$> 89.7$ |
|
1 |
|
DLPH |
$\bf{> 92.8}$ |
95 |
2 |
|
LEP |
$>84.5$ |
95 |
3, 4 |
|
OPAL |
$>86.0$ |
95 |
3, 5 |
|
L3 |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
|
|
6 |
|
ATLS |
|
|
7 |
|
CMS |
|
|
8 |
|
ATLS |
|
|
9 |
|
CMS |
|
|
10 |
|
ATLS |
|
|
11 |
|
CMS |
|
|
12 |
|
ATLS |
|
|
13 |
|
LHCB |
|
|
14 |
|
CMS |
|
|
15 |
|
TEVA |
|
|
16 |
|
CDF |
|
|
17 |
|
D0 |
|
|
18 |
|
CMS |
|
|
19 |
|
D0 |
|
|
20 |
|
D0 |
|
|
21 |
|
CDF |
|
|
22 |
|
OPAL |
$>89.8$ |
95 |
3, 23 |
|
ALEP |
1
ABDALLAH 2008B give limits in eight $\mathit CP$-conserving benchmark scenarios and some $\mathit CP$-violating scenarios. See paper for excluded regions for each scenario. Supersedes ABDALLAH 2004 .
|
2
SCHAEL 2006B make a combined analysis of the LEP data. The quoted limit is for the $\mathit m{}^{{\mathrm {max}}}_{h}$ scenario with ${\mathit m}_{{{\mathit t}}}$ = 174.3 GeV. In the $\mathit CP$-violating CPX scenario no lower bound on ${\mathit m}_{{{\mathit H}_{{1}}^{0}}}$ can be set at 95$\%$ CL. See paper for excluded regions in various scenarios. See Figs. $2 - 6$ and Tabs. $14 - 21$ for limits on ${\mathit \sigma (}$ ${{\mathit Z}}{{\mathit H}^{0}}{)}\cdot{}$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ ) and ${\mathit \sigma (}$ ${{\mathit H}_{{1}}^{0}}{{\mathit H}_{{2}}^{0}}{)}\cdot{}$ B(${{\mathit H}_{{1}}^{0}},{{\mathit H}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ ).
|
3
Search for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}_{{1}}^{0}}{{\mathit A}^{0}}$ in the final states ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ and ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ , and ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}_{{1}}^{0}}{{\mathit Z}}$ . Universal scalar mass of 1$~$TeV, SU(2) gaugino mass of 200 GeV, and $\mu $= $-200$ GeV are assumed, and two-loop radiative corrections incorporated. The limits hold for ${\mathit m}_{{{\mathit t}}}$=175 GeV, and for the $\mathit m{}^{{\mathrm {max}}}_{h}$ scenario.
|
4
ABBIENDI 2004M exclude 0.7 $<$ tan ${{\mathit \beta}}$ $<$ 1.9, assuming ${\mathit m}_{{{\mathit t}}}$ = 174.3 GeV. Limits for other MSSM benchmark scenarios, as well as for $\mathit CP$ violating cases, are also given.
|
5
ACHARD 2002H also search for the final state ${{\mathit H}_{{1}}^{0}}$ ${{\mathit Z}}$ $\rightarrow$ 2 ${{\mathit A}^{0}}{{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ . In addition, the MSSM parameter set in the ``large-$\mu $'' and ``no-mixing'' scenarios are examined.
|
6
AABOUD 2016AA search for production of a Higgs boson in gluon fusion and in association with a ${{\mathit b}}{{\overline{\mathit b}}}$ pair followed by the decay ${{\mathit H}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in 3.2 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. See their Fig. 5(a, b) for limits on cross section times branching ratio for ${\mathit m}_{{{\mathit H}_{{2}}^{0}}}$ = $200 - 1200$ GeV, and Fig. 5(c, d) for the excluded region in the MSSM parameter space in the ${{\mathit m}}{}^{{\mathrm {mod+}}}_{h}$ and hMSSM scenarios.
|
7
KHACHATRYAN 2016A search for production of a Higgs boson in gluon fusion and in association with a ${{\mathit b}}{{\overline{\mathit b}}}$ pair followed by the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. See their Fig. 7 for the excluded region in the MSSM parameter space in the ${{\mathit m}}{}^{{\mathrm {mod+}}}_{h}$ benchmark scenario and Fig. 9 for limits on cross section times branching ratio.
|
8
AAD 2015CE search for production of ${{\mathit H}_{{2}}^{0}}$ decaying to ${{\mathit H}^{0}}{{\mathit H}^{0}}$ in the final states ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ and ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit W}}{{\mathit W}^{*}}$ in 20.3 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV and combine with data from AAD 2015H ( ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit b}}{{\overline{\mathit b}}}$ ) and AAD 2015BK ( ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ ). See their Fig. 7 for excluded regions in the parameter space in several scenarios.
|
9
KHACHATRYAN 2015AY search for production of a Higgs boson in association with a ${{\mathit b}}$ quark in the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ in 19.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV and combine with 7 TeV data. See their Fig. 6 for the limits on cross section times branching ratio for ${\mathit m}_{{{\mathit A}^{0}}}$ = $100 - 900$ GeV and Figs. $7 - 9$ for the excluded region in the MSSM parameter space in various benchmark scenarios.
|
10
AAD 2014AW search for production of a Higgs boson followed by the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in 19.5--20.3 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. See their Fig. 11 for the limits on cross section times branching ratio and their Figs. 9 and 10 for the excluded region in the MSSM parameter space. For ${\mathit m}_{{{\mathit A}^{0}}}$ = 140 GeV, the region tan ${{\mathit \beta}}>$ 5.4 is excluded at 95$\%$ CL in the ${{\mathit m}}{}^{{\mathrm {max}}}_{h}$ scenario.
