# MASS LIMITS for ${{\boldsymbol W}^{\,'}}$ (Heavy Charged Vector Boson Other Than ${{\boldsymbol W}}$) in Hadron Collider Experiments INSPIRE search

Couplings of ${{\mathit W}^{\,'}}$ to quarks and leptons are taken to be identical with those of ${{\mathit W}}$. The following limits are obtained from ${{\mathit p}}{{\overline{\mathit p}}}$ or ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}^{\,'}}$ X with ${{\mathit W}^{\,'}}$ decaying to the mode indicated in the comments. New decay channels ($\mathit e.g.$, ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ ) are assumed to be suppressed. The most recent preliminary results can be found in the ${{\mathit W}^{\,'}}$-boson searches'' review above.
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$\bf{ > 5200}$ OUR LIMIT
1
 2019 B
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$
$\text{none 500 - 3250}$ 95 2
 2019 E
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$> 6000$ 95 3
 2019 C
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$\text{none 1300 - 3600}$ 95 4
 2019 D
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 400 - 4000}$ 95 5
 2019 AY
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$
$> 4300$ 95 6
 2019 CP
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit W}}{{\mathit H}}$ , ${{\mathit \ell}}{{\mathit \nu}}$
$> 2600$ 95 7
 2019 I
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$\text{none 1000 - 3000}$ 95 8
 2018 AF
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 500 - 2820}$ 95 9
 2018 AI
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$\text{none 300 - 3000}$ 95 10
 2018 AK
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 800 - 3200}$ 95 11
 2018 AL
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$> 5100$ 95 12
 2018 BG
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$\text{none 250 - 2460}$ 95 13
 2018 CH
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 1200 - 3300}$ 95 14
 2018 F
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 500 - 3700}$ 95 15
 2018 K
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$
$\text{none 1000 - 3600}$ 95 16
 2018
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 1000 - 3050}$ 95 17
 2018 AX
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\bf{\text{none 400 - 5200}}$ 95 18
 2018 AZ
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$\text{none 1000 - 3400}$ 95 19
 2018 BK
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 600 - 3300}$ 95 20
 2018 BO
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 900 - 4400}$ 95 21
 2018 CV
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$
$\text{none 800 - 2330}$ 95 22
 2018 DJ
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$> 2800$ 95 23
 2018 ED
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$\text{none 1200 - 3200, 3300 - 3600}$ 95 24
 2018 P
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$>3600$ 95 25
 2017 AK
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 1100 - 2500}$ 95 26
 2017 AO
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$> 2220$ 95 27
 2017 B
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$> 2300$ 95 28
 2017 J
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}_{{\tau}}}$ ${{\mathit \tau}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \tau}}{{\mathit j}}{{\mathit j}}$
$\text{none 600 - 2700}$ 95 29
 2017 W
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 4100$ 95 30
 2017 Z
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$> 2200$ 95 31
 2017 A
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$>2300$ 95 32
 2017 AK
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit W}}{{\mathit H}}$
$> 2900$ 95 33
 2017 H
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit N}}$
$> 2600$ 95 34
 2017 I
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$>2450$ 95 35
 2017 R
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$\text{none 2780 - 3150}$ 95 35
 2017 R
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$> 2600$ 95 36
 2016 AE
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$> 4070$ 95 37
 2016 V
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$>1810$ 95 38
 2016 R
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$>2600$ 95 39
 2016 S
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 2150$ 95 40
 2016 AO
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 1000 - 1600}$ 95 41
 2016 AP
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$\text{none 800 - 1500}$ 95 42
 2016 BD
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \ell}}{{\mathit \nu}}$
$\text{none 1500 - 2600}$ 95 43
 2016 K
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 500 - 1600}$ 95 44
 2016 L
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 300 - 2700}$ 95 45
 2016 O
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$
$\text{none 400 - 1590}$ 95 46
 2015 AU
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 1500 - 1760}$ 95 47
 2015 AV
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 300 - 1490}$ 95 48
 2015 AZ
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 1300 - 1500}$ 95 49
 2015 CP
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 500 - 1920}$ 95 50
 2015 R
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 800 - 2450}$ 95 51
 2015 V
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 1470$ 95 52
 2015 C
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$>3710$ 95 53
 2015 T
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$\text{none 1000 - 3010}$ 95 54
 2014 O
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
55
 2019 BB
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit j}}{{\mathit \ell}}{{\mathit \ell}}$
56
 2019 V
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit B}}{{\mathit t}}$ , ${{\mathit T}}{{\mathit b}}$
57
 2018 AA
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \gamma}}$
58
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$
$> 4500$ 95 59
 2018 CJ
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit W}}{{\mathit H}}$ , ${{\mathit \ell}}{{\mathit \nu}}$
60
 2017 U
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
61
 2015 BB
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$
$\text{none 300 - 880}$ 95 62
 2015 C
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 1200 - 1900 and 2000 - 2200}$ 95 63
 2015 V
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$>3240$ 95
 2014 AI
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
64
 2014 AT
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \gamma}}$
$\text{none 200 - 1520}$ 95 65
 2014 S
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 1000 - 1700}$ 95 66
 2014
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
67
 2014 A
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 500 - 950}$ 95 68
 2013 AO
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 1100 - 1680}$ 95
 2013 D
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 1000 - 1920}$ 95
 2013 A
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
69
 2013 AJ
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$> 2900$ 95 70
 2013 AQ
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$\text{none 800 - 1510}$ 95 71
 2013 E
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 700 - 940}$ 95 72
 2013 U
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 700 - 1130}$ 95 73
 2012 AV
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 200 - 760}$ 95 74
 2012 BB
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
75
 2012 CK
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$
$> 2550$ 95 76
 2012 CR
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
77
 2012 M
ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$
78
 2012 N
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$
$\text{none 200 - 1143}$ 95 74
 2012 AF
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
79
 2012 AR
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$
80
 2012 BG
CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$
$> 1120$ 95
 2011 C
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$
$\text{none 180 - 690}$ 95 81
 2011 H
D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 600 - 863}$ 95 82
 2011 L
D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 285 - 516}$ 95 83
 2010 N
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$\text{none 280 - 840}$ 95 84
 2009 AC
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 1000$ 95
 2008 C
D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$
$\text{none 300 - 800}$ 95
 2004 C
D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 225 - 536}$ 95 85
 2003 B
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$
$\text{none 200 - 480}$ 95 86
 2002 C
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$
$>786$ 95 87
 2001 I
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$
$\text{none 300 - 420}$ 95 88
 1997 G
CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$>720$ 95 89
 1996 C
D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$
$>610$ 95 90
 1995 E
D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \tau}}{{\mathit \nu}}$
$\text{none 260 - 600}$ 95 91
 1993
RVUE ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
1  AABOUD 2019B search for right-handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \ell}}$ and hypothetical heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying to ${{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ . See their Figs. 7 and 8 for excluded regions in $\mathit M_{{{\mathit W}_{{R}}}}$ $−$ ${{\mathit M}_{{N}}}$ plane.
