# Direct Mass Limits for ${{\boldsymbol H}^{0}}$ INSPIRE search

The mass limits shown below apply to a Higgs boson ${{\mathit H}^{0}}$ with Standard Model couplings whose mass is a priori unknown. These mass limits are compatible with and independent of the observed signal at about 125 GeV. In particular, the symbol ${{\mathit H}^{0}}$ employed below does not in general refer to the observed signal at about 125 GeV.

The cross section times branching ratio limits quoted in the footnotes below are typically given relative to those of a Standard Model Higgs boson of the relevant mass. These limits can be reinterpreted in terms of more general models (e.g.$~$extended Higgs sectors) in which the Higgs couplings to ${{\mathit W}}$, ${{\mathit Z}}$ and fermions are re-scaled from their Standard Model values.

All data that have been superseded by newer results are marked as not used'' or have been removed from this compilation, and are documented in previous editions of this $\mathit Review$ of Particle Physics.

VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$\bf{ \text{> 122 and none 128 - 1000}}$ OUR EVALUATION
$\mathbf {\text{none } 145 - 1000}$ 95 1
 2015 AW
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ combined
$\text{none 90 - 102, 149 - 172}$ 95 2
 2013 L
CDF ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , combined
$\text{none 90 - 109, 149 - 182}$ 95 3
 2013 M
TEVA Tevatron combined
$\text{none 90 - 101, 157 - 178}$ 95 4
 2013 L
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , combined
$\mathbf {\text{none } 110 - 121.5}, \mathbf {128 - 145}$ 95 5
 2012 N
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ combined
$>114.1$ 95 6
 2004
DLPH ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$
$>112.7$ 95 6
 2003 B
OPAL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$
$\bf{>114.4}$ 95 7, 6
 2003 D
LEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$
$>111.5$ 95 6, 8
 2002
ALEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$
$>112.0$ 95 6
 2001 C
L3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$\text{none 132 - 200}$ 95 9
 2015 AA
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
10
 2015 G
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
11
 2014 AS
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \mu}}{{\mathit \mu}}$
12
 2014 J
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \gamma}}$
$\text{none 114.5 - 119, 129.5 - 832}$ 95 13
 2014 AA
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ 4 ${{\mathit \ell}}$
14
 2014 AI
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
$\text{none 127 - 600}$ 95 15
 2014 G
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
16
 2013 B
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
17
 2013 C
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
$\text{none }$ 95 18
 2013 K
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
19
 2013 E
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 4${{\mathit \ell}}$
20
 2013 F
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit \ell}}{{\mathit \tau}}{{\mathit j}}{{\mathit j}}$
$\text{none 159 - 176}$ 95 21
 2013 G
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
22
 2013 H
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
23
 2013 I
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit \ell}}{{\mathit \nu}}{{\mathit j}}{{\mathit j}}$
24
 2013 J
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , leptonic
25
 2013 K
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}{{\mathit X}}$
26
 2013 AL
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}$ , ${{\mathit W}}{{\mathit W}^{(*)}}$ , ${{\mathit Z}}{{\mathit Z}^{(*)}}$
27
 2013 BK
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \gamma}}$
$\text{none 145 - 710}$ 95 28
 2013 Q
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ combined
29
 2013 X
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit t}}{{\overline{\mathit t}}}{{\mathit X}}$
$\text{none 113 - 122, 128 - 133, 138 - 149}$ 95 30
 2013 Y
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 130 - 164, 170 - 180}$ 95 31
 2013 Y
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$
$\text{none 129 - 160}$ 95 32
 2013 Y
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$
$\text{none 111 - 122, 131 - 559}$ 95 33
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ combined
$\text{none 133 - 261}$ 95 34
 2012 AJ
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
35
 2012 BU
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$\text{none 319 - 558}$ 95 36
 2012 BZ
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$
$\text{none 300 - 322, 353 - 410}$ 95 37
 2012 CA
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$
38
 2012 CN
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
39
 2012 CO
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$
$\text{none 134 - 156, 182 - 233, 256 - 265, 268 - 415}$ 95 40
 2012 D
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$
$\text{none 113 - 115, 134.5 - 136}$ 95 41
 2012 G
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
42
 2012 AK
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit t}}{{\overline{\mathit t}}}{{\mathit X}}$
43
 2012 AM
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , inclusive 4${{\mathit \ell}}$
44
 2012 AN
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
45
 2012 J
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}$
46
 2012 Q
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
$\text{none 100 - 106}$ 95 47
 2012 T
TEVA ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
48
 2012 K
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
49, 50
 2012 AY
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}{{\mathit X}}$ , ${{\mathit H}^{0}}{{\mathit Z}}{{\mathit X}}$
51
 2012 C
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$
52
 2012 D
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$
$\text{none 129 - 270}$ 95 53
 2012 E
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
54
 2012 F
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}{{\mathit X}}$ , ${{\mathit H}^{0}}{{\mathit Z}}{{\mathit X}}$
$\text{none 128 - 132}$ 95 55
 2012 G
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$\text{none 134 - 158, 180 - 305, 340 - 465}$ 95 56
 2012 H
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$
$\text{none 270 - 440}$ 95 57
 2012 I
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$
58
 2012 K
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
59
 2011 G
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
60
 2011 J
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$
$\text{none 162 - 166}$ 95 61
 2010 F
TEVA ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
62
 2010 M
TEVA ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit g}}{{\mathit g}}{{\mathit X}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
63
 2009 A
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$
64
 2009 U
D0 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
65
 2006
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$
66
 2006 O
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$
1  KHACHATRYAN 2015AW search for ${{\mathit H}^{0}}$ production in the decays ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}}$ , and ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ , ${{\mathit \ell}}$ ${{\mathit \ell}}{{\mathit \tau}}{{\mathit \tau}}$ , ${{\mathit \ell}}$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \nu}}$ , and ${{\mathit \ell}}{{\mathit \ell}}{{\mathit q}}{{\mathit q}}$ in up to 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 19.7 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$=8 TeV in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $145 - 1000$ GeV. See their Fig. 7 for limits on cross section times branching ratio.
