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 $\bf{ > 6000}$ OUR LIMIT $\text{none 1000 - 3400}$ 95 1 SIRUNYAN 2021 Y CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $> 3200$ 95 2 AAD 2020 AJ ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $> 4300$ 95 3 AAD 2020 AT ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 1100 - 4000}$ 95 4 AAD 2020 T ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 1800 - 3600}$ 95 5 SIRUNYAN 2020 AI CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 1200 - 3800}$ 95 6 SIRUNYAN 2020 Q CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ 7 AABOUD 2019 B ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ $\text{none 500 - 3250}$ 95 8 AABOUD 2019 E ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\bf{> 6000}$ 95 9 AAD 2019 C ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $\text{none 1300 - 3600}$ 95 10 AAD 2019 D ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 400 - 4000}$ 95 11 SIRUNYAN 2019 AY CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$ $> 4300$ 95 12 SIRUNYAN 2019 CP CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit W}}{{\mathit H}}$ , ${{\mathit \ell}}{{\mathit \nu}}$ $> 2600$ 95 13 SIRUNYAN 2019 I CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\text{none 1000 - 3000}$ 95 14 AABOUD 2018 AF ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 500 - 2820}$ 95 15 AABOUD 2018 AI ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\text{none 300 - 3000}$ 95 16 AABOUD 2018 AK ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 800 - 3200}$ 95 17 AABOUD 2018 AL ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $> 5100$ 95 18 AABOUD 2018 BG ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $\text{none 250 - 2460}$ 95 19 AABOUD 2018 CH ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 1200 - 3300}$ 95 20 AABOUD 2018 F ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 500 - 3700}$ 95 21 AABOUD 2018 K ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$ $\text{none 1000 - 3600}$ 95 22 SIRUNYAN 2018 CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 1000 - 3050}$ 95 23 SIRUNYAN 2018 AX CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 400 - 5200}$ 95 24 SIRUNYAN 2018 AZ CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $\text{none 1000 - 3400}$ 95 25 SIRUNYAN 2018 BK CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 600 - 3300}$ 95 26 SIRUNYAN 2018 BO CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 900 - 4400}$ 95 27 SIRUNYAN 2018 CV CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ $\text{none 800 - 2330}$ 95 28 SIRUNYAN 2018 DJ CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $> 2800$ 95 29 SIRUNYAN 2018 ED CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\text{none 1200 - 3200, 3300 - 3600}$ 95 30 SIRUNYAN 2018 P CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $>3600$ 95 31 AABOUD 2017 AK ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 1100 - 2500}$ 95 32 AABOUD 2017 AO ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $> 2220$ 95 33 AABOUD 2017 B ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $> 2300$ 95 34 KHACHATRYAN 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 35 KHACHATRYAN 2017 W CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $> 4100$ 95 36 KHACHATRYAN 2017 Z CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $> 2200$ 95 37 SIRUNYAN 2017 A CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $>2300$ 95 38 SIRUNYAN 2017 AK CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit W}}{{\mathit H}}$ $> 2900$ 95 39 SIRUNYAN 2017 H CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit N}}$ $> 2600$ 95 40 SIRUNYAN 2017 I CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $>2450$ 95 41 SIRUNYAN 2017 R CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\text{none 2780 - 3150}$ 95 41 SIRUNYAN 2017 R CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $> 2600$ 95 42 AABOUD 2016 AE ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $> 4070$ 95 43 AABOUD 2016 V ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $>1810$ 95 44 AAD 2016 R ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $>2600$ 95 45 AAD 2016 S ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $> 2150$ 95 46 KHACHATRYAN 2016 AO CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 1000 - 1600}$ 95 47 KHACHATRYAN 2016 AP CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\text{none 800 - 1500}$ 95 48 KHACHATRYAN 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 49 KHACHATRYAN 2016 K CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 500 - 1600}$ 95 50 KHACHATRYAN 2016 L CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 300 - 2700}$ 95 51 KHACHATRYAN 2016 O CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$ $\text{none 400 - 1590}$ 95 52 AAD 2015 AU ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 1500 - 1760}$ 95 53 AAD 2015 AV ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 300 - 1490}$ 95 54 AAD 2015 AZ ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 1300 - 1500}$ 95 55 AAD 2015 CP ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 500 - 1920}$ 95 56 AAD 2015 R ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 800 - 2450}$ 95 57 AAD 2015 V ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $> 1470$ 95 58 KHACHATRYAN 2015 C CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $>3710$ 95 59 KHACHATRYAN 2015 T CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $\text{none 1000 - 3010}$ 95 60 KHACHATRYAN 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. • • 61 AAD 2020 AD ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit