$\bf{> 4.25}$ |
95 |
1 |
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CMS |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
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2 |
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ATLS |
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3 |
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ATLS |
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4 |
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ATLS |
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5 |
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ATLS |
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6 |
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CMS |
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7 |
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CMS |
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8 |
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CMS |
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9 |
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ATLS |
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10 |
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ATLS |
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11 |
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ATLS |
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12 |
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ATLS |
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13 |
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ATLS |
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14 |
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ATLS |
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15 |
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ATLS |
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16 |
|
CMS |
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17 |
|
CMS |
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18 |
|
CMS |
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19 |
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CMS |
$> 1.8$ |
95 |
20 |
|
CMS |
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|
21 |
|
CMS |
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|
22 |
|
CMS |
$> 4.1$ |
95 |
23 |
|
CMS |
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|
24 |
|
CMS |
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|
25 |
|
CMS |
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|
26 |
|
CMS |
$> 4.1$ |
95 |
27 |
|
ATLS |
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|
28 |
|
ATLS |
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|
29 |
|
ATLS |
|
|
30 |
|
ATLS |
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|
31 |
|
ATLS |
$> 2.68$ |
95 |
32 |
|
ATLS |
$\text{>1.23 (>0.84)}$ |
95 |
33 |
|
ATLS |
$\text{>0.94 (>0.71)}$ |
95 |
34 |
|
ATLS |
$> 2.23$ |
95 |
35 |
|
ATLS |
$> 0.845$ |
95 |
36 |
|
ATLS |
|
|
37 |
|
CDF |
|
|
38 |
|
RVUE |
|
|
39 |
|
CDF |
$> 1.058$ |
95 |
40 |
|
CDF |
$> 0.754$ |
95 |
41 |
|
D0 |
$> 0.607$ |
|
42 |
|
CDF |
$> 1.05$ |
|
43 |
|
D0 |
|
|
44 |
|
CDF |
$> 0.90$ |
|
45 |
|
D0 |
|
|
46 |
|
CDF |
$> 0.889$ |
|
47 |
|
CDF |
$> 0.785$ |
|
48 |
|
D0 |
$> 0.71$ |
|
49 |
|
CDF |
1
SIRUNYAN 2018BB use 35.9 (36.3) fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for dilepton resonances in the dielectron (dimuon) channel. See their paper for other limits with warp parameter values $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.01 and 0.05. This updates the results of KHACHATRYAN 2017T.
|
2
AAD 2020C use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit W}^{+}}{{\mathit W}^{-}}$ , and ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ final states. See their Figure 5(b)(c) for limits on the cross section as a function of the KK graviton mass. In the case of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1 and 2, gravitons are excluded in the mass range $260 - 3000$ GeV and $260 - 1760$ GeV, respectively.
|
3
AABOUD 2019A use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ final state. See their Figure 9 for limits on the cross section times branching fraction as a function of the KK graviton mass. Assuming $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1, gravitons in the mass range $313 - 1362$ GeV are excluded. This updates the results of AABOUD 2016I.
|
4
AABOUD 2019O use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit W}}{{\mathit W}}$ final state. See their Figure 12 for limits on the cross section times branching fraction as a function of the KK graviton mass for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1 and $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 2.
|
5
AAD 2019D use 139 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for diboson resonances in the all-hadronic final state. See their Figure 9(b) for the limit on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1. This updates the results of AABOUD 2018F.
|
6
SIRUNYAN 2019 use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit b}}{{\overline{\mathit b}}}$ final state. See their Figure 9 for limits on the cross section times branching fraction as a function of the KK graviton mass. Assuming $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1, gravitons in the mass range $290 - 810$ GeV are excluded. This updates the result of KHACHATRYAN 2016BQ.
|
7
SIRUNYAN 2019BE use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production by combining the results from four final states: ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \tau}}{{\overline{\mathit \tau}}}$ , ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ , and ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit V}}{{\mathit V}}$ . See their Figure 7 for limits on the cross section times branching fraction as a function of the KK graviton mass.
|
8
SIRUNYAN 2019CF use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit q}}{{\overline{\mathit q}}^{\,'}}{{\mathit \ell}}{{\mathit \nu}}$ final state. See their Figure 7 for limits on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1 and 0.3.