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. A limit on cross section times branching ratio which corresponds to ($0.45 - 4.8$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 200$ GeV at 95 $\%$CL. An excess of events over background is observed with a local significance of 2.0 $\sigma$ at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 124 and 203 GeV are excluded at 95$\%$ CL.
3  AALTONEN 2013M combine all Tevatron data from the CDF and D0 Collaborations. A limit on cross section times branching ratio which corresponds to ($0.37 - 3.1$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 200$ GeV at 95$\%$ CL. An excess of events over background is observed with a local significance of 3.0$\sigma$ at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 121 and 225 GeV are excluded at 95$\%$ CL.
4  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. A limit on cross section times branching ratio which corresponds to ($0.66 - 3.1$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 200$ GeV at 95$\%$ CL. An excess of events over background is observed with a local significance of 1.7$\sigma$ at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 125 and 218 GeV are excluded at 95$\%$ CL.
5  CHATRCHYAN 2012N search for ${{\mathit H}^{0}}$ production in the decays ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit Z}}$ ${{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ , ${{\mathit W}}$ ${{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit \tau}}{{\mathit \tau}}$ , and ${{\mathit b}}{{\overline{\mathit b}}}$ in $4.9 - 5.1$ fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and $5.1 - 5.3$ fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The expected exclusion region for no signal is $110 - 145$ GeV at 99.9$\%$ CL. See also CHATRCHYAN 2013Y.
6  Search for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit Z}}$ at $\mathit E_{{\mathrm {cm}}}{}\leq{}$209 GeV in the final states ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ with ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ and ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ with ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ .
7  Combination of the results of all LEP experiments.
8  A 3$\sigma$ excess of candidate events compatible with ${\mathit m}_{{{\mathit H}^{0}}}$ near 114$~$GeV is observed in the combined channels ${{\mathit q}}{{\overline{\mathit q}}}{{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit q}}{{\overline{\mathit q}}}{{\mathit \ell}}{{\overline{\mathit \ell}}}$ , ${{\mathit q}}{{\overline{\mathit q}}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ .
9  AAD 2015AA search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ in 4.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. A limit on cross section times branching ratio which corresponds to ($0.2 - 6$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 200$ GeV at 95$\%$ CL.
10  AAD 2015G search for ${{\mathit W}}{{\mathit H}^{0}}$ and ${{\mathit Z}}{{\mathit H}^{0}}$ production followed by ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ in 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. A limit on the cross section times branching ratio which corresponds to ($0.8 - 2.6$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 140$ GeV at 95$\%$ CL.
11  AAD 2014AS search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in 4.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. A limit on the cross section times branching ratio which corresponds to ($6.5 - 16.8$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 150$ GeV at 95$\%$ CL.
12  AAD 2014J search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \gamma}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \gamma}}$ in 4.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. A limit on cross section times branching ratio which corresponds to ($4 - 18$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 150$ GeV at 95$\%$ CL.
13  CHATRCHYAN 2014AA search for ${{\mathit H}^{0}}$ production in the decay mode ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ in 5.1 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. The expected exclusion region for no signal is $115 - 740$ GeV at the 95$\%$ CL. See their Fig. 18 for cross section limits for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 1000$ GeV.
14  CHATRCHYAN 2014AI search for ${{\mathit W}}{{\mathit H}^{0}}$ and ${{\mathit Z}}{{\mathit H}^{0}}$ production followed by ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ in up to 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 18.9 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. A limit on the cross section times branching ratio which corresponds to ($1 - 3$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 135$ GeV at 95$\%$ CL.
15  CHATRCHYAN 2014G search for ${{\mathit H}^{0}}$ production in the decay mode ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ in 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.4 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The expected exclusion region for no signal is $115 - 600$ GeV at the 95$\%$ CL. See their Fig. 21 (left) for cross section limits for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 600$ GeV.