2  AABOUD 2019E search for right-handed ${{\mathit W}^{\,'}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 8 for limit on on $\sigma \cdot{}\mathit B$.
3  AAD 2019C search for ${{\mathit W}^{\,'}}$ with SM-like couplings in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. Bosonic decays and ${{\mathit W}}−{{\mathit W}^{\,'}}$ interference are neglected. The limits on ${{\mathit e}}$ and ${{\mathit \mu}}$ separately are 6.0 and 5.1 TeV respectively. See their Fig. 2 for limits on $\sigma \cdot{}B$.
4  AAD 2019D search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3400 GeV for ${{\mathit g}_{{V}}}$ = 1. If we assume $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$, the limit increases $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3800 GeV and $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3500 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1, respectively. See their Fig. 9 for limits on $\sigma \cdot{}B$.
5  SIRUNYAN 2019AY limits shown for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}}−{{\mathit W}^{\,'}}$ interference and bosonic decays of ${{\mathit W}^{\,'}}$ are not included. See their Fig. 5 for limits on $\sigma \cdot{}\mathit B$. Limits in the context of a nonuniversal gauge interaction are shown in Fig. 7. Model independent limits on ${{\mathit \sigma}}{{\mathit B}}{{\mathit A}}{{\mathit \epsilon}}$ can be seen in Fig. 8.
6  SIRUNYAN 2019CP present a statistical combinations of searches for ${{\mathit W}^{\,'}}$ decaying to pairs of bosons or leptons in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. If we assume ${{\mathit M}}_{{{\mathit W}^{\,'}}}$ = ${{\mathit M}}_{{{\mathit Z}^{\,'}}}$, the limit becomes ${{\mathit M}}_{{{\mathit W}^{\,'}}}$ $>$ 4500 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit M}}_{{{\mathit W}^{\,'}}}$ $>$ 5000 GeV for ${{\mathit g}_{{V}}}$ = 1. See their Figs. 2 and 3 for limits on $\sigma \cdot{}B$.
7  SIRUNYAN 2019I search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2800 GeV if we assume $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$.
8  AABOUD 2018AF give the limit above for right-handed ${{\mathit W}^{\,'}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. These limits also exclude ${{\mathit W}}$ bosons with left-handed couplings with masses below 2.9 TeV, at the 95$\%$ confidence level. ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}_{{R}}}$ is assumed to be forbidden. See their Fig.5 for limits on $\sigma \cdot{}{{\mathit B}}$ for both cases of left- and right-handed ${{\mathit W}^{\,'}}$.
9  AABOUD 2018AI search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2670 GeV for ${{\mathit g}_{{V}}}$ = 1. If we assume $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$, the limit increases $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2930 GeV and $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2800 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1, respectively. See their Fig. 5 for limits on $\sigma \cdot{}\mathit B$.
10  AABOUD 2018AK search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2800 GeV for ${{\mathit g}_{{V}}}$ = 1.
11  AABOUD 2018AL search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2900 GeV for ${{\mathit g}_{{V}}}$ = 1.
12  AABOUD 2018BG limit is for ${{\mathit W}^{\,'}}$ with SM-like couplings using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. Bosonic decays of ${{\mathit W}^{\,'}}$ and ${{\mathit W}}−{{\mathit W}^{\,'}}$ interference are neglected. See Fig. 2 for limits on $\sigma \cdot{}{{\mathit B}}$.
13  AABOUD 2018CH search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2260 GeV for ${{\mathit g}_{{V}}}$ = 1.
14  AABOUD 2018F search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3000 GeV for ${{\mathit g}_{{V}}}$ = 1. If we assume $\mathit M_{{{\mathit Z}^{\,'}}}$ = $\mathit M_{{{\mathit W}^{\,'}}}$, the limit increases $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3500 GeV and $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3100 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1, respectively. See their Fig.5 for limits on $\sigma \cdot{}{{\mathit B}}$.
15  AABOUD 2018K limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}}−{{\mathit W}^{\,'}}$ interference and bosonic decays of ${{\mathit W}^{\,'}}$ are not included. See their Fig. 4 for limit on $\sigma \cdot{}{{\mathit B}}$.
16  SIRUNYAN 2018 limit is for right-handed ${{\mathit W}^{\,'}}$ using $pp$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}_{{R}}}$ decay is assumed to be forbidden. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3.4 TeV if $\mathit M_{{{\mathit \nu}_{{R}}}}{}\ll$ $\mathit M_{{{\mathit W}^{\,'}}}$. See their Fig. 5 for exclusion limits on ${{\mathit W}^{\,'}}$ models having both left- and right-handed couplings.
