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Limits for ${{\mathit H}^{\pm\pm}}$ with $\mathit T_{3}$ = $\pm{}$1
ATLS ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$
CHATRCHYAN
2012 AU
CMS ${{\mathit \tau}}{{\mathit \tau}}$
CMS ${{\mathit \mu}}{{\mathit \tau}}$
CMS ${{\mathit e}}{{\mathit \tau}}$
CMS ${{\mathit \mu}}{{\mathit \mu}}$
CMS ${{\mathit e}}{{\mathit \mu}}$
CMS ${{\mathit e}}{{\mathit e}}$
2021 U
ATLS ${{\mathit H}^{\pm\pm}}{{\mathit H}^{\mp}}$ associated production, ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ , ${{\mathit H}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit Z}}$
SIRUNYAN
CMS ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$
KANEMURA
RVUE ${{\mathit W}^{(*)\pm}}{{\mathit W}^{(*)\pm}}$
KHACHATRYAN
2013 Y
D0 ${{\mathit \tau}}{{\mathit \tau}}$
2008 AA
CDF ${{\mathit e}}{{\mathit \tau}}$
CDF ${{\mathit \mu}}{{\mathit \tau}}$
$>118.4$ 95 25
ASAKA
1 AABOUD 2019K search for pair production of ${{\mathit H}^{++}}{{\mathit H}^{--}}$ followed by the decay ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ in 36.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The search is interpreted in a doublet-triplet extension of the scalar sector with a vev of 0.1 GeV, leading to B( ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ ) = 1. See their Fig. 5 for limits on the cross section for ${\mathit m}_{{{\mathit H}^{++}}}$ between 200 and 700 GeV.
5 CHATRCHYAN 2012AU search for ${{\mathit H}^{++}}{{\mathit H}^{--}}$ production with 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. The limit assumes 100$\%$ branching ratio to the specified final state. See their Table 6 for limits including associated ${{\mathit H}^{++}}{{\mathit H}^{-}}$ production or assuming different scenarios.
8 AAD 2021U search for pair production of ${{\mathit H}^{++}}{{\mathit H}^{--}}$ followed by the decay ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ in 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The search is interpreted in a triplet extension of the SM Higgs sector with a triplet vev of 0.1 GeV, leading to B( ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ ) = 1. See their Fig. 9(a) for limits on the cross section for ${\mathit m}_{{{\mathit H}^{++}}}$ between 200 and 600 GeV.
9 AAD 2021U search for associated production of ${{\mathit H}^{\pm\pm}}{{\mathit H}^{\mp}}$ followed by the decays ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ , ${{\mathit H}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit Z}}$ in 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. ${{\mathit H}^{\pm\pm}}$ and ${{\mathit H}^{\pm}}$ are assumed to be degenerate in mass within 5 GeV. The search is interpreted in a triplet extension of the SM Higgs sector with a triplet vev of 0.1 GeV, leading to B( ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ ) = 1. See their Fig. 9(b) for limits on the cross section for ${\mathit m}_{{{\mathit H}^{++}}}$ between 200 and 600 GeV.
10 SIRUNYAN 2021W search for vector boson fusion production of ${{\mathit H}^{\pm\pm}}$ decaying to ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \nu}}{{\mathit \ell}^{\pm}}{{\mathit \nu}}$ in 137 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. See their Fig. 8 for limits on cross section times branching ratio for ${\mathit m}_{{{\mathit H}^{++}}}$ = $0.2 - 3.0$ TeV.
11 SIRUNYAN 2019CQ search for ${{\mathit H}^{\pm\pm}}$ production by vector boson fusion followed by the decay ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit \ell}}{{\mathit \nu}}$ in 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. See their Fig. 5 for limits on cross section times branching ratio for ${\mathit m}_{{{\mathit H}^{\pm\pm}}}$ between 0.6 and 2 TeV.
12 SIRUNYAN 2018CC search for ${{\mathit H}^{\pm\pm}}$ production by vector boson fusion followed by the decay ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ in 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. See their Fig. 3 for limits on cross section times branching ratio for ${\mathit m}_{{{\mathit H}^{\pm\pm}}}$ between 200 and 1000 GeV.