16  AALTONEN 2013B search for associated ${{\mathit H}^{0}}{{\mathit Z}}$ production in the final state ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , and ${{\mathit H}^{0}}{{\mathit W}}$ production in ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ (${{\mathit \ell}}$ not identified) with an improved ${{\mathit b}}$ identification algorithm in 9.45 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 ($0.72 - 11.8$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 150$ GeV at 95$\%$CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 3.06, where 3.33 is expected for no signal.
17  AALTONEN 2013C search for associated ${{\mathit H}^{0}}{{\mathit W}}$ and ${{\mathit H}^{0}}{{\mathit Z}}$ as well as vector-boson fusion ${{\mathit H}^{0}}{{\mathit q}}{{\overline{\mathit q}}^{\,'}}$ production in the final state ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit W}}$ $/$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ with 9.45 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 is ($7.0 - 64.6$) times larger than the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 9.0, where 11.0 is expected for no signal.
18  AALTONEN 2013K search for ${{\mathit H}^{0}}$ production (with a possible additional ${{\mathit W}}$ or ${{\mathit Z}}$) in the final state ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ 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 ($0.49 - 14.1$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 200$ GeV at 95$\%$ CL. The limit at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 3.26, where 3.25 is expected for no signal. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 124 and 200 GeV are excluded at 95$\%$ CL.
19  ABAZOV 2013E search for ${{\mathit H}^{0}}$ production in four-lepton final states from ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ and ${{\mathit H}^{0}}{{\mathit Z}}$ in $9.6 - 9.8$ 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 ($8.6 - 78.9$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $115 - 200$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 42.3, where 42.8 is expected for no signal.
20  ABAZOV 2013F search for ${{\mathit H}^{0}}$ production in final states ${{\mathit e}}{{\mathit \tau}}{{\mathit j}}{{\mathit j}}$ and ${{\mathit \mu}}{{\mathit \tau}}$ 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 ${{\mathit H}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}$ and ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ . A limit on cross section times branching ratio which corresponds to ($9.4 - 17.9$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $105 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 11.3, where 9.0 is expected for no signal.
21  ABAZOV 2013G search for ${{\mathit H}^{0}}$ production in final states ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \nu}}{{\mathit \ell}^{-}}{{\mathit \nu}}$ in 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV and give a limit on cross section times branching ratio for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 4.1, where 3.4 is expected for no signal. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 125 and 218 GeV are excluded at 95$\%$ CL.
22  ABAZOV 2013H search for ${{\mathit H}^{0}}$ production with the decay ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 9.6 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. A limit on cross section times branching ratio which corresponds to ($8.3 - 25.4$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 12.8, where 8.7 is expected for no signal.
23  ABAZOV 2013I search for ${{\mathit H}^{0}}$ production in the final state with one lepton and two or more jets plus missing $\mathit E_{T}$ with ${{\mathit b}}$ identification in 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The search is mainly sensitive to ${{\mathit H}^{0}}$ ${{\mathit W}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ , and ${{\mathit H}^{0}}$ ${{\mathit V}}$ $\rightarrow$ ${{\mathit V}}{{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}{{\mathit q}}{{\overline{\mathit q}}}$ (${{\mathit V}}$ = ${{\mathit W}}$, ${{\mathit Z}}$). A limit on cross section times branching ratio which corresponds to ($1.3 - 11.4$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 200$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 5.8, where 4.7 is expected for no signal. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 150 and 188 GeV are excluded at 95$\%$ CL.
24  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 ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ and gluon fusion production with ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ , ${{\mathit Z}}{{\mathit Z}^{(*)}}$ , decaying to leptonic final states, and to ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ production with ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ . A limit on cross section times branching ratio which corresponds to ($4.4 - 12.7$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 200$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 8.4, where 6.3 is expected for no signal.
25  ABAZOV 2013K search for associated ${{\mathit H}^{0}}{{\mathit Z}}$ production in the final states ${{\mathit \ell}}{{\mathit \ell}}{{\mathit b}}{{\mathit b}}$ with ${{\mathit b}}$ identification 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 ($1.8 - 53$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 7.1, where 5.1 is expected for no signal.
26  CHATRCHYAN 2013AL search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ , ${{\mathit W}}{{\mathit W}^{(*)}}$ , and ${{\mathit Z}}{{\mathit Z}^{(*)}}$ 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. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 110 and 600 GeV are excluded at 99$\%$ CL.
27  CHATRCHYAN 2013BK search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \gamma}}$ $\rightarrow$ ${{\mathit \ell}}$ ${{\mathit \ell}}{{\mathit \gamma}}$ in 5.0 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.6 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. A limit on cross section times branching ratio which corresponds to ($4 - 25$) times the expected Standard Model cross section is given in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 160$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 9.5, where 10 is expected for no signal.
