$\bf{
> 5200}$
|
OUR LIMIT
|
|
|
1 |
|
ATLS |
$\text{none 500 - 3250}$ |
95 |
2 |
|
ATLS |
$> 6000$ |
95 |
3 |
|
ATLS |
$\text{none 1300 - 3600}$ |
95 |
4 |
|
ATLS |
$\text{none 400 - 4000}$ |
95 |
5 |
|
CMS |
$> 4300$ |
95 |
6 |
|
CMS |
$> 2600$ |
95 |
7 |
|
CMS |
$\text{none 1000 - 3000}$ |
95 |
8 |
|
ATLS |
$\text{none 500 - 2820}$ |
95 |
9 |
|
ATLS |
$\text{none 300 - 3000}$ |
95 |
10 |
|
ATLS |
$\text{none 800 - 3200}$ |
95 |
11 |
|
ATLS |
$> 5100$ |
95 |
12 |
|
ATLS |
$\text{none 250 - 2460}$ |
95 |
13 |
|
ATLS |
$\text{none 1200 - 3300}$ |
95 |
14 |
|
ATLS |
$\text{none 500 - 3700}$ |
95 |
15 |
|
ATLS |
$\text{none 1000 - 3600}$ |
95 |
16 |
|
CMS |
$\text{none 1000 - 3050}$ |
95 |
17 |
|
CMS |
$\bf{\text{none 400 - 5200}}$ |
95 |
18 |
|
CMS |
$\text{none 1000 - 3400}$ |
95 |
19 |
|
CMS |
$\text{none 600 - 3300}$ |
95 |
20 |
|
CMS |
$\text{none 900 - 4400}$ |
95 |
21 |
|
CMS |
$\text{none 800 - 2330}$ |
95 |
22 |
|
CMS |
$> 2800$ |
95 |
23 |
|
CMS |
$\text{none 1200 - 3200, 3300 - 3600}$ |
95 |
24 |
|
CMS |
$>3600$ |
95 |
25 |
|
ATLS |
$\text{none 1100 - 2500}$ |
95 |
26 |
|
ATLS |
$> 2220$ |
95 |
27 |
|
ATLS |
$> 2300$ |
95 |
28 |
|
CMS |
$\text{none 600 - 2700}$ |
95 |
29 |
|
CMS |
$> 4100$ |
95 |
30 |
|
CMS |
$> 2200$ |
95 |
31 |
|
CMS |
$>2300$ |
95 |
32 |
|
CMS |
$> 2900$ |
95 |
33 |
|
CMS |
$> 2600$ |
95 |
34 |
|
CMS |
$>2450$ |
95 |
35 |
|
CMS |
$\text{none 2780 - 3150}$ |
95 |
35 |
|
CMS |
$> 2600$ |
95 |
36 |
|
ATLS |
$> 4070$ |
95 |
37 |
|
ATLS |
$>1810$ |
95 |
38 |
|
ATLS |
$>2600$ |
95 |
39 |
|
ATLS |
$> 2150$ |
95 |
40 |
|
CMS |
$\text{none 1000 - 1600}$ |
95 |
41 |
|
CMS |
$\text{none 800 - 1500}$ |
95 |
42 |
|
CMS |
$\text{none 1500 - 2600}$ |
95 |
43 |
|
CMS |
$\text{none 500 - 1600}$ |
95 |
44 |
|
CMS |
$\text{none 300 - 2700}$ |
95 |
45 |
|
CMS |
$\text{none 400 - 1590}$ |
95 |
46 |
|
ATLS |
$\text{none 1500 - 1760}$ |
95 |
47 |
|
ATLS |
$\text{none 300 - 1490}$ |
95 |
48 |
|
ATLS |
$\text{none 1300 - 1500}$ |
95 |
49 |
|
ATLS |
$\text{none 500 - 1920}$ |
95 |
50 |
|
ATLS |
$\text{none 800 - 2450}$ |
95 |
51 |
|
ATLS |
$> 1470$ |
95 |
52 |
|
CMS |
$>3710$ |
95 |
53 |
|
CMS |
$\text{none 1000 - 3010}$ |
95 |
54 |
|
CMS |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
|
|
55 |
|
ATLS |
|
|
56 |
|
CMS |
|
|
57 |
|
ATLS |
|
|
58 |
|
ATLS |
$> 4500$ |
95 |
59 |
|
ATLS |
|
|
60 |
|
CMS |
|
|
61 |
|
ATLS |
$\text{none 300 - 880}$ |
95 |
62 |
|
CDF |
$\text{none 1200 - 1900 and 2000 - 2200}$ |
95 |
63 |
|
CMS |
$>3240$ |
95 |
|
|
ATLS |
|
|
64 |
|
ATLS |
$\text{none 200 - 1520}$ |
95 |
65 |
|
ATLS |
$\text{none 1000 - 1700}$ |
95 |
66 |
|
CMS |
|
|
67 |
|
CMS |
$\text{none 500 - 950}$ |
95 |
68 |
|
ATLS |
$\text{none 1100 - 1680}$ |
95 |
|
|
ATLS |
$\text{none 1000 - 1920}$ |
95 |
|
|
CMS |
|
|
69 |
|
CMS |
$> 2900$ |
95 |
70 |
|
CMS |
$\text{none 800 - 1510}$ |
95 |
71 |
|
CMS |
$\text{none 700 - 940}$ |
95 |
72 |
|
CMS |
$\text{none 700 - 1130}$ |
95 |
73 |
|
ATLS |
$\text{none 200 - 760}$ |
95 |
74 |
|
ATLS |
|
|
75 |
|
ATLS |
$> 2550$ |
95 |
76 |
|
ATLS |
|
|
77 |
|
ATLS |
|
|
78 |
|
CDF |
$\text{none 200 - 1143}$ |
95 |
74 |
|
CMS |
|
|
79 |
|
CMS |
|
|
80 |
|
CMS |
$> 1120$ |
95 |
|
|
CDF |
$\text{none 180 - 690}$ |
95 |
81 |
|
D0 |
$\text{none 600 - 863}$ |
95 |
82 |
|
D0 |
$\text{none 285 - 516}$ |
95 |
83 |
|
CDF |
$\text{none 280 - 840}$ |
95 |
84 |
|
CDF |
$> 1000$ |
95 |
|
|
D0 |
$\text{none 300 - 800}$ |
95 |
|
|
D0 |
$\text{none 225 - 536}$ |
95 |
85 |
|
CDF |
$\text{none 200 - 480}$ |
95 |
86 |
|
CDF |
$>786$ |
95 |
87 |
|
CDF |
$\text{none 300 - 420}$ |
95 |
88 |
|
CDF |
$>720$ |
95 |
89 |
|
D0 |
$>610$ |
95 |
90 |
|
D0 |
$\text{none 260 - 600}$ |
95 |
91 |
|
RVUE |
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.
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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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
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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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
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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.
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AAD 2015V search for new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.
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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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = $\mathit M_{W}$ $\mathit M_{Z}/\mathit M{}^{2}_{{{\mathit W}^{\,'}}}$.
