• • • We do not use the following data for averages, fits, limits, etc. • • • |
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|
1 |
|
ATLS |
$> 2400$ |
95 |
2 |
|
CMS |
|
|
3 |
|
ATLS |
$>1800$ |
95 |
4 |
|
ATLS |
|
|
5 |
|
ATLS |
|
|
6 |
|
ATLS |
|
|
7 |
|
LHCB |
$> 1140$ |
95 |
8 |
|
CMS |
|
|
9 |
|
CMS |
$\text{none 200 - 700, 750 - 890}$ |
95 |
10 |
|
ATLS |
$\text{none 275 - 960}$ |
95 |
10 |
|
ATLS |
|
|
11 |
|
ATLS |
$> 703$ |
|
12 |
|
ATLS |
$> 494$ |
|
13 |
|
ATLS |
$\text{none 500 - 1740}$ |
95 |
14 |
|
ATLS |
$> 1300$ |
95 |
15 |
|
CMS |
$> 2100$ |
95 |
14 |
|
CMS |
|
|
16 |
|
RVUE |
$\text{none 167 - 687}$ |
95 |
17 |
|
CMS |
$> 805$ |
95 |
14 |
|
CDF |
$> 805$ |
95 |
14 |
|
CDF |
|
|
18 |
|
RVUE |
|
|
19 |
|
RVUE |
|
|
20 |
|
CDF |
$\text{none 208 - 408}$ |
95 |
21 |
|
D0 |
|
|
22 |
|
D0 |
$> 280$ |
95 |
23 |
|
CDF |
|
|
24 |
|
ZEUS |
$>207$ |
95 |
25 |
|
D0 |
$\text{none 90 - 206.7}$ |
95 |
26 |
|
DLPH |
|
|
27 |
|
CDF |
$>600$ |
95 |
28 |
|
CDF |
$\text{none 350 - 440}$ |
95 |
29 |
|
CDF |
|
|
30 |
|
CDF |
$\text{none 260 - 480}$ |
95 |
31 |
|
CDF |
1
AAD 2016W search for color octet vector resonance decaying to ${{\mathit b}}{{\mathit B}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The vector like quark ${{\mathit B}}$ is assumed to decay to ${{\mathit b}}{{\mathit H}}$ . See their Fig.3 and Fig.4 for limits on $\sigma \cdot{}\mathit B$.
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2
KHACHATRYAN 2016E search for top-color ${{\mathit Z}^{\,'}}$ decaying to ${{\mathit t}}{{\overline{\mathit t}}}$ . The quoted limit is for ${\Gamma}_{{\mathit Z}^{\,'}}/{\mathit m}_{{{\mathit Z}^{\,'}}}$ = 0.012. Also exclude ${\mathit m}_{{{\mathit Z}^{\,'}}}$ $<$ 2.9 TeV for wider topcolor ${{\mathit Z}^{\,'}}$ with ${\Gamma}_{{\mathit Z}^{\,'}}/{\mathit m}_{{{\mathit Z}^{\,'}}}$ = 0.1.
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3
AAD 2015AB search for long-lived hidden valley ${{\mathit \pi}_{{v}}}$ particles which are produced in pairs by the decay of a scalar boson. ${{\mathit \pi}_{{v}}}$ is assumed to decay into dijets. See their Fig. 10 for the limit on ${{\mathit \sigma}}\mathit B$.
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4
AAD 2015AO search for top-color ${{\mathit Z}^{\,'}}$ decaying to ${{\mathit t}}{{\overline{\mathit t}}}$ . The quoted limit is for ${\Gamma}_{{\mathit Z}^{\,'}}/{\mathit m}_{{{\mathit Z}^{\,'}}}$ = 0.012.
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5
AAD 2015BB search for minimal walking technicolor (MWT) isotriplet vector and axial-vector resonances decaying to ${{\mathit W}}{{\mathit h}}$ or ${{\mathit Z}}{{\mathit h}}$ . See their Fig. 3 for the exclusion limit in the MWT parameter space.
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6
AAD 2015Q search for long-lived hidden valley ${{\mathit \pi}_{{v}}}$ particles which are produced in pairs by the decay of scalar boson. ${{\mathit \pi}_{{v}}}$ is assumed to decay into dijets. See their Fig. 5 and Fig. 6 for the limit on $\sigma \mathit B$.
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7
AAIJ 2015AN search for long-lived hidden valley ${{\mathit \pi}_{{v}}}$ particles which are produced in pairs by the decay of scalar boson with a mass of 120GeV. ${{\mathit \pi}_{{v}}}$ is assumed to decay into dijets. See their Fig. 4 for the limit on $\sigma \mathit B$.
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8
KHACHATRYAN 2015C search for a vector techni-resonance decaying to ${{\mathit W}}{{\mathit Z}}$ . The limit assumes ${{\mathit M}}_{{{\mathit \pi}_{{T}}}}$ = (3/4) ${{\mathit M}}_{{{\mathit \rho}_{{T}}}}$ $−$ 25 GeV. See their Fig.3 for the limit in ${{\mathit M}}_{{{\mathit \pi}_{{T}}}}−{{\mathit M}}_{{{\mathit \rho}_{{T}}}}$ plane of the low scale technicolor model.
