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 collaboration
CERN-EP-2022-146, 2022.

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...

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....

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$_a$ =...