17  SIRUNYAN 2018AX search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. See their Fig.6 for limits on $\sigma \cdot{}$B.
18  SIRUNYAN 2018AZ limit is derived for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. No interference with SM ${{\mathit W}}$ process is considered. The bosonic decays are assumed to be negligible. See their Fig.6 for limits on $\sigma \cdot{}{{\mathit B}}$.
19  SIRUNYAN 2018BK search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes M$_{{{\mathit W}^{\,'}}}>$ 3100 GeV for ${{\mathit g}_{{V}}}$ = 1.
20  SIRUNYAN 2018BO limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
21  SIRUNYAN 2018CV search for right-handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \ell}}$ and hypothetical heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying to ${{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ . The quoted limit is for ${{\mathit M}_{{N}}}$ = ${{\mathit M}}_{{{\mathit W}_{{R}}}}$/2. See their Fig. 6 for excluded regions in the ${{\mathit M}}_{{{\mathit W}_{{R}}}}−{{\mathit M}_{{N}}}$ plane.
22  SIRUNYAN 2018DJ search for resonances decaying to $WZ$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2270 GeV for ${{\mathit g}_{{V}}}$ = 1.
23  SIRUNYAN 2018ED search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit above is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. If we assume $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$, the limit increases $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2900 GeV and $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2800 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1, respectively.
24  SIRUNYAN 2018P give this limit for a heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. If they assume $\mathit M_{{{\mathit Z}^{\,'}}}$ = $\mathit M_{{{\mathit W}^{\,'}}}$, the limit increases to $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 3800 GeV.
25  AABOUD 2017AK search for a new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit above is for a ${{\mathit W}^{\,'}}$ boson having axial-vector SM couplings and decaying to quarks with 75$\%$ branching fraction.
26  AABOUD 2017AO search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for a ${{\mathit W}^{\,'}}$ in the heavy-vector-triplet model with ${{\mathit g}_{{V}}}$ = 3. See their Fig.4 for limits on $\sigma \cdot{}{{\mathit B}}$.
27  AABOUD 2017B search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit c}}{{\overline{\mathit c}}}$ ; ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ ) in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes ${{\mathit M}}_{{{\mathit W}^{\,'}}}$ $>$ 1750 GeV for ${{\mathit g}_{{V}}}$ = 1. If we assume ${{\mathit M}}_{{{\mathit W}^{\,'}}}$ = ${{\mathit M}}_{{{\mathit Z}^{\,'}}}$, the limit increases ${{\mathit M}}_{{{\mathit W}^{\,'}}}>$ 2310 GeV and ${{\mathit M}}_{{{\mathit W}^{\,'}}}>$ 1730 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1, respectively. See their Fig.3 for limits on ${{\mathit \sigma}}\cdot{}{{\mathit B}}$.
28  KHACHATRYAN 2017J search for right-handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \tau}}$ and hypothetical heavy neutrino ${{\mathit N}_{{\tau}}}$, with ${{\mathit N}_{{\tau}}}$ decaying into ${{\mathit \tau}}{{\mathit j}}{{\mathit j}}$ . The quoted limit is for $\mathit M_{{{\mathit N}_{{\tau}}}}$ = $\mathit M_{{{\mathit W}_{{R}}}}$/2. The limit becomes $\mathit M_{{{\mathit W}_{{R}}}}$ $>$ 2350 GeV (1630 GeV) for $\mathit M_{{{\mathit W}_{{R}}}}/\mathit M_{{{\mathit N}_{{\tau}}}}$ = 0.8 (0.2). See their Fig. 4 for excluded regions in the $\mathit M_{{{\mathit W}_{{R}}}}−\mathit M_{{{\mathit N}_{{\tau}}}}$ plane.
29  KHACHATRYAN 2017W search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
30  KHACHATRYAN 2017Z limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The bosonic decays of ${{\mathit W}^{\,'}}$ and the interference with SM ${{\mathit W}}$ process are neglected.
31  SIRUNYAN 2017A search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ with ${{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit q}}{{\overline{\mathit q}}}{{\mathit q}}{{\overline{\mathit q}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2000 GeV for ${{\mathit g}_{{V}}}$ = 1. If we assume $\mathit M_{{{\mathit Z}^{\,'}}}$ = $\mathit M_{{{\mathit W}^{\,'}}}$, the limit increases $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2400 GeV and $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2300 GeV for ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1, respectively. See their Fig.6 for limits on $\sigma \cdot{}\mathit B$.
32  SIRUNYAN 2017AK search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ or ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 and 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2300 GeV for ${{\mathit g}_{{V}}}$ = 1. If we assume $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$, the limit increases $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2400 GeV for both ${{\mathit g}_{{V}}}$ = 3 and ${{\mathit g}_{{V}}}$ = 1. See their Fig.1 and 2 for limits on ${{\mathit \sigma}}\cdot{}{{\mathit B}}$.
33  SIRUNYAN 2017H search for right-handed ${{\mathit W}^{\,'}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}^{\,'}}$ is assumed to decay into ${{\mathit \tau}}$ and a heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying to ${{\mathit \tau}}{{\mathit q}}{{\overline{\mathit q}}}$ . The limit above assumes M$_{N}$ = M$_{{{\mathit W}^{\,'}}}$/2.
34  SIRUNYAN 2017I limit is for a right-handed ${{\mathit W}^{\,'}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit becomes ${{\mathit M}}_{{{\mathit W}^{\,'}}}$ $>$ 2400 GeV for ${{\mathit M}}_{{{\mathit \nu}_{{R}}}}{}\ll$ ${{\mathit M}}_{{{\mathit W}^{\,'}}}$.