|
9
AABOUD 2018AK use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for ${{\mathit W}}{{\mathit W}}$ resonances in ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}}$ final states (${{\mathit \ell}}={{\mathit e}}$, ${{\mathit \mu}}$). See their Figure 7(d) for the limit on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1. This updates the results of AABOUD 2016AE.
|
10
AABOUD 2018AL use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for diboson resonances in the ${{\mathit \ell}}{{\mathit \ell}}{{\mathit q}}{{\overline{\mathit q}}}$ and ${{\mathit \nu}}{{\overline{\mathit \nu}}}{{\mathit q}}{{\overline{\mathit q}}}$ final states. See their Figure 14 for the limit on cross section times branching fraction as a function of the the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5 and 1. This updates the results of AABOUD 2016AE.
|
11
AABOUD 2018BF use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for ${{\mathit Z}}{{\mathit Z}}$ resonances in the ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \ell}}{{\mathit \ell}}$ and ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \nu}}{{\overline{\mathit \nu}}}$ final states (${{\mathit \ell}}={{\mathit e}}$, ${{\mathit \mu}}$). See their Figure 10 for the limit on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1.
|
12
AABOUD 2018BI use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for top-quark pairs decaying into the lepton-plus jets topology. See their Figure 16 for the limit on the KK graviton mass as a function of the cross section times branching fraction, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1.
|
13
AABOUD 2018CJ combine the searches for heavy resonances decaying into bosonic and leptonic final states from 36.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\sqrt {s }$ = 13 TeV. The lower limit on the KK graviton mass, with $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1, is 2.3 TeV.
|
14
AABOUD 2018CQ use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ final state. See their Figure 2 for limits on the cross section times branching fraction as a function of the KK graviton mass. Assuming $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 1, gravitons in the mass range $325 - 885$ GeV are excluded.
|
15
AABOUD 2018CW use 36.1 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit b}}{{\overline{\mathit b}}}$ final state. See their Figure 7 for limits on the cross section times branching fraction as a function of the KK graviton mass.
|
16
SIRUNYAN 2018AF use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ final state. See their Figure 9 for limits on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5. This updates the results of KHACHATRYAN 2015R.
|
17
SIRUNYAN 2018AS use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for ${{\mathit Z}}{{\mathit Z}}$ resonances in the ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \nu}}{{\overline{\mathit \nu}}}$ final state (${{\mathit \ell}}={{\mathit e}}$, ${{\mathit \mu}}$). See their Figure 5 for the limit on the KK graviton mass as a function of the cross section times branching fraction, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1, 0.5, and 1.0.
|
18
SIRUNYAN 2018AX use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for WW resonances in ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}}$ final states (${{\mathit \ell}}={{\mathit e}}$, ${{\mathit \mu}}$). See their Figure 6 for the limit on the KK graviton mass as a function of the cross section times branching fraction, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5. This updates the results of KHACHATRYAN 2014A.
|
19
SIRUNYAN 2018BK use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for ${{\mathit Z}}{{\mathit Z}}$ resonances in the ${{\mathit \nu}}{{\overline{\mathit \nu}}}{{\mathit q}}{{\overline{\mathit q}}}$ final state. See their Figure 4 for the limit on the KK graviton mass as a function of the cross section times branching fraction, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5 .
|
20
SIRUNYAN 2018BO use up to 36 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for dijet resonances. Besides the quoted bound, KK graviton masses between 1.9 TeV and 2.5 TeV are also excluded. See their Figure 11 for the limit on the product of the cross section, branching fraction and acceptance as a function of the KK graviton mass. This updates the results of KHACHATRYAN 2017W.
|
21
SIRUNYAN 2018CW use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ final state. See their Figure 8 for limits on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5.
|
22
SIRUNYAN 2018DJ use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for ${{\mathit Z}}{{\mathit Z}}$ resonances in 2 ${{\mathit \ell}}$2 ${{\mathit q}}$ final states (${{\mathit \ell}}$ = ${{\mathit e}}$, ${{\mathit \mu}}$). See their Figure 6 for the limit on the KK graviton mass as a function of the cross section times branching fraction. Assuming $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5, a graviton mass is excluded below 925 GeV.
|
23
SIRUNYAN 2018DU use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV, in the diphoton channel to place a lower limit on the mass of the lightest KK graviton. See their paper for limits with other warp parameter values $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.01 and 0.2. This updates the results of KHACHATRYAN 2016M.
