# MASS LIMITS FOR NEUTRAL HIGGS BOSONS IN EXTENDED HIGGS MODELS

This Section covers models which do not fit into either the Standard Model or its simplest minimal Supersymmetric extension (MSSM), leading to anomalous production rates, or nonstandard final states and branching ratios. In particular, this Section covers limits which may apply to generic two-Higgs-doublet models (2HDM), or to special regions of the MSSM parameter space where decays to invisible particles or to photon pairs are dominant (see the review on Status of Higgs Boson Physics''). Concerning the mass limits for ${{\mathit H}^{0}}$ and ${{\mathit A}^{0}}$ listed below, see the footnotes or the comment lines for details on the nature of the models to which the limits apply.
The observed signal at about 125 GeV, see section ${{\mathit H}^{0}}$'', can be interpreted as one of the neutral Higgs bosons of an extended Higgs sector.

# Mass Limits for ${{\boldsymbol H}^{0}}$ with Vanishing Yukawa Couplings INSPIRE search

These limits assume that ${{\mathit H}^{0}}$ couples to gauge bosons with the same strength as the Standard Model Higgs boson, but has no coupling to quarks and leptons (this is often referred to as fermiophobic'').
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
• • • We do not use the following data for averages, fits, limits, etc. • • •
95 1
 2013 K
CDF ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
$\text{none 100 - 113}$ 95 2
 2013 L
CDF ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}{{\mathit W}^{*}}$ , ${{\mathit Z}}{{\mathit Z}^{*}}$
$\text{none 100 - 116}$ 95 3
 2013 M
TEVA ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}{{\mathit W}^{*}}$ , ${{\mathit Z}}{{\mathit Z}^{*}}$
4
 2013 G
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
$\text{none 100 - 113}$ 95 5
 2013 H
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
6
 2013 I
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
7
 2013 J
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ , ${{\mathit Z}}{{\mathit Z}^{(*)}}$
$\text{none 100 - 114}$ 95 8
 2013 L
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}{{\mathit W}^{*}}$ , ${{\mathit Z}}{{\mathit Z}^{*}}$
$\text{none 110 - 147}$ 95 9
 2013 AL
CMS ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 110 - 118, 119.5 - 121}$ 95 10
 2012 N
ATLS ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 100 - 114}$ 95 11
 2012 AN
CDF ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 110 - 194}$ 95 12
 2012 AO
CMS ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}{{\mathit W}^{(*)}}$ , ${{\mathit Z}}{{\mathit Z}^{(*)}}$
$\text{none 70 - 106}$ 95 13
 2009 AB
CDF ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 70 - 100}$ 95 14
 2008 U
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$> 105.8$ 95 15
 2007
ALEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$
$>104.1$ 95 16, 17
 2004 L
DLPH ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$>107$ 95 18
 2003 C
L3 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ , ${{\mathit Z}}{{\mathit Z}^{*}}$ , ${{\mathit \gamma}}{{\mathit \gamma}}$
$>105.5$ 95 16, 19
 2002 F
OPAL ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$>105.4$ 95 20
 2002 C
L3 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 60 - 82}$ 95 21
 2001 H
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$>94.9$ 95 22
 2000 S
L3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$>100.7$ 95 23
 2000 L
ALEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$>96.2$ 95 24
 1999 O
OPAL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$>78.5$ 95 25
 1999 B
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
26
 1999 P
DLPH ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit \gamma}}$ and/or ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
1  AALTONEN 2013K search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ in 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. A limit on cross section times branching ratio which corresponds to ($1.3 - 6.6$) times the expected cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 200$ GeV at 95$\%$ CL.
2  AALTONEN 2013L combine all CDF searches with $9.45 - 10.0$ fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV.
3  AALTONEN 2013M combine all Tevatron data from the CDF and D0 Collaborations of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV.
4  ABAZOV 2013G search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ in 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. A limit on cross section times branching ratio which corresponds to ($2 - 9$) times the expected cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 200$ GeV at 95$\%$ CL.