28  CHATRCHYAN 2013Q search for ${{\mathit H}^{0}}$ production in the decays ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}}$ and ${{\mathit H}^{0}}$ $\rightarrow$ $\rightarrow$ 4 ${{\mathit \ell}}$ , ${{\mathit \ell}}$ ${{\mathit \ell}}{{\mathit \tau}}{{\mathit \tau}}$ , ${{\mathit \ell}}$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \nu}}$ , and ${{\mathit \ell}}{{\mathit \ell}}{{\mathit q}}{{\mathit q}}$ in up to 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 5.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV in the range ${\mathit m}_{{{\mathit H}^{0}}}$ = $145 - 1000$ GeV. Superseded by KHACHATRYAN 2015AW.
29  CHATRCHYAN 2013X search for ${{\mathit H}^{0}}{{\mathit t}}{{\overline{\mathit t}}}$ production followed by ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , one top decaying to ${{\mathit \ell}}{{\mathit \nu}}$ and the other to either ${{\mathit \ell}}{{\mathit \nu}}$ or ${{\mathit q}}{{\overline{\mathit q}}}$ in 5.0 fb${}^{-1}$ and 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 and 8 TeV. A limit on cross section times branching ratio which corresponds to ($4.0 - 8.6$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 140$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 5.8, where 5.2 is expected for no signal.
30  CHATRCHYAN 2013Y search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 5.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The expected exclusion region for no signal is $110 - 144$ GeV at 95$\%$ CL.
31  CHATRCHYAN 2013Y search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ in 5.0 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 5.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The expected exclusion region for no signal is $120 - 180$ GeV at 95$\%$ CL.
32  CHATRCHYAN 2013Y search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ in 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 5.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The expected exclusion region for no signal is $122 - 160$ GeV at 95$\%$ CL.
33  AAD 2012AI search for ${{\mathit H}^{0}}$ production in ${{\mathit p}}{{\mathit p}}$ collisions for the final states ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ , ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}{{\mathit W}^{(*)}}$ , ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit \tau}}{{\mathit \tau}}$ with 4.6--4.8 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV, and ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ , ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}$ ${{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ with $5.8 - 5.9$ fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The 99$\%$ CL excluded range is $113 - 114$, $117 - 121$, and $132 - 527$ GeV. An excess of events over background with a local significance of 5.9 $\sigma$ is observed at ${\mathit m}_{{{\mathit H}^{0}}}$ = 126 GeV.
34  AAD 2012AJ search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which corresponds to ($0.2 - 10$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 600$ GeV at 95$\%$ CL.
35  AAD 2012BU search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is ($2.9 - 11.7$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL.
36  AAD 2012BZ search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \nu}}{{\overline{\mathit \nu}}}$ with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which corresponds to (0.2--4) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $200 - 600$ GeV at 95$\%$ CL.
37  AAD 2012CA search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit q}}{{\overline{\mathit q}}}$ with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which corresponds to (0.7--9) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $200 - 600$ GeV at 95$\%$ CL.
38  AAD 2012CN search for associated ${{\mathit H}^{0}}{{\mathit W}}$ and ${{\mathit H}^{0}}{{\mathit Z}}$ production in the channels ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , and ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is ($2.5 - 5.5$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 130$ GeV at 95$\%$ CL.
39  AAD 2012CO search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ with 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is (1.9--10) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $300 - 600$ GeV at 95$\%$ CL.
40  AAD 2012D search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ in 4.8 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 600$ GeV. An excess of events over background with a local significance of 2.1 ${{\mathit \sigma}}$ is observed at 125 GeV.
41  AAD 2012G search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 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. An excess of events over background with a local significance of 2.8 ${{\mathit \sigma}}$ is observed at 126.5 GeV.
42  AALTONEN 2012AK search for associated ${{\mathit H}^{0}}{{\mathit t}}{{\overline{\mathit t}}}$ production in the decay chain ${{\mathit t}}$ ${{\overline{\mathit t}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}{{\mathit b}}{{\mathit b}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}}{{\mathit b}}{{\mathit b}}$ with 9.45 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 is ($10 - 40$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 20.5, where 12.6 is expected.
43  AALTONEN 2012AM search for ${{\mathit H}^{0}}$ production in inclusive four-lepton final states coming from ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}{{\mathit \ell}}{{\mathit \ell}}$ , or ${{\mathit H}^{0}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}{{\mathit \ell}}{{\mathit \ell}}$ , with 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 is ($7.2 - 42.4$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 300$ GeV at 95$\%$ CL. The best limit is for ${\mathit m}_{{{\mathit H}^{0}}}$ = 200 GeV.
44  AALTONEN 2012AN search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ with 10 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. A limit on cross section times branching ratio which is (7.7--21.3) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 17.0, where 9.9 is expected.
45  AALTONEN 2012J search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ (one leptonic, the other hadronic) with 6.0 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 is ($14.6 - 70.2$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The best limit is for ${\mathit m}_{{{\mathit H}^{0}}}$ = 120 GeV.