13 KANEMURA 2015 examine the case where ${{\mathit H}^{++}}$ decays preferentially to ${{\mathit W}^{(*)}}{{\mathit W}^{(*)}}$ and estimate that a lower mass limit of $\sim{}$84 GeV can be derived from the same-sign dilepton data of AAD 2015AG if ${{\mathit H}^{++}}$ decays with 100$\%$ branching ratio to ${{\mathit W}^{(*)}}{{\mathit W}^{(*)}}$ .
14 KHACHATRYAN 2015D search for ${{\mathit H}^{\pm\pm}}$ production by vector boson fusion followed by the decay ${{\mathit H}^{\pm\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\mathit W}^{\pm}}$ in 19.4 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. See their Fig. 4 for limits on cross section times branching ratio for ${\mathit m}_{{{\mathit H}^{++}}}$ between 160 and 800 GeV.
15 KANEMURA 2014 examine the case where ${{\mathit H}^{++}}$ decays preferentially to ${{\mathit W}^{(*)}}{{\mathit W}^{(*)}}$ and estimate that a lower mass limit of $\sim{}$60 GeV can be derived from the same-sign dilepton data of AAD 2012CY.
16 AAD 2013Y search for ${{\mathit H}^{++}}{{\mathit H}^{--}}$ production in a generic search of events with three charged leptons in 4.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. The limit assumes 100$\%$ branching ratio to the specified final state.
17 AAD 2012AY search for ${{\mathit H}^{++}}{{\mathit H}^{--}}$ production with 1.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. The limit assumes 100$\%$ branching ratio to the specified final state.
18 AAD 2012CQ search for ${{\mathit H}^{++}}{{\mathit H}^{--}}$ production with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. The limit assumes 100$\%$ branching ratio to the specified final state. See their Table 1 for limits assuming smaller branching ratios.
19 ABAZOV 2012A search for ${{\mathit H}^{++}}{{\mathit H}^{--}}$ production in 7.0 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV.
21 AALTONEN 2008AA search for ${{\mathit H}^{++}}{{\mathit H}^{--}}$ production in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$= 1.96 TeV. The limit assumes 100$\%$ branching ratio to the specified final state.
28 ASAKA 1995 point out that ${{\mathit H}^{++}}$ decays dominantly to four fermions in a large region of parameter space where the limit of ACTON 1992M from the search of dilepton modes does not apply.
AAD 2021U
JHEP 2106 146 Search for doubly and singly charged Higgs bosons decaying into vector bosons in multi-lepton final states with the ATLAS detector using proton-proton collisions at $\sqrt{s}$ = 13 TeV
SIRUNYAN 2021W
EPJ C81 723 Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton?proton collisions at $\sqrt{s} = 13\,{\text {TeV}} $
AABOUD 2019K
EPJ C79 58 Search for doubly charged scalar bosons decaying into same-sign $W$ boson pairs with the ATLAS detector
SIRUNYAN 2019CQ
PL B798 134985 Search for anomalous electroweak production of vector boson pairs in association with two jets in proton-proton collisions at 13 TeV
SIRUNYAN 2018CC
PRL 120 081801 Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV
KANEMURA 2015
PTEP 2015 051B02 LHC Run-I Constraint on the Mass of Doubly Charged Higgs Bosons in the Same-Sign Diboson Decay Scenario
KHACHATRYAN 2015D
PRL 114 051801 Study of Vector Boson Scattering and Search for New Physics in Events with Two Same-Sign Leptons and Two Jets
PR D90 115018 Bounds on the Mass of Doubly-Charged Higgs Bosons in the Same-Sign Diboson Decay Scenario
AAD 2013Y
PR D87 052002 Search for New Phenomena in Events with Three Charged Leptons at $\sqrt {s }$ = 7 TeV with the ATLAS Detector
CHATRCHYAN 2012AU
EPJ C72 2189 A Search for a Doubly-Charged Higgs Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AALTONEN 2008AA
PRL 101 121801 Search for Doubly Charged Higgs Bosons with Lepton-Flavor-Violating Decays Involving Tau Leptons
ASAKA 1995
PL B345 36 Four Fermion Decay of Higgs Bosons