5  ABAZOV 2013H search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 9.6 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV.
6  ABAZOV 2013I search for ${{\mathit H}^{0}}$ production in the final state with one lepton and two or more jets plus missing $\mathit E_{T}$ in 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The search is sensitive to ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ and vector-boson fusion Higgs production with ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ . A limit on cross section times branching ratio which corresponds to ($8 - 30$) times the expected cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 200$ GeV at 95$\%$ CL.
7  ABAZOV 2013J search for ${{\mathit H}^{0}}$ production in the final states ${{\mathit e}}{{\mathit e}}{{\mathit \mu}}$ , ${{\mathit e}}{{\mathit \mu}}{{\mathit \mu}}$ , ${{\mathit \mu}}{{\mathit \tau}}{{\mathit \tau}}$ , and ${{\mathit e}^{\pm}}{{\mathit \mu}^{\pm}}$ in $8.6 - 9.7$ fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The search is sensitive to ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ production with ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ , ${{\mathit Z}}{{\mathit Z}^{(*)}}$ , decaying to leptonic final states. A limit on cross section times branching ratio which corresponds to ($2.4 - 13.0$) times the expected cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 200$ GeV at 95$\%$ CL.
8  ABAZOV 2013L combine all D0 results with up to 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV.
9  CHATRCHYAN 2013AL search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 5.1 fb${}^{-1}$ and 5.3 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 and 8 TeV.
10  AAD 2012N search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ with 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 150$ GeV.
11  AALTONEN 2012AN search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ with 10 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV.
12  CHATRCHYAN 2012AO use data from CHATRCHYAN 2012G, CHATRCHYAN 2012E, CHATRCHYAN 2012H, CHATRCHYAN 2012I, CHATRCHYAN 2012D, and CHATRCHYAN 2012C.
13  AALTONEN 2009AB search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 3.0 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $70 - 150$ GeV. Associated ${{\mathit H}^{0}}{{\mathit W}}$ , ${{\mathit H}^{0}}{{\mathit Z}}$ production and ${{\mathit W}}{{\mathit W}}$ , ${{\mathit Z}}{{\mathit Z}}$ fusion are considered.
14  ABAZOV 2008U search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $70 - 150$ GeV. Associated ${{\mathit H}^{0}}{{\mathit W}}$ , ${{\mathit H}^{0}}{{\mathit Z}}$ production and ${{\mathit W}}{{\mathit W}}$ , ${{\mathit Z}}{{\mathit Z}}$ fusion are considered. See their Tab. 1 for the limit on $\sigma \cdot{}$B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ ), and see their Fig. 3 for the excluded region in the ${\mathit m}_{{{\mathit H}^{0}}}$ $-$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ ) plane.
15  SCHAEL 2007 search for Higgs bosons in association with a fermion pair and decaying to ${{\mathit W}}{{\mathit W}^{*}}$ . The limit is from this search and HEISTER 2002L for a ${{\mathit H}^{0}}$ with SM production cross section.
16  Search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance with a ${{\mathit Z}}~$boson, followed by ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ , or ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , at $\mathit E_{{\mathrm {cm}}}{}\leq{}$209 GeV. The limit is for a ${{\mathit H}^{0}}$ with SM production cross section.
18  ACHARD 2003C search for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit H}^{0}}$ followed by ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ or ${{\mathit Z}}{{\mathit Z}^{*}}$ at $\mathit E_{{\mathrm {cm}}}$= 200-209 GeV and combine with the ACHARD 2002C result. The limit is for a ${{\mathit H}^{0}}$ with SM production cross section. For B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) + B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ ) = 1, m$_{{{\mathit H}^{0}}}$ $>$ 108.1 GeV is obtained. See fig.$~$6 for the limits under different BR assumptions.
19  For B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )=1, ${\mathit m}_{{{\mathit H}^{0}}}>$117 GeV is obtained.