46  AALTONEN 2012Q search for associated ${{\mathit H}^{0}}{{\mathit Z}}$ production in the final state ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ with 9.45 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 ($1.0 - 37.5$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $90 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 7.1, where 3.9 is expected. A broad excess of events for ${\mathit m}_{{{\mathit H}^{0}}}$ $>$ 110 GeV is observed, with a local significance of 2.4 $\sigma$ at ${\mathit m}_{{{\mathit H}^{0}}}$ = 135 GeV.
47  AALTONEN 2012T combine AALTONEN 2012Q, AALTONEN 2012R, AALTONEN 2012S, ABAZOV 2012O, ABAZOV 2012P, and ABAZOV 2012K. An excess of events over background is observed which is most significant in the region ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 135$ GeV, with a local significance of up to 3.3 $\sigma$. The local significance at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 2.8 $\sigma$, which corresponds to ($\sigma$( ${{\mathit H}^{0}}{{\mathit W}}$ ) + $\sigma$( ${{\mathit H}^{0}}{{\mathit Z}}$ )) B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ )) = ($0.23$ ${}^{+0.09}_{-0.08}$) pb, compared to the Standard Model expectation at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV of $0.12$ $\pm0.01$ pb.
48  ABAZOV 2012K search for associated ${{\mathit H}^{0}}{{\mathit Z}}$ production in the final state ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , and ${{\mathit H}^{0}}{{\mathit W}}$ production with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ (${{\mathit \ell}}$ not identified) with 9.5 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 is ($1.9 - 16.8$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $100 - 150$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 4.3, where 3.9 is expected.
49  CHATRCHYAN 2012AY search for associated ${{\mathit H}^{0}}{{\mathit W}}$ and ${{\mathit H}^{0}}{{\mathit Z}}$ production in the channels ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ , and ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}$ , ${{\mathit W}}{{\mathit W}^{(*)}}$ , with 5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is ($3.1 - 9.1$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 200$ GeV at 95$\%$ CL.
50  CHATRCHYAN 2012AY combine CHATRCHYAN 2012F and CHATRCHYAN 2012AO in addition and give a limit on cross section times branching ratio which is ($2.1 - 3.7$) times larger than the expected Standard Model cross section for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 170$ GeV at 95$\%$ CL. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 3.3.
51  CHATRCHYAN 2012C search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in 4.7$~$fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is ($4 - 12$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $190 - 600$ GeV at 95$\%$ CL. The best limit is at ${\mathit m}_{{{\mathit H}^{0}}}$ = 200 GeV.
52  CHATRCHYAN 2012D search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit q}}{{\overline{\mathit q}}}$ in 4.6$~$fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which corresponds to ($1 - 22$) times the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $130 - 164$ GeV, $200 - 600$ GeV at 95$\%$ CL. The best limit is at ${\mathit m}_{{{\mathit H}^{0}}}$ = 230 GeV. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values in the ranges ${\mathit m}_{{{\mathit H}^{0}}}$ = $154 - 161$ GeV and $200 - 470$ GeV are excluded at 95$\%$ CL.
53  CHATRCHYAN 2012E search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \nu}}{{\mathit \ell}^{-}}{{\overline{\mathit \nu}}}$ in 4.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 600$ GeV.
54  CHATRCHYAN 2012F search for associated ${{\mathit H}^{0}}{{\mathit W}}$ and ${{\mathit H}^{0}}{{\mathit Z}}$ production followed by ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ , and ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , in 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is ($3.1 - 9.0$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 135$ GeV at 95$\%$ CL. The best limit is at ${\mathit m}_{{{\mathit H}^{0}}}$ = 110 GeV.
55  CHATRCHYAN 2012G search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 4.8 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. An excess of events over background with a local significance of 3.1 ${{\mathit \sigma}}$ is observed at 124 GeV.
56  CHATRCHYAN 2012H search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{(*)}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ in 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 600$ GeV. Excesses of events over background are observed around 119, 126 and 320 GeV. The region ${\mathit m}_{{{\mathit H}^{0}}}$ = $114.4 - 134$ GeV remains consistent with the expectation for the production of a SM-like Higgs boson.
57  CHATRCHYAN 2012I search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \nu}}{{\overline{\mathit \nu}}}$ in 4.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV in the mass range ${\mathit m}_{{{\mathit H}^{0}}}$ = $250 - 600$ GeV.
58  CHATRCHYAN 2012K search for ${{\mathit H}^{0}}$ production in the decay ${{\mathit H}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ with 4.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. A limit on cross section times branching ratio which is ($3.2 - 7.0$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 145$ GeV at 95$\%$ CL.
59  ABAZOV 2011G search for ${{\mathit H}^{0}}$ production in 5.4 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV in the decay mode ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}^{\,'}}$ (and processes with similar final states). A limit on cross section times branching ratio which is ($3.9 - 37$) times larger than the expected Standard Model cross section is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $115 - 200$ GeV at 95$\%$ CL. The best limit is at ${\mathit m}_{{{\mathit H}^{0}}}$ = 160 GeV.
