L_st0p7_DMtt

    Data from figaux. 04f.

    10.17182/hepdata.136029.v1/t110

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_0L_st0p35

    Data from figaux. 05a.

    10.17182/hepdata.136029.v1/t111

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_0L_st0p35

    Data from figaux. 05c.

    10.17182/hepdata.136029.v1/t112

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_0L_st0p35

    Data from figaux. 05e.

    10.17182/hepdata.136029.v1/t113

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_0L_st0p35_DMtt

    Data from figaux. 05b.

    10.17182/hepdata.136029.v1/t114

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_0L_st0p35_DMtt

    Data from figaux. 05d.

    10.17182/hepdata.136029.v1/t115

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_0L_st0p35_DMtt

    Data from figaux. 05f.

    10.17182/hepdata.136029.v1/t116

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_1L_st0p7

    Data from figaux. 06a.

    10.17182/hepdata.136029.v1/t117

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_1L_st0p7

    Data from figaux. 06c.

    10.17182/hepdata.136029.v1/t118

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_1L_st0p7

    Data from figaux. 06e.

    10.17182/hepdata.136029.v1/t119

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_1L_st0p7_DMtt

    Data from figaux. 06b.

    10.17182/hepdata.136029.v1/t120

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_1L_st0p7_DMtt

    Data from figaux. 06d.

    10.17182/hepdata.136029.v1/t121

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_1L_st0p7_DMtt

    Data from figaux. 06f.

    10.17182/hepdata.136029.v1/t122

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_1L_st0p35

    Data from figaux. 07a.

    10.17182/hepdata.136029.v1/t123

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_1L_st0p35

    Data from figaux. 07c.

    10.17182/hepdata.136029.v1/t124

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_1L_st0p35

    Data from figaux. 07e.

    10.17182/hepdata.136029.v1/t125

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • mamH_xSecUpperLimit_1L_st0p35_DMtt

    Data from figaux. 07b.

    10.17182/hepdata.136029.v1/t126

    Model dependent upper limit on the cross section for the $m_a$ vs. $ m_{H^{\pm}}$ signal grid assuming tan$\beta$ = 1,...

  • mHtblow_xSecUpperLimit_1L_st0p35_DMtt

    Data from figaux. 07d.

    10.17182/hepdata.136029.v1/t127

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 150 GeV,...

  • mHtbhigh_xSecUpperLimit_1L_st0p35_DMtt

    Data from figaux. 07f.

    10.17182/hepdata.136029.v1/t128

    Model dependent upper limit on the cross section for the $m_{H^{\pm}}$ vs. tan$\beta$ signal grid assuming $m_a$ = 250 GeV,...

  • SR0L_mwtagged

    Data from fig. 08b.

    10.17182/hepdata.136029.v1/t129

    The distributions of $m_{\mathrm{b1},\mathrm{W-tagged}}$ in the 0L inclusive signal region. For each bin yields for the data and total SM...

  • SR0L_mtbmet

    Data from fig. 08c.

    10.17182/hepdata.136029.v1/t130

    The distributions of $m_{\mathrm{T}}^{\mathrm{b,E_{\mathrm{T}^{\mathrm{miss}}}}}$ in the 0L inclusive signal region. For each bin yields for the data and total SM...

  • SR0L_nwtagged

    Data from fig. 08d.

    10.17182/hepdata.136029.v1/t131

    The distributions of $N_{\mathrm{W-tagged}}$ in the 0L inclusive signal region. For each bin yields for the data and total SM...

  • SR1L_Had_mbj

    Data from fig. 09b.

    10.17182/hepdata.136029.v1/t132

    The distributions of $m_{\mathrm{b1},\mathrm{\cancel{b1}}}$ in the hadronic top inclusive signal region. For each bin yields for the data and total...

  • SR1L_Lep_nwtaggged

    Data from fig. 09c.

    10.17182/hepdata.136029.v1/t133

    The distributions of $m_{\mathrm{b1},\mathrm{\cancel{b1}}}$ in the leptonic top inclusive signal region. For each bin yields for the data and total...

  • SR1L_Lep_mbj

    Data from fig. 09d.

    10.17182/hepdata.136029.v1/t134

    The distributions of $m_{\mathrm{b1},\mathrm{\cancel{b1}}}$ in the leptonic top inclusive signal region. For each bin yields for the data and total...

  • cutflow_SR0L

    Data from tabaux. 01.

    10.17182/hepdata.136029.v1/t135

    Cutflow for the reference point $(\it{m}_{\mathrm{H^{\pm}}}, \it{m}_{a}, tan\beta, sin\theta )=$ (500,100,1,0.7) , (800,150,20,0.7), (600,250,30,0.7), (1000,400,1,0.7) in 0L regions. Results are...