35  SIRUNYAN 2017R search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. Mass regions $\mathit M_{{{\mathit W}^{\,'}}}$ $<$ 2370 GeV and 2870 $<$ $\mathit M_{{{\mathit W}^{\,'}}}$ $<$ 2970 GeV are excluded for ${{\mathit g}_{{V}}}$ = 1. If we assume $\mathit M_{{{\mathit Z}^{\,'}}}$ = $\mathit M_{{{\mathit W}^{\,'}}}$, the excluded mass regions are 1000 $<$ $\mathit M_{{{\mathit W}^{\,'}}}$ $<$ 2500 GeV and 2760 $<$ $\mathit M_{{{\mathit W}^{\,'}}}$ $<$ 3300 GeV for ${{\mathit g}_{{V}}}$ = 3; 1000 $<$ $\mathit M_{{{\mathit W}^{\,'}}}$ $<$ 2430 GeV and 2810 $<$ $\mathit M_{{{\mathit W}^{\,'}}}$ $<$ 3130 GeV for ${{\mathit g}_{{V}}}$ = 1. See their Fig.5 for limits on ${{\mathit \sigma}}\cdot{}{{\mathit B}}$.
36  AABOUD 2016AE search for resonances decaying to ${{\mathit V}}{{\mathit V}}$ (${{\mathit V}}$ = ${{\mathit W}}$ or ${{\mathit Z}}$) in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. Results from ${{\mathit \nu}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}}$ , ${{\mathit \nu}}{{\mathit \ell}}{{\mathit q}}{{\mathit q}}$ , ${{\mathit \ell}}{{\mathit \ell}}{{\mathit q}}{{\mathit q}}$ and ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}$ final states are combined. The quoted limit is for a heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3 and $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$.
37  AABOUD 2016V limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The bosonic decays of ${{\mathit W}^{\,'}}$ and the interference with SM ${{\mathit W}}$ process are neglected.
38  AAD 2016R search for ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}^{\,'}}{{\mathit \ell}^{\,'}}$ , ${{\mathit \ell}}{{\mathit \ell}}{{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ , and all hadronic channels are combined. The quoted limit assumes ${{\mathit g}}_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/{{\mathit g}}_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = (${{\mathit M}_{{W}}}/{{\mathit M}}_{{{\mathit W}^{\,'}}}){}^{2}$.
39  AAD 2016S search for a new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for a ${{\mathit W}^{\,'}}$ having SM-like couplings to quarks.
40  KHACHATRYAN 2016AO limit is for a SM-like right-handed using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The quoted limit combines ${{\mathit t}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit b}}$ and ${{\mathit t}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit b}}$ events.
41  KHACHATRYAN 2016AP search for a resonance decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. Both ${{\mathit H}}$ and ${{\mathit W}}$ are assumed to decay to fat jets. The quoted limit is for heavy-vector-triplet ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3.
42  KHACHATRYAN 2016BD search for resonance decaying to ${{\mathit H}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The quoted limit is for heavy-vector-triplet (HVT) ${{\mathit W}^{\,'}}$ with ${{\mathit g}_{{V}}}$ = 3. The HVT model ${\mathit m}_{{{\mathit W}^{\,'}}}$ = ${\mathit m}_{{{\mathit Z}^{\,'}}}$ $>$ 1.8 TeV is also obtained by combining ${{\mathit W}^{\,'}}$/ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ / ${{\mathit Z}}$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit b}}{{\mathit b}}$ , ${{\mathit q}}{{\mathit q}}{{\mathit \tau}}{{\mathit \tau}}$ , ${{\mathit q}}{{\mathit q}}{{\mathit b}}{{\mathit b}}$ , and ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}$ channels.
43  KHACHATRYAN 2016K search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
44  KHACHATRYAN 2016L search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV with the data scouting technique, increasing the sensitivity to the low mass resonances.
45  KHACHATRYAN 2016O limit is for ${{\mathit W}^{\,'}}$ having universal couplings. Interferences with the SM amplitudes are assumed to be absent.
46  AAD 2015AU search for ${{\mathit W}^{\,'}}$ decaying into the ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}^{\,'}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{W}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
47  AAD 2015AV limit is for a SM like right-handed ${{\mathit W}^{\,'}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ decay is assumed to be forbidden.
48  AAD 2015AZ search for ${{\mathit W}^{\,'}}$ decaying into the ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
49  AAD 2015CP search for ${{\mathit W}^{\,'}}$ decaying into the ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
50  AAD 2015R limit is for a SM like right-handed ${{\mathit W}^{\,'}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ decay is assumed to be forbidden.
51  AAD 2015V search for new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.
52  KHACHATRYAN 2015C search for ${{\mathit W}^{\,'}}$ decaying via ${{\mathit W}}{{\mathit Z}}$ to fully leptonic final states using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=8 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = $\mathit M_{W}$ $\mathit M_{Z}/\mathit M{}^{2}_{{{\mathit W}^{\,'}}}$.
53  KHACHATRYAN 2015T limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling which interferes the SM ${{\mathit W}}$ boson constructively using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. For ${{\mathit W}^{\,'}}$ without interference, the limit becomes $>$ 3280 GeV.
54  KHACHATRYAN 2014O search for right-handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \ell}}$ and hypothetical heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying into ${{\mathit \ell}}{{\mathit j}}$ ${{\mathit j}}$ . The quoted limit is for ${{\mathit M}}_{{{\mathit \nu}_{{eR}}}}$ = ${{\mathit M}}_{{{\mathit \nu}}_{ {{\mathit \mu}} {{\mathit R}} }}$ = ${{\mathit M}}_{{{\mathit W}_{{R}}}}$/2. See their Fig. 3 and Fig. 5 for excluded regions in the ${{\mathit M}}_{{{\mathit W}_{{R}}}}−{{\mathit M}}_{{{\mathit \nu}}}$ plane.