60  CHATRCHYAN 2011J search for ${{\mathit H}^{0}}$ production with ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \nu}}{{\mathit \nu}}$ in 36 pb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. See their Fig. 6 for a limit on cross section times branching ratio for ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 600$ GeV at 95$\%$ CL. In the Standard Model with an additional generation of heavy quarks and leptons which receive their masses via the Higgs mechanism, ${\mathit m}_{{{\mathit H}^{0}}}$ values between 144 and 207 GeV are excluded at 95$\%$ CL.
61  AALTONEN 2010F combine searches for ${{\mathit H}^{0}}$ decaying to ${{\mathit W}^{+}}{{\mathit W}^{-}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with 4.8 fb${}^{-1}$ (CDF) and 5.4 fb${}^{-1}$ (${D0}$).
62  AALTONEN 2010M combine searches for ${{\mathit H}^{0}}$ decaying to ${{\mathit W}^{+}}{{\mathit W}^{-}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with 4.8 fb${}^{-1}$ (CDF) and 5.4 fb${}^{-1}$ (${D0}$) and derive limits ${\mathit \sigma (}$ ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{)}\cdot{}$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$ ) $<$ ($1.75 - 0.38$) pb for ${\mathit m}_{{{\mathit H}}}$ = $120 - 165$ GeV, where ${{\mathit H}^{0}}$ is produced in ${{\mathit g}}{{\mathit g}}$ fusion. In the Standard Model with an additional generation of heavy quarks, ${\mathit m}_{{{\mathit H}^{0}}}$ between 131 and 204 GeV is excluded at 95$\%$ CL.
63  AALTONEN 2009A search for ${{\mathit H}^{0}}$ production in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ =1.96 TeV in the decay mode ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \nu}}{{\overline{\mathit \nu}}}$ . A limit on ${\mathit \sigma (}{{\mathit H}^{0}}{)}$ $\cdot{}$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{(*)}}$ ) between 0.7 and 2.5 pb (95$\%$ CL) is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $110 - 200$ GeV, which is $1.7 - 45$ times larger than the expected Standard Model cross section. The best limit is obtained for ${\mathit m}_{{{\mathit H}^{0}}}$ = 160 GeV.
64  ABAZOV 2009U search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ with ${{\mathit \tau}}$ $\rightarrow$ hadrons in 1 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The production mechanisms include associated +${{\mathit H}^{0}}$ production, weak boson fusion, and gluon fusion. A limit (95$\%$ CL) is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $105 - 145$ GeV, which is $20 - 82$ times larger than the expected Standard Model cross section. The limit for ${\mathit m}_{{{\mathit H}^{0}}}$ = 115 GeV is 29 times larger than the expected Standard Model cross section.
65  ABAZOV 2006 search for Higgs boson production in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with the decay chain ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \nu}}{{\mathit \ell}^{'\mp}}{{\overline{\mathit \nu}}}$ . A limit ${{\mathit \sigma}}({{\mathit H}^{0}})\cdot{}$B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) $<$ ($5.6 - 3.2$) pb (95 $\%$CL) is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 200$ GeV, which far exceeds the expected Standard Model cross section.
66  ABAZOV 2006O search for associated ${{\mathit H}^{0}}{{\mathit W}}$ production in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with the decay ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ , in the final states ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{'\mp}}{{\mathit \nu}}{{\mathit \nu}^{\,'}}{{\mathit X}}$ where ${{\mathit \ell}}$ = ${{\mathit e}}$, ${{\mathit \mu}}$. A limit ${\mathit \sigma (}$ ${{\mathit H}^{0}}{{\mathit W}}{)}\cdot{}$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) $<$ ($3.2 - 2.8$) pb (95 $\%$CL) is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = $115 - 175$ GeV, which far exceeds the expected Standard Model cross section.