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9
KHACHATRYAN 2015W search for long-lived hidden valley ${{\mathit \pi}_{{v}}}$ particles which are produced in pairs in the decay of heavy higgs boson ${{\mathit H}}$. ${{\mathit \pi}_{{v}}}$ is assumed to decay into ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ . See their Fig. 7 and Fig. 8 for the limits on $\sigma \mathit B$.
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10
AAD 2014AT search for techni-${{\mathit \omega}}$ and techni-${{\mathit a}}$ resonances decaying to ${{\mathit V}}{{\mathit \gamma}}$ with ${{\mathit V}}$ = ${{\mathit W}}$( $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ ) or ${{\mathit Z}}$( $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ ).
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11
AAD 2014V search for vector techni-resonances decaying into electron or muon pairs in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. See their table IX for exclusion limits with various assumptions.
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12
AAD 2013AN search for vector techni-resonance ${{\mathit a}_{{T}}}$ decaying into ${{\mathit W}}{{\mathit \gamma}}$ .
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13
AAD 2013AN search for vector techni-resonance ${{\mathit \omega}_{{T}}}$ decaying into ${{\mathit Z}}{{\mathit \gamma}}$ .
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14
Search for top-color ${{\mathit Z}^{\,'}}$ decaying to ${{\mathit t}}{{\overline{\mathit t}}}$ . The quoted limit is for ${\Gamma}_{{\mathit Z}^{\,'}}/{\mathit m}_{{{\mathit Z}^{\,'}}}$ = 0.012.
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15
CHATRCHYAN 2013AP search for top-color leptophobic ${{\mathit Z}^{\,'}}$ decaying to ${{\mathit t}}{{\overline{\mathit t}}}$ . The quoted limit is for ${\Gamma}_{{\mathit Z}^{\,'}}/{\mathit m}_{{{\mathit Z}^{\,'}}}$ = 0.012.
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16
BAAK 2012 give electroweak oblique parameter constraints on the QCD-like technicolor models. See their Fig. 28.
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17
CHATRCHYAN 2012AF search for a vector techni-resonance decaying to ${{\mathit W}}{{\mathit Z}}$ . The limit assumes $\mathit M_{{{\mathit \pi}_{{T}}}}$= (3/4) $\mathit M_{{{\mathit \rho}_{{T}}}}−$ 25$~$GeV. See their Fig. 3 for the limit in $\mathit M_{{{\mathit \pi}_{{T}}}}−\mathit M~_{{{\mathit \rho}_{{T}}}}$ plane of the low scale technicolor model.
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18
Using the LHC limit on the Higgs boson production cross section, CHIVUKULA 2011 obtain a limit on the top-Higgs mass $>$ 300 GeV at 95$\%$ CL assuming 150 GeV top-pion mass.
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19
Using the LHC limit on the Higgs boson production cross section, CHIVUKULA 2011A obtain a limit on the techinipion mass ruling out the region 110 GeV $<$ ${\mathit m}_{{{\mathit P}}}$ $<$ 2${\mathit m}_{{{\mathit t}}}$. Existence of color techni-fermions, top-color mechanism, and ${{\mathit N}_{{TC}}}{}\geq{}$ 3 are assumed.
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20
AALTONEN 2010I search for the vector techni-resonances (${{\mathit \rho}_{{T}}}$, ${{\mathit \omega}_{{T}}}$) decaying into ${{\mathit W}}{{\mathit \pi}_{{T}}}$ with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ and ${{\mathit \pi}_{{T}}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit b}}{{\overline{\mathit c}}}$ , or ${{\mathit b}}{{\overline{\mathit u}}}$ . See their Fig.$~$3 for the exclusion plot in ${{\mathit M}}_{{{\mathit \pi}_{{T}}}}−{{\mathit M}}_{{{\mathit \rho}_{{T}}}}$ plane.
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21
ABAZOV 2010A search for a vector techni-resonance decaying into ${{\mathit W}}{{\mathit Z}}$ . The limit assumes ${{\mathit M}}_{{{\mathit \rho}_{{T}}}}<$ ${{\mathit M}}_{{{\mathit \pi}_{{T}}}}$ + ${{\mathit M}}_{W}$.
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22
ABAZOV 2007I search for the vector techni-resonances (${{\mathit \rho}_{{T}}}$, ${{\mathit \omega}_{{T}}}$) decaying into ${{\mathit W}}{{\mathit \pi}_{{T}}}$ with ${{\mathit W}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}$ and ${{\mathit \pi}_{{T}}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ or ${{\mathit b}}{{\overline{\mathit c}}}$ . See their Fig. 2 for the exclusion plot in ${{\mathit M}}_{{{\mathit \pi}_{{T}}}}−{{\mathit M}}_{{{\mathit \rho}_{{T}}}}$ plane.
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23
ABULENCIA 2005A search for resonances decaying to electron or muon pairs in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions. at $\sqrt {s }$ = 1.96 TeV. The limit assumes Technicolor-scale mass parameters ${{\mathit M}_{{V}}}$ = ${{\mathit M}_{{A}}}$ = 500 GeV.