J}}{{\mathit J}}$ 62 AAD 2020 W ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ 63 AABOUD 2019 BB ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit j}}{{\mathit \ell}}{{\mathit \ell}}$ 64 SIRUNYAN 2019 V CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit B}}{{\mathit t}}$ , ${{\mathit T}}{{\mathit b}}$ 65 AABOUD 2018 AA ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \gamma}}$ 66 AABOUD 2018 AD ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ $> 4500$ 95 67 AABOUD 2018 CJ ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit W}}{{\mathit H}}$ , ${{\mathit \ell}}{{\mathit \nu}}$ 68 KHACHATRYAN 2017 U CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ 69 AAD 2015 BB ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}$ $\text{none 300 - 880}$ 95 70 AALTONEN 2015 C CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 1200 - 1900 and 2000 - 2200}$ 95 71 KHACHATRYAN 2015 V CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $>3240$ 95 AAD 2014 AI ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ 72 AAD 2014 AT ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \gamma}}$ $\text{none 200 - 1520}$ 95 73 AAD 2014 S ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 1000 - 1700}$ 95 74 KHACHATRYAN 2014 CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ 75 KHACHATRYAN 2014 A CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 500 - 950}$ 95 76 AAD 2013 AO ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 1100 - 1680}$ 95 AAD 2013 D ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 1000 - 1920}$ 95 CHATRCHYAN 2013 A CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ 77 CHATRCHYAN 2013 AJ CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $> 2900$ 95 78 CHATRCHYAN 2013 AQ CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $\text{none 800 - 1510}$ 95 79 CHATRCHYAN 2013 E CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 700 - 940}$ 95 80 CHATRCHYAN 2013 U CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 700 - 1130}$ 95 81 AAD 2012 AV ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 200 - 760}$ 95 82 AAD 2012 BB ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ 83 AAD 2012 CK ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$ $> 2550$ 95 84 AAD 2012 CR ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ 85 AAD 2012 M ATLS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ 86 AALTONEN 2012 N CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$ $\text{none 200 - 1143}$ 95 82 CHATRCHYAN 2012 AF CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ 87 CHATRCHYAN 2012 AR CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\overline{\mathit t}}}{{\mathit q}}$ 88 CHATRCHYAN 2012 BG CMS ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \ell}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit j}}{{\mathit j}}$ $> 1120$ 95 AALTONEN 2011 C CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ $\text{none 180 - 690}$ 95 89 ABAZOV 2011 H D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 600 - 863}$ 95 90 ABAZOV 2011 L D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 285 - 516}$ 95 91 AALTONEN 2010 N CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $\text{none 280 - 840}$ 95 92 AALTONEN 2009 AC CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $> 1000$ 95 ABAZOV 2008 C D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ $\text{none 300 - 800}$ 95 ABAZOV 2004 C D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $\text{none 225 - 536}$ 95 93 ACOSTA 2003 B CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ $\text{none 200 - 480}$ 95 94 AFFOLDER 2002 C CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$ $>786$ 95 95 AFFOLDER 2001 I CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \mu}}{{\mathit \nu}}$ $\text{none 300 - 420}$ 95 96 ABE 1997 G CDF ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ $>720$ 95 97 ABACHI 1996 C D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ $>610$ 95 98 ABACHI 1995 E D0 ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ , ${{\mathit \tau}}{{\mathit \nu}}$ $\text{none 260 - 600}$ 95 99 RIZZO 1993 RVUE ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ 1  SIRUNYAN 2021Y search for resonances decaying to ${{\mathit t}}{{\mathit b}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 2 for limits on ${{\mathit \sigma}}$ $\cdot{}$ B( ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ ). 2  AAD 2020AJ 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 M$_{{{\mathit W}^{\,'}} }$ $>$ 2900 GeV for ${{\mathit g}_{{V}}}$ = 1. See their Fig. 6 for limits on $\sigma \cdot{}B$. 3  AAD 2020AT 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 ${{\mathit M}}$ $_{{{\mathit W}^{\,'}} }$ $>$ 3900 GeV for ${{\mathit g}_{{V}}}$ = 1. See their Fig. 13 for limits on $\sigma \cdot{}B$. 4  AAD 2020T search for ${{\mathit W}^{\,'}}$ with SM-like couplings in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 4(c) for limits on the product of the cross section, acceptance, and branching fraction. 5  SIRUNYAN 2020AI limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. 6  SIRUNYAN 2020Q 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. 7  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. 8  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 $\sigma \cdot{}\mathit B$. 9  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 $\sigma \cdot{}B$. 10  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 $\sigma \cdot{}B$. 11  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. 12  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 $\sigma \cdot{}B$. 