|
24
SIRUNYAN 2018F use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for Higgs boson pair production in the ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ final state. See their Figure 7 for limits on the cross section times branching fraction as a function of the KK graviton mass, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1.
|
25
SIRUNYAN 2018I use 19.7 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for narrow resonances decaying to bottom quark pairs. See their Figure 3 for the limit on the KK graviton mass as a function of the cross section times branching fraction in the mass range of $325 - 1200$ GeV.
|
26
SIRUNYAN 2018P use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for diboson resonances with dijet final states. See their Figure 6 for the limit on the KK graviton mass as a function of the cross section times branching fraction, including theoretical values for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.5. This updates the results of SIRUNYAN 2017AK.
|
27
AABOUD 2017AP use 36.7 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV in the diphoton channel to place a lower limit on the mass of the lightest KK graviton. This updates the results of AABOUD 2016H.
|
28
AAD 2016R use 20.3 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to place a lower bound on the mass of the lightest KK graviton. See their Figure 4 for the limit on the KK graviton mass as a function of the cross section times branching fraction.
|
29
AAD 2015AU use 20 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for KK gravitons in a warped extra dimension decaying to ${{\mathit Z}}{{\mathit Z}}$ dibosons. See their Figure 2 for limits on the KK graviton mass as a function of the cross section times branching fraction.
|
30
AAD 2015AZ use 20.3 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to place a lower bound on the mass of the lightest KK graviton. See their Figure 2 for limits on the KK graviton mass as a function of the cross section times branching ratio.
|
31
AAD 2015CT use 20.3 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to place a lower bound on the mass of the lightest KK graviton. See their Figures 6b and 6c for the limit on the KK graviton mass as a function of the cross section times branching fraction.
|
32
AAD 2014V use 20.3 (20.5) fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV in the dielectron (dimuon) channels to place a lower bound on the mass of the lightest KK graviton. This updates the results of AAD 2012CC .
|
33
AAD 2013A use 4.7 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV in the ${{\mathit \ell}}{{\mathit \nu}}{{\mathit \ell}}{{\mathit \nu}}$ channel, to place a lower bound on the mass of the lightest KK graviton.
|
34
AAD 2013AO use 4.7 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV in the ${{\mathit \ell}}{{\mathit \nu}}{{\mathit j}}{{\mathit j}}$ channel, to place a lower bound on the mass of the lightest KK graviton.
|
35
AAD 2013AS use 4.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV in the diphoton channel to place lower limits on the mass of the lightest KK graviton. The diphoton channel is combined with previous results in the dielectron and dimuon channels to set the best limit. See their Table 2 for warp parameter values $\mathit k/{{\overline{\mathit M}}_{{P}}}$ between 0.01 and 0.1. This updates the results of AAD 2012Y .
|
36
AAD 2012AD use 1.02 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV to search for KK gravitons in a warped extra dimension decaying to ${{\mathit Z}}{{\mathit Z}}$ dibosons in the ${{\mathit l}}{{\mathit l}}{{\mathit j}}{{\mathit j}}$ and ${{\mathit l}}{{\mathit l}}{{\mathit l}}{{\mathit l}}$ channels (${{\mathit \ell}}={{\mathit e}}$, ${{\mathit \mu}}$). The limit is quoted for the combined ${{\mathit l}}{{\mathit l}}{{\mathit j}}{{\mathit j}}$ + ${{\mathit l}}{{\mathit l}}{{\mathit l}}{{\mathit l}}$ channels. See their Figure 5 for limits on the cross section ${\mathit \sigma (}$ ${{\mathit G}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}{)}$ as a function of the graviton mass.