20  ACHARD 2002C search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance with a ${{\mathit Z}}$ boson, followed by ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ , or ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , at $\mathit E_{{\mathrm {cm}}}{}\leq{}$209 GeV. The limit is for a ${{\mathit H}^{0}}$ with SM production cross section. For B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )=1, ${\mathit m}_{{{\mathit H}^{0}}}>$114 GeV is obtained.
21  AFFOLDER 2001H search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance and a ${{\mathit W}}$ or ${{\mathit Z}}$ (tagged by two jets, an isolated lepton, or missing $\mathit E_{\mathit T}$). The limit assumes Standard Model values for the production cross section and for the couplings of the ${{\mathit H}^{0}}$ to ${{\mathit W}}$ and ${{\mathit Z}}$ bosons. See their Fig.$~$11 for limits with B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )$<1$.
22  ACCIARRI 2000S search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance with a ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , or ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ pair in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ collisions at $\mathit E_{{\mathrm {cm}}}$= $189~$GeV. The limit is for a ${{\mathit H}^{0}}$ with SM production cross section. For B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )=1, ${\mathit m}_{{{\mathit H}^{0}}}>98~$GeV is obtained. See their Fig.$~$5 for limits on B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )$\cdot{}\sigma\mathrm {( {{\mathit e}^{+}} {{\mathit e}^{-}} \rightarrow {{\mathit H}} {{\mathit f}} {{\overline{\mathit f}}} )}/\sigma\mathrm {( {{\mathit e}^{+}} {{\mathit e}^{-}} \rightarrow {{\mathit H}} {{\mathit f}} {{\overline{\mathit f}}} )}$ (SM).
23  BARATE 2000L search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance with a ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , or ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ pair in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ collisions at $\mathit E_{{\mathrm {cm}}}$= $88 - 202~$GeV. The limit is for a ${{\mathit H}^{0}}$ with SM production cross section. For B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )=1, ${\mathit m}_{{{\mathit H}^{0}}}>109~$GeV is obtained. See their Fig.$~$3 for limits on B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )$\cdot{}\sigma\mathrm {( {{\mathit e}^{+}} {{\mathit e}^{-}} \rightarrow {{\mathit H}} {{\mathit f}} {{\overline{\mathit f}}} )}/\sigma\mathrm {( {{\mathit e}^{+}} {{\mathit e}^{-}} \rightarrow {{\mathit H}} {{\mathit f}} {{\overline{\mathit f}}} )}$ (SM).
24  search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance with a ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , or ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ pair in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ collisions at 189 GeV. The limit is for a ${{\mathit H}^{0}}$ with SM production cross section. See their Fig.$~$4 for limits on $\sigma\mathrm {( {{\mathit e}^{+}} {{\mathit e}^{-}} \rightarrow {{\mathit H}^{0}} {{\mathit Z}^{0}} )}{\times }$B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )${\times }$B( ${{\mathit X}^{0}}$ $\rightarrow$ ${{\mathit f}}{{\overline{\mathit f}}}$ ) for various masses. Updates the results of ACKERSTAFF 1998Y.
25  ABBOTT 1999B search for associated production of a ${{\mathit \gamma}}{{\mathit \gamma}}$ resonance and a dijet pair. The limit assumes Standard Model values for the production cross section and for the couplings of the ${{\mathit H}^{0}}$ to ${{\mathit W}}$ and ${{\mathit Z}}$ bosons. Limits in the range of ${\mathit \sigma (}{{\mathit H}^{0}}+{{\mathit Z}}/{{\mathit W}}{)}\cdot{}$B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )= $0.80 - 0.34~$pb are obtained in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$= $65 - 150$ GeV.
26  ABREU 1999P search for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit \gamma}}$ with ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ or ${{\mathit \gamma}}{{\mathit \gamma}}$ , and ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit q}}{{\overline{\mathit q}}}$ with ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ . See their Fig.$~$4 for limits on $\sigma {\times }$B. Explicit limits within an effective interaction framework are also given.