55  AABOUD 2019BB search for right handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \ell}}$ and a boosted hypothetical heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying to ${{\mathit \ell}}$ and a large radius jet ${{\mathit j}}$ = ${{\mathit q}}{{\overline{\mathit q}}}$ . See their Fig. 7 for excluded regions in ${{\mathit M}}_{{{\mathit W}_{{R}}}}−{{\mathit M}_{{N}}}$ plane.
56  SIRUNYAN 2019V search for a new resonance decaying to a top quark and a heavy vector-like bottom partner ${{\mathit B}}$ decaying to ${{\mathit H}}{{\mathit b}}$ (or a bottom quark and a heavy vector-like top partner ${{\mathit T}}$ decaying to ${{\mathit H}}{{\mathit t}}$ ) in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 8 for limits on ${{\mathit \sigma}}\cdot{}{{\mathit B}}$.
57  AABOUD 2018AA search for a narrow charged vector boson decaying to ${{\mathit W}}{{\mathit \gamma}}$ . See their Fig. 9 for the exclusion limit in M$_{{{\mathit W}^{\,'}}}$ $−$ $\sigma$B plane.
58  AABOUD 2018AD search for resonances decaying to ${{\mathit H}}{{\mathit X}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit X}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}^{\,'}}$ ) in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Figs. $3 - 5$ for limits on $\sigma \cdot{}$B.
59  AABOUD 2018CJ search for heavy-vector-triplet ${{\mathit W}^{\,'}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit quoted above is for model with ${{\mathit g}_{{V}}}$ = 3 assuming $\mathit M_{{{\mathit W}^{\,'}}}$ = $\mathit M_{{{\mathit Z}^{\,'}}}$. The limit becomes $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 5500 GeV for model with ${{\mathit g}_{{V}}}$ = 1.
60  KHACHATRYAN 2017U search for resonances decaying to ${{\mathit H}}{{\mathit W}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ; ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ ) in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit on the heavy-vector-triplet model is $\mathit M_{{{\mathit Z}^{\,'}}}$ = $\mathit M_{{{\mathit W}^{\,'}}}$ $>$ 2 TeV for ${{\mathit g}_{{V}}}$ = 3, in which constraints from the ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit H}}{{\mathit Z}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ , ${{\mathit \nu}}{{\overline{\mathit \nu}}}$ ) are combined. See their Fig.3 and Fig.4 for limits on $\sigma \cdot{}\mathit B$.
61  AAD 2015BB search for ${{\mathit W}^{\,'}}$ decaying into ${{\mathit W}}{{\mathit H}}$ with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ . See their Fig. 4 for the exclusion limits in the heavy vector triplet benchmark model parameter space.
62  AALTONEN 2015C limit is for a SM-like right-handed ${{\mathit W}^{\,'}}$ assuming ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ decays are forbidden, using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.96 TeV. See their Fig. 3 for limit on $\mathit g_{{{\mathit W}^{\,'}}}/\mathit g_{{{\mathit W}}}$.
63  KHACHATRYAN 2015V search new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.
64  AAD 2014AT search for a narrow charged vector boson decaying to ${{\mathit W}}{{\mathit \gamma}}$ . See their Fig. 3a for the exclusion limit in ${\mathit m}_{{{\mathit W}^{\,'}}}−\sigma \mathit B$ plane.
65  AAD 2014S search for ${{\mathit W}^{\,'}}$ decaying into the ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=8 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
66  KHACHATRYAN 2014 search for ${{\mathit W}^{\,'}}$ decaying into ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=8 TeV. The quoted limit assumes ${{\mathit g}}_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/{{\mathit g}}_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = (${{\mathit M}_{{W}}}/{{\mathit M}}_{{{\mathit W}^{\,'}}}){}^{2}$.
67  KHACHATRYAN 2014A search for ${{\mathit W}^{\,'}}$ decaying into the ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ , or ${{\mathit W}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ , ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$ . ${{\mathit p}}{{\mathit p}}$ collisions data at $\sqrt {s }$=8 TeV are used for the search. See their Fig. 13 for the exclusion limit on the number of events in the mass$−$width plane.
68  AAD 2013AO search for ${{\mathit W}^{\,'}}$ decaying into the ${{\mathit W}}{{\mathit Z}}$ final state with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit Z}}$ $\rightarrow$ 2 ${{\mathit j}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
69  CHATRCHYAN 2013AJ search for resonances decaying to ${{\mathit W}}{{\mathit Z}}$ pair, using the hadronic decay modes of ${{\mathit W}}$ and ${{\mathit Z}}$, in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV. See their Fig. 7 for the limit on the cross section.
70  CHATRCHYAN 2013AQ limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling which interferes with the SM ${{\mathit W}}$ boson using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV.
71  CHATRCHYAN 2013E limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling which intereferes with the SM ${{\mathit W}}$ boson using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV. For ${{\mathit W}^{\,'}}$ with right-handed coupling, the bound becomes $>$1850 GeV ($>$1910 GeV) if ${{\mathit W}^{\,'}}$ decays to both leptons and quarks (only to quarks). If both left- and right-handed couplings are present, the limit becomes $>$1640 GeV.
72  CHATRCHYAN 2013U search for ${{\mathit W}^{\,'}}$ decaying to the ${{\mathit W}}{{\mathit Z}}$ final state, with ${{\mathit W}}$ decaying into jets, in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
73  The AAD 2012AV quoted limit is for a SM-like right-handed ${{\mathit W}^{\,'}}$ using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV. ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ decay is assumed to be forbidden.