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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.
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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.
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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.
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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 ${{\mathit \sigma}}\cdot{}{{\mathit B}}$.
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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.
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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.
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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.
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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 $\sigma \cdot{}\mathit B$.
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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.
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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 $\mathit g_{{{\mathit W}^{\,'}}}/\mathit g_{{{\mathit W}}}$.
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KHACHATRYAN 2015V search new resonance decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.
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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.
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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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
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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 ${{\mathit g}}_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/{{\mathit g}}_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = (${{\mathit M}_{{W}}}/{{\mathit M}}_{{{\mathit W}^{\,'}}}){}^{2}$.
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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.
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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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
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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.
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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.
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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.
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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 $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
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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.
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AAD 2012BB use ${{\mathit p}}{{\mathit p}}$ collisions data at $\sqrt {s }$=7 TeV. The quoted limit assumes $\mathit g_{ {{\mathit W}^{\,'}} {{\mathit W}} {{\mathit Z}} }/\mathit g_{ {{\mathit W}} {{\mathit W}} {{\mathit Z}} }$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit W}^{\,'}}}){}^{2}$.
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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.
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AAD 2012CR use ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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AALTONEN 2009AC search for new particle decaying to dijets using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.96 TeV.
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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.
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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.
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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.
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ABE 1997G search for new particle decaying to dijets using ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$=1.8 TeV.
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89
For bounds on ${{\mathit W}_{{R}}}$ with nonzero right-handed mass, see Fig.$~$5 from ABACHI 1996C.
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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 ${\mathit m}_{{{\mathit W}^{\,'}}}$.
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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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