13  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 $\mathit M_{{{\mathit W}^{\,'}} }$ = $\mathit M_{{{\mathit Z}^{\,'}} }$. 14  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 ${{\mathit W}^{\,'}}$ . 15  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 $\sigma \cdot{}\mathit B$. 16  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. 17  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. 18  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 $\sigma \cdot{}{{\mathit B}}$ . 19  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. 20  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 $\sigma \cdot{}{{\mathit B}}$ . 21  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 $\sigma \cdot{}{{\mathit B}}$ . 22  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. 23  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. 24  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 $\sigma \cdot{}B$. 25  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. 26  SIRUNYAN 2018BO limit is for ${{\mathit W}^{\,'}}$ with SM-like coupling using ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. 27  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. 28  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. 29  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. 30  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. 31  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. 32  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 $\sigma \cdot{}{{\mathit B}}$ . 33  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 ${{\mathit \sigma}}$ $\cdot{}{{\mathit B}}$ . 34  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. 35  KHACHATRYAN 2017W search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. 36  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. 37  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 $\sigma \cdot{}\mathit B$. 38  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 ${{\mathit \sigma}}$ $\cdot{}{{\mathit B}}$ . 39  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. 40  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 ${{\mathit M}}$ $_{{{\mathit \nu}_{{R}}} }{}\ll$ ${{\mathit M}}$ $_{{{\mathit W}^{\,'}} }$. 41  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 ${{\mathit \sigma}}$ $\cdot{}{{\mathit B}}$ . 42  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 $\mathit M_{{{\mathit W}^{\,'}} }$ = $\mathit M_{{{\mathit Z}^{\,'}} }$. 43  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. 44  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 ${{\mathit g}}$ $_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/{{\mathit g}}$ $_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = (${{\mathit M}_{{W}}}$ /${{\mathit M}}$ $_{{{\mathit W}^{\,'}} }){}^{2}$. 45  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. 46  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. 47  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. 48  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. 49  KHACHATRYAN 2016K search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. 50  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. 51  KHACHATRYAN 2016O limit is for ${{\mathit W}^{\,'}}$ having universal couplings. Interferences with the SM amplitudes are assumed to be absent. 52  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{W}/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 53  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. 54  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}} }/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 55  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}} }/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 56  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. 57  AAD 2015V search for new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. 58  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = $\mathit M_{W}$ $\mathit M_{Z}/\mathit M{}^{2}_{{{\mathit W}^{\,'}} }$. 59  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. 60  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. 61  AAD 2020AD search for a narrow resonance decaying to a pair of large-radius-jets ${{\mathit J}_{{1}}}$ and ${{\mathit J}_{{2}}}$ employing a machine-learning procedure. See their Fig. 3 for limits on $\sigma \cdot{}B$ depending on assumptions about invariant masses for ${{\mathit J}_{{1}}}$ , ${{\mathit J}_{{2}}}$ , and ${{\mathit J}_{{1}}}{{\mathit J}_{{2}}}$ . 62  AAD 2020W search for ${{\mathit W}^{\,'}}$ decaying to ${{\mathit W}}{{\mathit Z}^{\,'}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 5(b) for limits on $\sigma \cdot{}B$ as a function of ${\mathit m}_{{{\mathit Z}^{\,'}}}$. The ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}^{\,'}}$ branching fraction was chosen to be 0.5 and the mass difference between the ${{\mathit W}^{\,'}}$ and ${{\mathit Z}^{\,'}}$ was set to 250 GeV. 63  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. 64  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 ${{\mathit \sigma}}$ $\cdot{}{{\mathit B}}$ . 65  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. 66  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. 67  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. 68  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 $\sigma \cdot{}\mathit B$. 69  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. 70  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 $\mathit g_{{{\mathit W}^{\,'}} }/\mathit g_{{{\mathit W}} }$. 71  KHACHATRYAN 2015V search new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. 