|
11
KHACHATRYAN 2014M search for production of a Higgs boson in gluon fusion and in association with a ${{\mathit b}}$ quark followed by the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.7 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. See their Figs. 7 and 8 for one- and two-dimensional limits on cross section times branching ratio and their Figs. 5 and 6 for the excluded region in the MSSM parameter space. For ${\mathit m}_{{{\mathit A}^{0}}}$ = 140 GeV, the region tan ${{\mathit \beta}}>$ 3.8 is excluded at 95$\%$ CL in the ${{\mathit m}}{}^{{\mathrm {max}}}_{h}$ scenario.
|
12
AAD 2013O search for production of a Higgs boson in the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ and ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ with $4.7 - 4.8$ fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. See their Fig. 6 for the excluded region in the MSSM parameter space and their Fig. 7 for the limits on cross section times branching ratio. For ${\mathit m}_{{{\mathit A}^{0}}}$ = $110 - 170$ GeV, tan ${{\mathit \beta}}{ {}\gtrsim{} }$ 10 is excluded, and for tan ${{\mathit \beta}}$ = 50, ${\mathit m}_{{{\mathit A}^{0}}}$ below 470 GeV is excluded at 95$\%$ CL in the $\mathit m{}^{{\mathrm {max}}}_{h}$ scenario.
|
13
AAIJ 2013T search for production of a Higgs boson in the forward region in the decay ${{\mathit H}_{{1,2}}^{0}}$/ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in 1.0 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. See their Fig. 2 for the limits on cross section times branching ratio and the excluded region in the MSSM parameter space.
|
14
CHATRCHYAN 2013AG search for production of a Higgs boson in association with a ${{\mathit b}}$ quark in the decay ${{\mathit H}_{{1,2}}^{0}}$/ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ in $2.7 - 4.8$ fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. See their Fig. 6 for the excluded region in the MSSM parameter space and Fig. 5 for the limits on cross section times branching ratio. For ${\mathit m}_{{{\mathit A}^{0}}}$ = $90 - 350$ GeV, upper bounds on tan ${{\mathit \beta}}$ of $18 - 42$ at 95$\%$ CL are obtained in the $\mathit m{}^{{\mathrm {max}}}_{h} $ scenario with ${{\mathit \mu}}$ = +200 GeV.
|
15
AALTONEN 2012AQ combine AALTONEN 2012X and ABAZOV 2011K. See their Table I and Fig. 1 for the limit on cross section times branching ratio and Fig. 2 for the excluded region in the MSSM parameter space.
|
16
AALTONEN 2012X search for associated production of a Higgs boson and a ${{\mathit b}}$ quark in the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , with 2.6 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. See their Table III and Fig. 15 for the limit on cross section times branching ratio and Figs. 17, 18 for the excluded region in the MSSM parameter space.
|
17
ABAZOV 2012G search for production of a Higgs boson in the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ with 7.3 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV and combine with ABAZOV 2011W and ABAZOV 2011K. See their Figs. 4, 5, and 6 for the excluded region in the MSSM parameter space. For ${\mathit m}_{{{\mathit A}^{0}}}$ = $90 - 180$ GeV, tan ${{\mathit \beta}}{ {}\gtrsim{} }$ 30 is excluded at 95$\%$ CL. in the $\mathit m{}^{{\mathrm {max}}}_{h}$ scenario.
|
18
CHATRCHYAN 2012K search for production of a Higgs boson in the decay ${{\mathit H}_{{1,2}}^{0}}$ $/$ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ with 4.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. See their Fig. 3 and Table 4 for the excluded region in the MSSM parameter space. For ${\mathit m}_{{{\mathit A}^{0}}}$ = 160 GeV, the region tan ${{\mathit \beta}}$ $>$ 7.1 is excluded at 95$\%$ CL in the $\mathit m{}^{{\mathrm {max}}}_{h}$ scenario. Superseded by KHACHATRYAN 2014M.
|
19
ABAZOV 2011K search for associated production of a Higgs boson and a ${{\mathit b}}$ quark, followed by the decay ${{\mathit H}_{{1,2}}^{0}}$/ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , in 5.2 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. See their Fig.$~$5/Table$~$2 for the limit on cross section times branching ratio and Fig.$~$6 for the excluded region in the MSSM parameter space for ${{\mathit \mu}}$ = $-200$ GeV.
|
20
ABAZOV 2011W search for associated production of a Higgs boson and a ${{\mathit b}}$ quark, followed by the decay ${{\mathit H}_{{1,2}}^{0}}$/ ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}$ , in 7.3 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. See their Fig.$~$2 for the limit on cross section times branching ratio and for the excluded region in the MSSM parameter space.
|
21
AALTONEN 2009AR search for Higgs bosons decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in two doublet models in 1.8 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. See their Fig. 2 for the limit on $\sigma \cdot{}$B( ${{\mathit H}^{0}_{{{1,2}}}}$ / ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ ) for different Higgs masses, and see their Fig. 3 for the excluded region in the MSSM parameter space.
|
22
ABBIENDI 2003G search for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}_{{1}}^{0}}{{\mathit Z}}$ followed by ${{\mathit H}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit A}^{0}}{{\mathit A}^{0}}$ , ${{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$ , ${{\mathit g}}{{\mathit g}}$ , or ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ . In the no-mixing scenario, the region ${\mathit m}_{{{\mathit H}_{{1}}^{0}}}$ = 45-85 GeV and ${\mathit m}_{{{\mathit A}^{0}}}$ = 2-9.5 GeV is excluded at 95$\%$ CL.
|
23
HEISTER 2002 excludes the range $0.7<$tan $\beta <2.3$. A wider range is excluded with different stop mixing assumptions. Updates BARATE 2001C.
|