References:
PR D92 012006 Observation and Measurement of Higgs Boson Decays to ${{\mathit W}}{{\mathit W}^{*}}$ with the ATLAS Detector
JHEP 1501 069 Search for the ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Decay of the Standard Model Higgs Boson in Associated (${{\mathit W}}/{{\mathit Z}}){{\mathit H}}$ Production with the ATLAS Detector
 KHACHATRYAN 2015AW
JHEP 1510 144 Search for a Higgs Boson in the Mass Range from 145 to 1000 GeV Decaying to a Pair of ${{\mathit W}}$ or ${{\mathit Z}}$ Bosons
PL B738 68 Search for the Standard Model Higgs Boson Decay to ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ with the ATLAS Detector
PL B732 8 Search for Higgs Boson Decays to a Photon and a ${{\mathit Z}}$ Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV with the ATLAS Detector
 CHATRCHYAN 2014AA
PR D89 092007 Measurement of the Properties of a Higgs Boson in the Four-Lepton Final State
 CHATRCHYAN 2014AI
PR D89 012003 Search for the Standard Model Higgs Boson Produced in Association with a ${{\mathit W}}$ or a ${{\mathit Z}}$ Boson and Decaying to Bottom Quarks
 CHATRCHYAN 2014G
JHEP 1401 096 Measurement of Higgs Boson Production and Properties in the ${{\mathit W}}{{\mathit W}}$ Decay Channel with Leptonic Final States
 AALTONEN 2013C
JHEP 1302 004 Search for the Higgs Boson in the All-Hadronic Final State using the Full CDF Data Set
 AALTONEN 2013M
PR D88 052014 Higgs Boson Studies at the Tevatron
 AALTONEN 2013L
PR D88 052013 Combination of Searches for the Higgs Boson Using the Full CDF Data Set
 AALTONEN 2013B
PR D87 052008 Updated Search for the Standard Model Higgs Boson in Events with Jets and Missing Transverse Energy using the Full CDF Data Set
 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 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
 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 2013K
PR D88 052010 Search for ${{\mathit Z}}$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit b}}{{\overline{\mathit b}}}$ Production 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 2013F
PR D88 052005 Search for the Higgs Boson in lepton, tau and Jets Final States
 ABAZOV 2013E
PR D88 032008 Measurement of the ${{\mathit Z}}{{\mathit Z}}$ Production Cross Section and Search for the Standard Model Higgs Boson in the Four Lepton Final State in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions
 CHATRCHYAN 2013Q
EPJ C73 2469 Search for a Standard-Model-Like Higgs Boson with a Mass in the Range 145 to 1000 GeV at the LHC
 CHATRCHYAN 2013BK
PL B726 587 Search for a Higgs Boson Decaying into a ${{\mathit Z}}$ and a Photon in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV
 CHATRCHYAN 2013X
JHEP 1305 145 Search for the Standard Model Higgs Boson Produced in Association with a Top-Quark Pair in ${{\mathit p}}{{\mathit p}}$ Collisions at the LHC
 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
 CHATRCHYAN 2013Y
JHEP 1306 081 Observation of a New Boson with Mass Near 125 GeV in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV
PL B716 62 Search for the Standard Model Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{{(*)}}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ Decay Mode with 4.7 ${\mathrm {fb}}{}^{-1}$ of ATLAS Data at $\sqrt {s }$ = 7 TeV
PL B718 391 Search for the Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit j}}{{\mathit j}}$ Decay Channel at $\sqrt {s }$ = 7 TeV with the ATLAS Detector
JHEP 1209 070 Search for the Standard Model Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ Decay Mode in $\sqrt {s }$ = 7 TeV ${{\mathit p}}{{\mathit p}}$ Collisions with ATLAS
PL B716 1 Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector at the LHC
PRL 108 111803 Search for the Standard Model Higgs Boson in the Diphoton Decay Channel with 4.9$~{\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 7$~$TeV with ATLAS
PL B717 29 Search for a Standard Model Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ ${{\mathit \ell}^{-}}{{\mathit \nu}}{{\overline{\mathit \nu}}}$ Decay Channel using 4.7 ${\mathrm {fb}}{}^{-1}$ of $\sqrt {s }$ = 7 TeV Data with the ATLAS Detector
PL B710 383 Search for the Standard Model Higgs Boson in the Decay Channel ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{{(*)}}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ with 4.8 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 7$~$TeV with ATLAS
PL B718 369 Search for the Standard Model Higgs Boson Produced in Association with a Vector Boson and Decaying to a ${\mathit {\mathit b}}$-Quark Pair with the ATLAS Detector
PL B717 70 Search for a Standard Model Higgs Boson in the Mass Range $200 - 600$ GeV in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ ${{\mathit \ell}^{-}}{{\mathit q}}{{\overline{\mathit q}}}$ Decay Channel with the ATLAS Detector
 AALTONEN 2012Q
PRL 109 111803 Search for the Standard Model Higgs Boson Decaying to a ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Pair in Events with Two Oppositely Charged Leptons Using the Full CDF Data Set
 AALTONEN 2012AK
PRL 109 181802 Search for the Standard Model Higgs Boson Produced in Association with Top Quarks Using the Full CDF Data Set
 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
 AALTONEN 2012T
PRL 109 071804 Evidence for a Particle Produced in Association with Weak Bosons and Decaying to a Bottom-Antibottom Quark Pair in Higgs Boson Searches at the Tevatron
 AALTONEN 2012AM
PR D86 072012 Novel Inclusive Search for the Higgs Boson in the Four-Lepton Final State at CDF
 AALTONEN 2012J