74  AAD 2012BB use ${{\mathit p}}{{\mathit p}}$ collisions data at $\sqrt {s }$=7 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
75  AAD 2012CK search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}^{\,'}}$ , ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$ events in ${{\mathit p}}{{\mathit p}}$ collisions. See their Fig. 5 for the limit on $\sigma \cdot{}$B.
76  AAD 2012CR use ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV.
77  AAD 2012M search for right-handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \ell}}$ and hypothetical heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying into ${{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ . See their Fig. 4 for the limit in the ${\mathit m}_{{{\mathit N}}}−{\mathit m}_{{{\mathit W}^{\,'}}}$ plane.
78  AALTONEN 2012N search for ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}^{\,'}}$ , ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit d}}$ events in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions. See their Fig. 3 for the limit on $\sigma \cdot{}$B.
79  CHATRCHYAN 2012AR search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}^{\,'}}$ , ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit d}}$ events in ${{\mathit p}}{{\mathit p}}$ collisions. See their Fig. 2 for the limit on $\sigma \cdot{}$B.
80  CHATRCHYAN 2012BG search for right-handed ${{\mathit W}_{{R}}}$ in collisions $\sqrt {s }$ = 7 TeV. ${{\mathit W}_{{R}}}$ is assumed to decay into ${{\mathit \ell}}$ and hypothetical heavy neutrino ${{\mathit N}}$, with ${{\mathit N}}$ decaying into ${{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ . See their Fig. 3 for the limit in the ${\mathit m}_{{{\mathit N}}}−{\mathit m}_{{{\mathit W}^{\,'}}}$ plane.
81  ABAZOV 2011H use data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.96 TeV. The quoted limit is obtained assuming ${{\mathit W}^{\,'}}{{\mathit W}}{{\mathit Z}}$ coupling strength is the same as the ordinary ${{\mathit W}}{{\mathit W}}{{\mathit Z}}$ coupling strength in the Standard Model.
82  ABAZOV 2011L limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling which interferes with the SM ${{\mathit W}}$ boson, using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.96 TeV. For ${{\mathit W}^{\,'}}$ with right-handed coupling, the bound becomes $>$885 GeV ($>$890 GeV) if ${{\mathit W}^{\,'}}$ decays to both leptons and quarks (only to quarks). If both left- and right-handed couplings present, the limit becomes $>$916 GeV.
83  AALTONEN 2010N use ${{\mathit p}}{{\overline{\mathit p}}}$ collision data at $\sqrt {s }$=1.96 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$. See their Fig.$~$4 for limits in mass-coupling plane.
84  AALTONEN 2009AC search for new particle decaying to dijets using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.96 TeV.
85  The ACOSTA 2003B quoted limit is for $\mathit M_{{{\mathit W}^{\,'}}}{}\gg\mathit M_{{{\mathit \nu}_{{R}}}}$, using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.8 TeV. For $\mathit M_{{{\mathit W}^{\,'}}}<\mathit M_{{{\mathit \nu}_{{R}}}}$, $\mathit M_{{{\mathit W}^{\,'}}}$ between 225 and 566 GeV is excluded.
86  The quoted limit is obtained assuming ${{\mathit W}^{\,'}}{{\mathit W}}{{\mathit Z}}$ coupling strength is the same as the ordinary ${{\mathit W}}{{\mathit W}}{{\mathit Z}}$ coupling strength in the Standard Model, using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.8 TeV. See their Fig.$~$2 for the limits on the production cross sections as a function of the ${{\mathit W}^{\,'}}$ width.
87  AFFOLDER 2001I combine a new bound on ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ of 754 GeV, using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.8 TeV, with the bound of ABE 2000 on ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \mu}}{{\mathit \nu}}$ to obtain quoted bound.
88  ABE 1997G search for new particle decaying to dijets using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.8 TeV.
89  For bounds on ${{\mathit W}_{{R}}}$ with nonzero right-handed mass, see Fig.$~$5 from ABACHI 1996C.
90  ABACHI 1995E assume that the decay ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ is suppressed and that the neutrino from ${{\mathit W}^{\,'}}$ decay is stable and has a mass significantly less ${\mathit m}_{{{\mathit W}^{\,'}}}$.
91  RIZZO 1993 analyses CDF limit on possible two-jet resonances. The limit is sensitive to the inclusion of the assumed ${{\mathit K}}$ factor.