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24
CHEKANOV 2002B search for color octet techni-${{\mathit \pi}}{{\mathit P}}$ decaying into dijets in ${{\mathit e}}{{\mathit p}}$ collisions. See their Fig.$~$5 for the limit on $\sigma\mathrm {( {{\mathit e}} {{\mathit p}} \rightarrow {{\mathit e}} {{\mathit P}} {{\mathit X}} )}\cdot{}$B( ${{\mathit P}}$ $\rightarrow$ 2 ${{\mathit j}}$ ).
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25
ABAZOV 2001B searches for vector techni-resonances (${{\mathit \rho}_{{{T}}}},{{\mathit \omega}_{{{T}}}}$) decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$ . The limit assumes $\mathit M_{{{\mathit \rho}_{{{T}}}}}$ = $\mathit M_{{{\mathit \omega}_{{{T}}}}}$ $<\mathit M_{{{\mathit \pi}_{{{T}}}}}+\mathit M_{{{\mathit W}}}$.
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26
The limit is independent of the ${{\mathit \pi}_{{{T}}}}$ mass. See their Fig.$~$9 and Fig.$~$10 for the exclusion plot in the $\mathit M_{{{\mathit \rho}_{{{T}}}}}-\mathit M_{{{\mathit \pi}_{{{T}}}}}$ plane. ABDALLAH 2001 limit on the techni-pion mass is $\mathit M_{{{\mathit \pi}_{{{T}}}}}>79.8$ GeV for $\mathit N_{\mathit D}$=2, assuming its point-like coupling to gauge bosons.
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27
AFFOLDER 2000F search for ${{\mathit \rho}_{{{T}}}}$ decaying into ${{\mathit W}}{{\mathit \pi}_{{{T}}}}$ or ${{\mathit \pi}_{{{T}}}}{{\mathit \pi}_{{{T}}}}$ with ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ and ${{\mathit \pi}_{{{T}}}}$ $\rightarrow$ ${{\overline{\mathit b}}}{{\mathit b}}$ , ${{\overline{\mathit b}}}{{\mathit c}}$ . See Fig.$~$1 in the above Note on ``Dynamical Electroweak Symmetry Breaking'' for the exclusion plot in the $\mathit M_{{{\mathit \rho}_{{{T}}}}}−\mathit M_{{{\mathit \pi}_{{{T}}}}}$ plane.
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28
AFFOLDER 2000K search for the ${{\mathit \rho}_{{{T8}}}}$ decaying into ${{\mathit \pi}_{{LQ}}}{{\mathit \pi}_{{LQ}}}$ with ${{\mathit \pi}_{{LQ}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit \nu}}$ . For ${{\mathit \pi}_{{LQ}}}$ $\rightarrow$ ${{\mathit c}}{{\mathit \nu}}$ , the limit is $\mathit M_{{{\mathit \rho}_{{{T8}}}}}>510~$GeV. See their Fig.$~$2 and Fig.$~$3 for the exclusion plot in the $\mathit M_{{{\mathit \rho}_{{{T8}}}}}−\mathit M_{{{\mathit \pi}_{{LQ}}}}$ plane.
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29
ABE 1999F search for a new particle ${{\mathit X}}$ decaying into ${{\mathit b}}{{\overline{\mathit b}}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$= 1.8 TeV. See Fig.$~$7 in the above Note on ``Dynamical Electroweak Symmetry Breaking'' for the upper limit on $\sigma\mathrm {( {{\mathit p}} {{\overline{\mathit p}}} \rightarrow {{\mathit X}} )}{\times }$B( ${{\mathit X}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ). ABE 1999F also exclude top gluons of width $\Gamma =0.3\mathit M$ in the mass interval $280<\mathit M<670$ GeV, of width $\Gamma =0.5\mathit M$ in the mass interval $340<\mathit M<640$ GeV, and of width $\Gamma =0.7\mathit M$ in the mass interval $375<\mathit M<560$ GeV.
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30
ABE 1999N search for the techni-${{\mathit \omega}}$ decaying into ${{\mathit \gamma}}{{\mathit \pi}_{{{T}}}}$ . The technipion is assumed to decay ${{\mathit \pi}_{{{T}}}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ . See Fig.$~$2 in the above Note on ``Dynamical Electroweak Symmetry Breaking'' for the exclusion plot in the $\mathit M_{{{\mathit \omega}_{{{T}}}}}−\mathit M_{{{\mathit \pi}_{{{T}}}}}$ plane.
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31
ABE 1997G search for a new particle ${{\mathit X}}$ decaying into dijets in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$= 1.8 TeV. See Fig.$~$5 in the above Note on ``Dynamical Electroweak Symmetry Breaking'' for the upper limit on $\sigma\mathrm {( {{\mathit p}} {{\overline{\mathit p}}} \rightarrow {{\mathit X}} )}{\times }$B( ${{\mathit X}}$ $\rightarrow$ 2 ${{\mathit j}}$ ).
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