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37
AALTONEN 2012V use 6 fb${}^{-1}$ of data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in a warped extra dimension decaying to ${{\mathit Z}}{{\mathit Z}}$ dibosons in the ${{\mathit l}}{{\mathit l}}{{\mathit j}}{{\mathit j}}$ and ${{\mathit l}}{{\mathit l}}{{\mathit l}}{{\mathit l}}$ channels (${{\mathit \ell}}={{\mathit e}}$, ${{\mathit \mu}}$). It provides improved limits over the previous analysis in AALTONEN 2011G. See their Figure 16 for limits from all channels combined on the cross section times branching ratio ${\mathit \sigma (}$ ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit G}^{*}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}{)}$ as a function of the graviton mass.
|
38
BAAK 2012 use electroweak precision observables to place a lower bound on the compactification scale $\mathit k$ $\mathit e{}^{- {{\mathit \pi}} {{\mathit k}} {{\mathit R}} }$, assuming Standard Model fields propagate in the bulk and the Higgs is confined to the IR brane. See their Fig. 27 for more details.
|
39
AALTONEN 2011G use $2.5 - 2.9$ fb${}^{-1}$ of data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in a warped extra dimension decaying to ${{\mathit Z}}{{\mathit Z}}$ dibosons via the ${{\mathit e}}{{\mathit e}}{{\mathit e}}{{\mathit e}}$ , ${{\mathit e}}{{\mathit e}}{{\mathit \mu}}{{\mathit \mu}}$ , ${{\mathit \mu}}{{\mathit \mu}}{{\mathit \mu}}{{\mathit \mu}}$ , ${{\mathit e}}{{\mathit e}}{{\mathit j}}{{\mathit j}}$ , and ${{\mathit \mu}}{{\mathit \mu}}{{\mathit j}}{{\mathit j}}$ channels. See their Fig. 20 for limits on the cross section ${\mathit \sigma (}$ ${{\mathit G}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}{)}$ as a function of the graviton mass.
|
40
AALTONEN 2011R uses 5.7 fb${}^{-1}$ of data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV in the dielectron channel to place a lower bound on the mass of the lightest graviton. It provides combined limits with the diphoton channel analysis of AALTONEN 2011U. For warp parameter values ${{\mathit k}}/{{\overline{\mathit M}}_{{P}}}$ between 0.01 to 0.1 the lower limit on the mass of the lightest graviton is between 612 and 1058 GeV. See their Table I for more details.
|
41
ABAZOV 2011H use 5.4 fb${}^{-1}$ of data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to place a lower bound on the mass of the lightest graviton. Their 95$\%$ C.L. exclusion limit does not include masses less than 300 GeV.
|
42
AALTONEN 2010N use 2.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to place a lower bound on the mass of the lightest graviton.
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43
ABAZOV 2010F use 5.4 fb${}^{-1}$ of data from ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to place a lower bound on the mass of the lightest graviton. For warp parameter values of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ between 0.01 and 0.1 the lower limit on the mass of the lightest graviton is between 560 and 1050 GeV. See their Fig. 3 for more details.
|
44
AALTONEN 2008S use ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to four electrons via two ${{\mathit Z}}$ bosons using 1.1 fb${}^{-1}$ of data. See their Fig. 8 for limits on $\sigma \cdot{}$B( ${{\mathit G}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ ) versus the graviton mass.
|
45
ABAZOV 2008J use ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to electrons and photons using 1 fb${}^{-1}$ of data. For warp parameter values of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ between 0.01 and 0.1 the lower limit on the mass of the lightest excitation is between 300 and 900 GeV. See their Fig. 4 for more details.
|
46
AALTONEN 2007G use ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to photons using 1.2 fb${}^{-1}$ of data. For warp parameter values of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1, 0.05, and 0.01 the bounds on the graviton mass are 850, 694, and 230 GeV, respectively. See their Fig. 3 for more details. See also AALTONEN 2007H.
|
47
AALTONEN 2007H use ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to electrons using 1.3 fb${}^{-1}$ of data. For a warp parameter value of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1 the bound on the graviton mass is 807 GeV. See their Fig. 4 for more details. A combined analysis with the diphoton data of AALTONEN 2007G yields for $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1 a graviton mass lower bound of 889 GeV.
|
48
ABAZOV 2005N use ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to muons, electrons or photons, using 260~pb${}^{-1}$ of data. For warp parameter values of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1, 0.05, and 0.01, the bounds on the graviton mass are 785, 650 and 250$~$GeV respectively. See their Fig.$~$3 for more details.
|
49
ABULENCIA 2005A use ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to muons or electrons, using 200~pb${}^{-1}$ of data. For warp parameter values of $\mathit k/{{\overline{\mathit M}}_{{P}}}$ = 0.1, 0.05, and 0.01, the bounds on the graviton mass are 710, 510 and 170 GeV respectively.
|