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 AABOUD 2019B
JHEP 1901 016 Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets at $\sqrt{s}$ = 13 TeV with the ATLAS detector
 AABOUD 2019E
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 AABOUD 2018AL
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 AABOUD 2018CJ
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 AABOUD 2018AI
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 AABOUD 2018CH
PL B787 68 Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
 AABOUD 2018AK
JHEP 1803 042 Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector
 AABOUD 2018K
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 AABOUD 2018BG
EPJ C78 401 Search for a new heavy gauge boson resonance decaying into a lepton and missing transverse momentum in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS experiment
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 SIRUNYAN 2018
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 SIRUNYAN 2018DJ
JHEP 1809 101 Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2?2q final states at $\sqrt{s}=13$ TeV
 SIRUNYAN 2018AX
JHEP 1805 088 Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at $\sqrt{s}=13$ TeV
 SIRUNYAN 2018BK
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 SIRUNYAN 2018BO
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 SIRUNYAN 2018AZ
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 SIRUNYAN 2018CV
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 SIRUNYAN 2018ED
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 SIRUNYAN 2018P
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 AABOUD 2017B
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 AABOUD 2017AK
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 AABOUD 2017AO
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 KHACHATRYAN 2017Z
PL B770 278 Search for Heavy Gauge ${{\mathit W}^{\,'}}$ Boson in Events with an Energetic Lepton and Large Missing Transverse Momentum at $\sqrt {s }$ = 13 TeV
 KHACHATRYAN 2017U
PL B768 137 Search for Heavy Resonances Decaying into a Vector Boson and a Higgs Boson in Final States with Charged Leptons, Neutrinos, and ${\mathit {\mathit b}}$ Quarks
 KHACHATRYAN 2017W
PL B769 520 Search for Dijet Resonances in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV and Constraints on Dark Matter and other Models
 KHACHATRYAN 2017J
JHEP 1703 077 Search for Heavy Neutrinos or Third-Generation Leptoquarks in Final States with Two Hadronically Decaying ${{\mathit \tau}}$ Leptons and Two Jets in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
 SIRUNYAN 2017R
EPJ C77 636 Search for Heavy Resonances that Decay into a Vector Boson and a Higgs Boson in Hadronic Final States at $\sqrt {s }$ = 13 TeV
 SIRUNYAN 2017I
JHEP 1708 029 Searches for ${{\mathit W}^{\,'}}$ Bosons Decaying to a Top Quark and a Bottom Quark in Proton-Proton Collisions at 13 TeV
 SIRUNYAN 2017H
JHEP 1707 121 Search for Third-Generation Scalar Leptoquarks and Heavy Right-Handed Neutrinos in Final States with Two Tau Leptons and Two Jets in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
 SIRUNYAN 2017A
JHEP 1703 162 Search for Massive Resonances Decaying into ${{\mathit W}}{{\mathit W}}$, ${{\mathit W}}{{\mathit Z}}$ or ${{\mathit Z}}{{\mathit Z}}$ Bosons in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
 SIRUNYAN 2017AK
PL B774 533 Combination of Searches for Heavy Resonances Decaying to ${{\mathit W}}{{\mathit W}}$, ${{\mathit W}}{{\mathit Z}}$, ${{\mathit Z}}{{\mathit Z}}$, ${{\mathit W}}{{\mathit H}}$, and ${{\mathit Z}}{{\mathit H}}$ Boson Pairs in Proton-Proton Collisions at $\sqrt {s }$ = 8 and 13 TeV
 AABOUD 2016V
PL B762 334 Search for New Resonances in Events with One Lepton and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
 AABOUD 2016AE
JHEP 1609 173 Searches for Heavy Diboson Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
PL B754 302 Search for New Phenomena in Dijet Mass and Angular Distributions from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
PL B755 285 Combination of Searches for ${{\mathit W}}{{\mathit W}}$, ${{\mathit W}}{{\mathit Z}}$, and ${{\mathit Z}}{{\mathit Z}}$ Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
 KHACHATRYAN 2016AO
JHEP 1602 122 Search for ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2016K
PRL 116 071801 Search for Narrow Resonances Decaying to Dijets in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
 KHACHATRYAN 2016L
PRL 117 031802 Search for Narrow Resonances in Dijet Final States at $\sqrt {s }$ = 8 TeV with the Novel CMS Technique of Data Scouting
 KHACHATRYAN 2016O
PL B755 196 Search for ${{\mathit W}^{\,'}}$ Decaying to Tau Lepton and Neutrino in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2016AP
JHEP 1602 145 Search for a Massive Resonance Decaying into a Higgs Boson and a ${{\mathit W}}$ or ${{\mathit Z}}$ Boson in Hadronic Final States in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2016BD
EPJ C76 237 Search for Massive ${{\mathit W}}{{\mathit H}}$ Resonances Decaying into the ${{\mathit \ell}}{{\mathit \nu}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Final State at $\sqrt {s }$ = 8 TeV
EPJ C75 165 Search for ${{\mathit W}^{\,'}}$ $\rightarrow$ ${\mathit {\mathit t}}{\mathit {\mathit b}}$ $\rightarrow$ ${\mathit {\mathit q}}{\mathit {\mathit q}}{\mathit {\mathit b}}{\mathit {\mathit b}}$ Decays in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
EPJ C75 69 Search for Resonant Diboson Production in the ${{\mathit \ell}}{{\mathit \ell}}{\mathit {\mathit q}}{\mathit {\overline{\mathit q}}}$ Final State in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
PR D91 052007 Search for New Phenomena in the Dijet Mass Distribution using ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
PL B743 235 Search for ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit b}}}$ in the Lepton Plus Jets Final State in Proton-Proton Collisions at a Centre-of-Mass Energy of $\sqrt {s }$ = 8 TeV with the ATLAS Detector
JHEP 1512 055 Search for High-Mass Diboson Resonances with Boson-Tagged Jets in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
EPJ C75 209 Search for Production of ${{\mathit W}}{{\mathit W}}/{{\mathit W}}{{\mathit Z}}$ Resonances Decaying to a Lepton, Neutrino and Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
EPJ C75 263 Search for a New Resonance Decaying to a ${{\mathit W}}$ or ${{\mathit Z}}$ Boson and a Higgs Boson in the ${{\mathit \ell}}{{\mathit \ell}}/{{\mathit \ell}}{{\mathit \nu}}/{{\mathit \nu}}{{\mathit \nu}}+{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Final States with the ATLAS Detector