References:
 AALTONEN 2013L
PR D88 052013 Combination of Searches for the Higgs Boson Using the Full CDF Data Set
 AALTONEN 2013M
PR D88 052014 Higgs Boson Studies at the Tevatron
 AALTONEN 2013K
PR D88 052012 Searches for the Higgs Boson Decaying to ${{\mathit W}^{+}}$ ${{\mathit W}^{-}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \nu}}{{\mathit \ell}^{-}}{{\overline{\mathit \nu}}}$ with the CDF II Detector
 ABAZOV 2013I
PR D88 052008 Search for the Standard Model Higgs Boson in ${{\mathit \ell}}{{\mathit \nu}}$ + Jets Final States in 9.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions with the ${D0}$ Detector
 ABAZOV 2013H
PR D88 052007 Search for a Higgs Boson in Diphoton Final States with the ${D0}$ Detector in 9.6 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2013G
PR D88 052006 Search for Higgs Boson Production in Oppositely Charged Dilepton and Missing Energy Final States in 9.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2013L
PR D88 052011 Combined Search for the Higgs Boson with the ${D0}$ Experiment
 ABAZOV 2013J
PR D88 052009 Search for Higgs Boson Production in Trilepton and Like-Charge Electron-Muon Final States with the ${D0}$ Detector
 CHATRCHYAN 2013AL
PL B725 36 Searches for Higgs Bosons in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV in the Context of Four-Generation and Fermiophobic Models
EPJ C72 2157 Search for a Fermiophobic Higgs Boson in the Diphoton Decay Channel with the ATLAS Detector
 AALTONEN 2012AN
PL B717 173 Search for a Higgs Boson in the Diphoton Final State using the Full CDF Data Set from ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 CHATRCHYAN 2012AO
JHEP 1209 111 Search for a Fermiophobic Higgs Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 AALTONEN 2009AB
PRL 103 061803 Search for a Fermiophobic Higgs Boson Decaying into Diphotons in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96$~$TeV
 ABAZOV 2008U
PRL 101 051801 Search for Decay of a Fermiophobic Higgs Boson ${{\mathit h}_{{f}}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ with the ${D0}$ Detector at $\sqrt {s }$ = 1.96 TeV
 SCHAEL 2007
EPJ C49 439 Search for Higgs Bosons Decaying to ${{\mathit W}}{{\mathit W}}$ in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collisions
 ABDALLAH 2004L
EPJ C35 313 Search for Fermiophobic Higgs Bosons in Final States with Photons at LEP 2
 ACHARD 2003C
PL B568 191 Search for a Higgs Boson Decaying to Weak Boson Pairs at LEP
 ABBIENDI 2002F
PL B544 44 Search for Associated Production on Massive States Decaying into Two Photons in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Annihilations at $\sqrt {s }$ = 88-GeV to 209-GeV
 ACHARD 2002C
PL B534 28 Search for a Higgs Boson Decaying into Two Photons at LEP
 AFFOLDER 2001H
PR D64 092002 Search for Narrow Diphoton Resonances and for ${{\mathit \gamma}}{{\mathit \gamma}}$ + ${{\mathit W}}/{{\mathit Z}}$ Signatures in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV
 ACCIARRI 2000S
PL B489 115 Search for a Higgs Boson Decaying into Two Photons in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Interactions at $\sqrt {s }$ = 189 GeV
 BARATE 2000L
PL B487 241 Search for ${{\mathit \gamma}}{{\mathit \gamma}}$ Decays of a Higgs Boson Produced in Association with a Fermion Pair in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collisions at LEP
 ABBIENDI 1999O
PL B464 311 Search for Higgs Boson and Other Massive States Decaying into Two Photons in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collisions at 189 GeV
 ABBOTT 1999B
PRL 82 2244 Search for High Mass Photon Pairs in ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ Events at $\sqrt {s }$ = 1.8 TeV
 ABREU 1999P
PL B458 431 Search for the Higgs Boson in Events with Isolated Photons at LEP II