PRL 108 181804 Search for a Low-Mass Standard Model Higgs Boson in the ${{\mathit \tau}}$ $−$ ${{\mathit \tau}}$ Decay Channel in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2012K
PL B716 285 Search for the Standard Model Higgs Boson in the ${{\mathit Z}}$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit \nu}}{{\overline{\mathit \nu}}}{{\mathit b}}{{\overline{\mathit b}}}$ Channel in 9.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2012H
PRL 108 111804 Search for the Standard Model Higgs Boson in the Decay Channel ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7$~$TeV
 CHATRCHYAN 2012E
PL B710 91 Search for the Standard Model Higgs Boson Decaying to ${{\mathit W}^{+}}{{\mathit W}^{-}}$ in the Fully Leptonic Final State in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2012F
PL B710 284 Search for the Standard Model Higgs Boson Decaying to Bottom Quarks in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7$~$TeV
 CHATRCHYAN 2012D
JHEP 1204 036 Search for a Higgs Boson in the Decay Channel ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{{(*)}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit \ell}^{-}}{{\mathit \ell}^{+}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7$~$TeV
 CHATRCHYAN 2012C
JHEP 1203 081 Search for the Standard Model Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ Decay Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7$~$TeV
 CHATRCHYAN 2012N
PL B716 30 Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC
 CHATRCHYAN 2012I
JHEP 1203 040 Search for the Standard Model Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ $\rightarrow$ 2 ${{\mathit \ell}}$2 ${{\mathit \nu}}$ Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7$~$TeV
 CHATRCHYAN 2012AY
JHEP 1211 088 Search for the Standard Model Higgs Boson Produced in Association with ${{\mathit W}}$ and ${{\mathit Z}}$ Bosons in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2012G
PL B710 403 Search for the Standard Model Higgs Boson Decaying into Two Photons in ${{\mathit p}}{{\mathit p}}$ Collisions $\sqrt {s }$ = 7$~$TeV
 CHATRCHYAN 2012K
PL B713 68 Search for Neutral Higgs Bosons Decaying to tau Pairs in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 ABAZOV 2011G
PRL 106 171802 Search for the Standard Model Higgs Boson in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit d}^{\,'}}{{\overline{\mathit q}}}$ Decay Channel
 CHATRCHYAN 2011J
PL B699 25 Measurement of ${{\mathit W}^{+}}{{\mathit W}^{-}}$ Production and Search for the Higgs Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 AALTONEN 2010F
PRL 104 061802 Combination of Tevatron Searches for the Standard Model Higgs Boson in the ${{\mathit W}^{+}}{{\mathit W}^{-}}$ Decay Mode
 AALTONEN 2010M
PR D82 011102 Combined Tevatron Upper Limit on ${{\mathit g}}$ ${{\mathit g}}$ $\rightarrow$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$ and Constraints on the Higgs Boson Mass in Fourth-Generation Fermion Models
 AALTONEN 2009A
PRL 102 021802 Search for a Higgs Boson Decaying to Two ${{\mathit W}}$ Bosons at CDF
 ABAZOV 2009U
PRL 102 251801 Search for the Standard Model Higgs Boson in Tau Final States
 ABAZOV 2006
PRL 96 011801 Search for the Higgs Boson in ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}{}^{(*)}$ Decays in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ =1.96 TeV
 ABAZOV 2006O
PRL 97 151804 Search for Associated Higgs Boson Production ${{\mathit W}}$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \nu}}{{\mathit \ell}^{'\pm}}{{\mathit \nu}^{\,'}}{{\mathit X}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABDALLAH 2004
EPJ C32 145 Final Results from DELPHI on the Searches for SM and MSSM Neutral Higgs Bosons
 ABBIENDI 2003B
EPJ C26 479 Search for the Standard Model Higgs Boson with the OPAL Detector at LEP
 HEISTER 2003D
PL B565 61 Search for the Standard Model Higgs Boson at LEP
 HEISTER 2002
PL B526 191 Final Results of the Searches for Neutral Higgs Bosons in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collisions at$\sqrt {s }$ up to 209 GeV
 ACHARD 2001C
PL B517 319 Standard Model Higgs Boson with the L3 Experiment at LEP
 CHATRCHYAN 2012AO
JHEP 1209 111 Search for a Fermiophobic Higgs Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 ABAZOV 2006T
PR D74 059904(errat.) Publisher's Note to ABAZOV 2006H. Limits on Anomalous Trilinear Gauge Couplings from ${{\mathit W}}$ ${{\mathit W}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit W}}$ ${{\mathit W}}$ $\rightarrow$ ${{\mathit e}^{\pm}}{{\mathit \mu}^{\mp}}$ , and ${{\mathit W}}$ ${{\mathit W}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ Events from ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 AALTONEN 2012R
PRL 109 111804 Search for the Standard Model Higgs Boson Decaying to a ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Pair in Events with One Charged Lepton and Large Missing Transverse Energy Using the Full CDF Data Set
 AALTONEN 2012S
PRL 109 111805 Search for the Standard Model Higgs Boson Decaying to a ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Pair in Events with No Charged Leptons and Large Missing Transverse Energy using the Full CDF Data Set
 ABAZOV 2012O
PRL 109 121803 Search for the Standard Model Higgs Boson in ${{\mathit Z}}$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit b}}{{\overline{\mathit b}}}$ Production with the ${D0}$ Detector in 9.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2012P
PRL 109 121804 Search for the Standard Model Higgs Boson in Associated ${{\mathit W}}{{\mathit H}}$ Production in 9.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions with the ${D0}$ Detector