 AALTONEN 2015C
PRL 115 061801 Search for Resonances Decaying to Top and Bottom Quarks with the CDF Experiment
 KHACHATRYAN 2015T
PR D91 092005 Search for Physics Beyond the Standard Model in Final States with a Lepton and Missing Transverse Energy in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2015C
PL B740 83 Search for New Resonances Decaying via ${{\mathit W}}{{\mathit Z}}$ to Leptons in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2015V
PR D91 052009 Search for Resonances and Quantum Black Holes using Dijet Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
PL B737 223 Search for ${{\mathit W}}{{\mathit Z}}$ Resonances in the Fully Leptonic Channel using ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
PL B738 428 Search for New Resonances in ${{\mathit W}}{{\mathit \gamma}}$ and ${{\mathit Z}}{{\mathit \gamma}}$ Final States in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
JHEP 1409 037 Search for New Particles in Events with one Lepton and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS detector
 KHACHATRYAN 2014A
JHEP 1408 174 Search for Massive Resonances Decaying into Pairs of Boosted Bosons in Semi-Leptonic Final States at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2014
JHEP 1408 173 Search for Massive Resonances in Dijet Systems Containing Jets Tagged as ${{\mathit W}}$ or ${{\mathit Z}}$ Boson Decays in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2014O
EPJ C74 3149 Search for Heavy Neutrinos and ${{\mathit W}}$ Bosons with Right-Handed Couplings in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
JHEP 1301 029 ATLAS Search for New Phenomena in Dijet Mass and Angular Distributions using ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
PR D87 112006 Search for Resonant Diboson Production in the ${{\mathit \ell}}{{\mathit \nu}}{{\mathit j}}{{\mathit j}}$ Decay Channels with the ATLAS Detector at 7 TeV
 CHATRCHYAN 2013U
JHEP 1302 036 Search for Exotic Resonances Decaying into ${{\mathit W}}{{\mathit Z}}/{{\mathit Z}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2013AJ
PL B723 280 Search for Heavy Resonances in the ${{\mathit W}}/{{\mathit Z}}$-Tagged Dijet Mass Spectrum in ${{\mathit p}}{{\mathit p}}$ Collisions at 7 TeV
 CHATRCHYAN 2013A
JHEP 1301 013 Search for Narrow Resonances and Quantum Black Holes in Inclusive and ${\mathit {\mathit b}}$-Tagged Dijet Mass Spectra from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2013E
PL B718 1229 Search for a ${{\mathit W}^{\,'}}$ Boson Decaying to a Bottom Quark and a Top Quark in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2013AQ
PR D87 072005 Search for New Physics in Final States with a Lepton and Missing Transverse Energy in ${{\mathit p}}{{\mathit p}}$ Collisions at the LHC
EPJ C72 2241 ATLAS Search for a Heavy Gauge Boson Decaying to a Charged Lepton and a Neutrino in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
EPJ C72 2056 Search for Heavy Neutrinos and Right-Handed ${{\mathit W}}$ Bosons in Events with Two Leptons and Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector
PR D86 091103 Search for Resonant Top Quark Plus Jet Production in ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ +Jets Events with the ATLAS Detector in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$= 7 TeV
PRL 109 081801 Search for ${\mathit {\mathit t}}{\mathit {\mathit b}}$ Resonances in Proton$−$Proton Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector
PR D85 112012 Search for Resonant ${{\mathit W}}{{\mathit Z}}$ production in the ${{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}^{\,'}}{{\mathit \ell}^{\,'}}$ Channel in $\sqrt {s }$ = 7 TeV ${{\mathit p}}{{\mathit p}}$ Collisions with the ATLAS Detector
 AALTONEN 2012N
PRL 108 211805 Search for a Heavy Particle Decaying to a Top Quark and a Light Quark in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 CHATRCHYAN 2012BG
PRL 109 261802 Search for Heavy Neutrinos and ${{\mathit W}_{{R}}}$ Bosons with Right-Handed Couplings in a Left-Right Symmetric Model in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2012AR
PL B717 351 Search for Charge-Asymmetric Production of ${{\mathit W}^{\,'}}$ Bosons in ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ $+$ jet Events from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 CHATRCHYAN 2012AF
PRL 109 141801 Search for a ${{\mathit W}^{\,'}}$ or Techni-${{\mathit \rho}}$ Decaying into ${{\mathit W}}{{\mathit Z}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
 AALTONEN 2011C
PR D83 031102 Search for a New Heavy Gauge Boson with Event Signature Electron+Missing Transverse Energy in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2011H
PRL 107 011801 Search for Resonant ${{\mathit W}}{{\mathit W}}$ and ${{\mathit W}}{{\mathit Z}}$ Production in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2011L
PL B699 145 Search for ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ Resonances with Left- and Right-Handed Couplings to Fermions
 AALTONEN 2010N
PRL 104 241801 Search for ${{\mathit W}}{{\mathit W}}$ and ${{\mathit W}}{{\mathit Z}}$ Resonances Decaying to Electron, Missing $\mathit E_{T}$, and Two Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 AALTONEN 2009AC
PR D79 112002 Search for New Particles Decaying into Dijets in Proton-Antiproton Collisions at $\sqrt {s }$ = 1.96$~$TeV
 ABAZOV 2008C
PRL 100 031804 Search for ${{\mathit W}^{\,'}}$ Bosons Decaying to an Electron and a Neutrino with the ${D0}$ Detector
 ABAZOV 2004C
PR D69 111101 Search for New Particles in the Two Jet Decay Channel with the ${D0}$ Detector
 ACOSTA 2003B
PRL 90 081802 Search for a ${{\mathit W}^{\,'}}$ Boson Decaying to a Top and Bottom Quark Pair in 1.8 TeV ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions
 AFFOLDER 2002C
PRL 88 071806 Search for New Heavy Particles in the ${{\mathit W}}{{\mathit Z}^{0}}$ Final States in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8-TeV
 AFFOLDER 2001I
PRL 87 231803 Search for Quark-Lepton Compositeness and a Heavy ${{\mathit W}^{\,'}}$ Boson using the ${{\mathit e}}{{\mathit \nu}}$ Channel in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV
 ABE 1997G
PR D55 5263 Search for New Particles Decaying to Dijets at CDF
 ABACHI 1996C
PRL 76 3271 Search for Right Handed ${{\mathit W}}$ Bosons and Heavy ${{\mathit W}^{\,'}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV
 ABACHI 1995E
PL B358 405 Search for Heavy ${{\mathit W}}$ Boson in 1.8 TeV ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions
 RIZZO 1993
PR D48 4470 Constraints on New Physics from Fermilab Tevatron Dijet Data