72  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. 73  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}} }/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 74  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 ${{\mathit g}}$ $_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/{{\mathit g}}$ $_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = (${{\mathit M}_{{W}}}$ /${{\mathit M}}$ $_{{{\mathit W}^{\,'}} }){}^{2}$. 75  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. 76  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}} }/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 77  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. 78  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. 79  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. 80  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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}} }/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 81  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. 82  AAD 2012BB use ${{\mathit p}}{{\mathit p}}$ collisions data at $\sqrt {s }$=7 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}} }/\mathit M_{{{\mathit W}^{\,'}} }){}^{2}$. 83  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. 84  AAD 2012CR use ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV. 85  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. 86  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. 87  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. 88  CHATRCHYAN 2012BG search for right-handed ${{\mathit W}_{{R}}}$ in ${{\mathit p}}{{\mathit p}}$ 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. 89  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. 90  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. 91  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. 92  AALTONEN 2009AC search for new particle decaying to dijets using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.96 TeV. 93  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. 94  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. 95  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. 96  ABE 1997G search for new particle decaying to dijets using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.8 TeV. 97  For bounds on ${{\mathit W}_{{R}}}$ with nonzero right-handed mass, see Fig.$~$5 from ABACHI 1996C. 98  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 ${\mathit m}_{{{\mathit W}^{\,'}}}$. 99  RIZZO 1993 analyses CDF limit on possible two-jet resonances. The limit is sensitive to the inclusion of the assumed ${{\mathit K}}$ factor.

References:

SIRUNYAN 2021Y PL B820 136535 Search for W? bosons decaying to a top and a bottom quark at s=13TeV in the hadronic final state AAD 2020T JHEP 2003 145 Search for new resonances in mass distributions of jet pairs using 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector AAD 2020AJ PR D102 112008 Search for resonances decaying into a weak vector boson and a Higgs boson in the fully hadronic final state produced in proton$-$proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector AAD 2020W JHEP 2006 151 Search for dijet resonances in events with an isolated charged lepton using $\sqrt{s} = 13$ TeV proton-proton collision data collected by the ATLAS detector AAD 2020AT EPJ C80 1165 Search for heavy diboson resonances in semileptonic final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector AAD 2020AD PRL 125 131801 Dijet resonance search with weak supervision using $\sqrt{s}=13$ TeV $pp$ collisions in the ATLAS detector SIRUNYAN 2020Q EPJ C80 237 A multi-dimensional search for new heavy resonances decaying to boosted WW, WZ, or ZZ boson pairs in the dijet final state at 13 TeV SIRUNYAN 2020AI JHEP 2005 033 Search for high mass dijet resonances with a new background prediction method in proton-proton collisions at $\sqrt{s} =$ 13 TeV AABOUD 2019E PL B788 347 Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector 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 2019BB PL B798 134942 Search for a right-handed gauge boson decaying into a high-momentum heavy neutrino and a charged lepton in $pp$ collisions with the ATLAS detector at $\sqrt{s}=13$ TeV AAD 2019C PR D100 052013 Search for a heavy charged boson in events with a charged lepton and missing transverse momentum from $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector AAD 2019D JHEP 1909 091 Search for diboson resonances in hadronic final states in 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector Also JHEP 2006 042 (errat.) Search for diboson resonances in hadronic final states in 139 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector SIRUNYAN 2019V JHEP 1903 127 Search for a W? boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state SIRUNYAN 2019I JHEP 1901 051 Search for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV SIRUNYAN 2019CP PL B798 134952 Combination of CMS searches for heavy resonances decaying to pairs of bosons or leptons SIRUNYAN 2019AY PL B792 107 Search for a W' boson decaying to a $\tau$ lepton and a neutrino in proton-proton collisions at $\sqrt{s} =$ 13 TeV AABOUD 2018AF PL B781 327 Search for $W' \rightarrow tb$ decays in the hadronic final state using pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector 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 AABOUD 2018K PRL 120 161802 Search for High-Mass Resonances Decaying to $\tau\nu$ in pp Collisions at $\sqrt{s}$=13??TeV with the ATLAS Detector AABOUD 2018AL JHEP 1803 009 Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector AABOUD 2018CJ PR D98 052008 Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36??fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector AABOUD 2018AI JHEP 1803 174 Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector Also JHEP 1811 051 (errat.) Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector 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 2018F PL B777 91 Search for Diboson Resonances with Boson-Tagged Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector AABOUD 2018AA PR D98 032015 Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\sqrt{s}=13$ $\mathrm{TeV}$ with the ATLAS detector AABOUD 2018AD PL B779 24 A search for resonances decaying into a Higgs boson and a new particle $X$ in the $XH \to qqbb$ final state with the ATLAS detector SIRUNYAN 2018 PL B777 39 Search for Heavy Resonances Decaying to a Top Quark and a Bottom Quark in the Lepton+Jets Final State in Proton-Proton Collisions at 13 TeV SIRUNYAN 2018P PR D97 072006 Search for massive resonances decaying into $WW$, $WZ$, $ZZ$, $qW$, and $qZ$ with dijet final states at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$ SIRUNYAN 2018BK JHEP 1807 075 Search for a heavy resonance decaying into a Z boson and a vector boson in the $ \nu \overline{\nu}\mathrm{q}\overline{\mathrm{q}} $ final state 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 2018ED JHEP 1811 172 Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV 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 2018AZ JHEP 1806 128 Search for high-mass resonances in final states with a lepton and missing transverse momentum at $ \sqrt{s}=13 $ TeV SIRUNYAN 2018CV JHEP 1805 148 Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at $\sqrt{s}=$ 13 TeV SIRUNYAN 2018BO JHEP 1808 130 Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles AABOUD 2017AO PL B774 494 Search for Heavy Resonances Decaying to a ${{\mathit W}}$ or ${{\mathit Z}}$ Boson and a Higgs Boson in the ${\mathit {\mathit q}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Final State in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector AABOUD 2017AK PR D96 052004 Search for New Phenomena in Dijet Events using 37 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collision Data Collected at $\sqrt {s }$ = 13 TeV with the ATLAS Detector AABOUD 2017B PL B765 32 Search for New Resonances Decaying to a ${{\mathit W}}$ or ${{\mathit Z}}$ Boson and a Higgs Boson in the ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$, ${{\mathit \ell}}{{\mathit \nu}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$, and ${{\mathit \nu}}{{\overline{\mathit \nu}}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Channels with ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector 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 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 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 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 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 2016AE JHEP 1609 173 Searches for Heavy Diboson Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector 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 AAD 2016R 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 AAD 2016S 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 KHACHATRYAN 2016AO JHEP 1602 122 Search for ${{\mathit W}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ 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 2016O PL B755 196 Search for ${{\mathit W}^{\,'}}$ Decaying to Tau Lepton and Neutrino 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 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 AAD 2015AV 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 AAD 2015AU 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 AAD 2015V 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 AAD 2015R 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 AAD 2015CP 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 AAD 2015AZ 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 Also EPJ C75 370 (errat.) Search for Production of WW/WZ Resonances Decaying to a Lepton, Neutrino and Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector AAD 2015BB 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 2015V PR D91 052009 Search for Resonances and Quantum Black Holes using Dijet Mass Spectra 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 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 AAD 2014S 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 AAD 2014AI 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 AAD 2014AT 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 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 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 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 AAD 2013D 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 AAD 2013AO 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 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 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 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 AAD 2012CK 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 AAD 2012BB 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 AAD 2012AV 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 AAD 2012M 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 AAD 2012CR 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 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 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 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 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