  • cutflow_SR1L_Lep

    Data from tabaux. 02.

    10.17182/hepdata.136029.v1/t136

    Cutflow for the reference point $(\it{m}_{\mathrm{H^{\pm}}}, \it{m}_{a}, tan\beta, sin\theta )=$ (500,100,1,0.7) , (800,150,20,0.7), (600,250,30,0.7), (1000,400,1,0.7) in 1L leptonic top regions....

  • cutflow_SR1L_Had

    Data from tabaux. 03.

    10.17182/hepdata.136029.v1/t137

    Cutflow for the reference point $(\it{m}_{\mathrm{H^{\pm}}}, \it{m}_{a}, tan\beta, sin\theta )=$ (500,100,1,0.7) , (800,150,20,0.7), (600,250,30,0.7), (1000,400,1,0.7) in 1L hadronic top regions....

  • highst_grid1_Acc_0L

    Data from figaux 09.

    10.17182/hepdata.136029.v1/t138

    Signal acceptance in the 0L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • highst_grid1_Eff_0L

    Data from figaux 08.

    10.17182/hepdata.136029.v1/t139

    Signal efficiency in the 0L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • highst_grid2_Acc_0L

    Data from figaux 13.

    10.17182/hepdata.136029.v1/t140

    Signal acceptance in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid2_Eff_0L

    Data from figaux 12.

    10.17182/hepdata.136029.v1/t141

    Signal efficiency in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid3_Acc_0L

    Data from figaux 11.

    10.17182/hepdata.136029.v1/t142

    Signal acceptance in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid3_Eff_0L

    Data from figaux 10.

    10.17182/hepdata.136029.v1/t143

    Signal efficiency in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid1_Acc_1L

    Data from figaux 15.

    10.17182/hepdata.136029.v1/t144

    Signal acceptance in the 1L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • highst_grid1_Eff_1L

    Data from figaux 14.

    10.17182/hepdata.136029.v1/t145

    Signal efficiency in the 1L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • highst_grid2_Acc_1L

    Data from figaux 19.

    10.17182/hepdata.136029.v1/t146

    Signal acceptance in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid2_Eff_1L

    Data from figaux 18.

    10.17182/hepdata.136029.v1/t147

    Signal efficiency in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid3_Acc_1L

    Data from figaux 17.

    10.17182/hepdata.136029.v1/t148

    Signal acceptance in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • highst_grid3_Eff_1L

    Data from figaux 16.

    10.17182/hepdata.136029.v1/t149

    Signal efficiency in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid1_Acc_0L

    Data from figaux 21.

    10.17182/hepdata.136029.v1/t150

    Signal acceptance in the 0L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • lowst_grid1_Eff_0L

    Data from figaux 20.

    10.17182/hepdata.136029.v1/t151

    Signal efficiency in the 0L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • lowst_grid2_Acc_0L

    Data from figaux 25.

    10.17182/hepdata.136029.v1/t152

    Signal acceptance in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid2_Eff_0L

    Data from figaux 24.

    10.17182/hepdata.136029.v1/t153

    Signal efficiency in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid3_Acc_0L

    Data from figaux 23.

    10.17182/hepdata.136029.v1/t154

    Signal acceptance in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid3_Eff_0L

    Data from figaux 22.

    10.17182/hepdata.136029.v1/t155

    Signal efficiency in the 0L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid1_Acc_1L

    Data from figaux 27.

    10.17182/hepdata.136029.v1/t156

    Signal acceptance in the 1L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • lowst_grid1_Eff_1L

    Data from figaux 26.

    10.17182/hepdata.136029.v1/t157

    Signal efficiency in the 1L region for 2HDM+a model DM signals on the plane defined by m$_a$--m$_{H^{\pm}}$ assuming tan$\beta$ =...

  • lowst_grid2_Acc_1L

    Data from figaux 31.

    10.17182/hepdata.136029.v1/t158

    Signal acceptance in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid2_Eff_1L

    Data from figaux 30.

    10.17182/hepdata.136029.v1/t159

    Signal efficiency in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid3_Acc_1L

    Data from figaux 29.

    10.17182/hepdata.136029.v1/t160

    Signal acceptance in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

  • lowst_grid3_Eff_1L

    Data from figaux 28.

    10.17182/hepdata.136029.v1/t161

    Signal efficiency in the 1L region for 2HDM+a model DM signals on the plane defined by m$_{H^{\pm}}$--tan$\beta$ assuming m$_a$ =...

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