pdgLive

ATLS

${{\mathit h}}$ $\rightarrow$ ${{\mathit \pi}_{{v}}}{{\mathit \pi}_{{v}}}$

⁷

AAIJ

LHCB

${{\mathit h}}$ $\rightarrow$ ${{\mathit \pi}_{{v}}}{{\mathit \pi}_{{v}}}$

$> 1140$

⁸

CMS

${{\mathit \rho}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$

⁹

CMS

${{\mathit H}}$ $\rightarrow$ ${{\mathit \pi}_{{v}}}{{\mathit \pi}_{{v}}}$

$\text{none 200 - 700, 750 - 890}$

¹⁰

2014

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \omega}_{{T}}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \gamma}}$

$\text{none 275 - 960}$

¹⁰

2014

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit a}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \gamma}}$

¹¹

2014

ATLS

color singlet techni-vector

$> 703$

¹²

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit a}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \gamma}}$

$> 494$

¹³

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \omega}_{{T}}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \gamma}}$

$\text{none 500 - 1740}$

¹⁴

ATLS

top-color ${{\mathit Z}^{\,'}}$

$> 1300$

¹⁵

CMS

top-color ${{\mathit Z}^{\,'}}$

$> 2100$

¹⁴

CMS

top-color ${{\mathit Z}^{\,'}}$

¹⁶

BAAK

2012

RVUE

QCD-like technicolor

$\text{none 167 - 687}$

¹⁷

2012

CMS

${{\mathit \rho}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$

$> 805$

¹⁴

CDF

top-color ${{\mathit Z}^{\,'}}$

$> 805$

¹⁴

CDF

top-color ${{\mathit Z}^{\,'}}$

¹⁸

RVUE

top-Higgs

¹⁹

RVUE

techini-${{\mathit \pi}}$

²⁰

2010

CDF

${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit \rho}_{{T}}}$ $/$ ${{\mathit \omega}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \pi}_{{T}}}$

$\text{none 208 - 408}$

²¹

2010

${{\mathit \rho}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit Z}}$

²²

2007

${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit \rho}_{{T}}}$ $/$ ${{\mathit \omega}_{{T}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \pi}_{{T}}}$

$> 280$

²³

ABULENCIA

2005

CDF

${{\mathit \rho}_{{{T}}}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

²⁴

CHEKANOV

2002

ZEUS

color octet techni-${{\mathit \pi}}$

$>207$

²⁵

2001

${{\mathit \rho}_{{{T}}}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$

$\text{none 90 - 206.7}$

²⁶

ABDALLAH

2001

DLPH

${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \rho}_{{{T}}}}$

²⁷

2000

CDF

color-singlet techni-${{\mathit \rho}}$, ${{\mathit \rho}_{{{T}}}}$ $\rightarrow$ ${{\mathit W}}{{\mathit \pi}_{{{T}}}}$ , 2${{\mathit \pi}_{{{T}}}}$

$>600$

²⁸

2000

CDF

color-octet techni-${{\mathit \rho}}$, ${{\mathit \rho}_{{{T8}}}}$ $\rightarrow$ 2 ${{\mathit \pi}_{{LQ}}}$

$\text{none 350 - 440}$

²⁹

1999

CDF

color-octet techni-${{\mathit \rho}}$, ${{\mathit \rho}_{{{T8}}}}$ $\rightarrow$ ${{\overline{\mathit b}}}{{\mathit b}}$

³⁰

1999

CDF

techni-${{\mathit \omega}}$, ${{\mathit \omega}_{{{T}}}}$ $\rightarrow$ ${{\mathit \gamma}}{{\overline{\mathit b}}}{{\mathit b}}$

$\text{none 260 - 480}$

³¹

1997

CDF

color-octet techni-${{\mathit \rho}}$, ${{\mathit \rho}_{{{T8}}}}$ $\rightarrow$ 2jets

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 $\sigma \cdot{}\mathit B$.

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.

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 ${{\mathit \sigma}}\mathit B$.

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.

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.

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 $\sigma \mathit B$.

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 $\sigma \mathit B$.

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.

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 $\sigma \mathit B$.

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 ${{\mathit Z}}$( $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ ).

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.

¹² AAD 2013AN search for vector techni-resonance ${{\mathit a}_{{T}}}$ decaying into ${{\mathit W}}{{\mathit \gamma}}$ .

¹³ AAD 2013AN search for vector techni-resonance ${{\mathit \omega}_{{T}}}$ decaying into ${{\mathit Z}}{{\mathit \gamma}}$ .

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.

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.

¹⁶ BAAK 2012 give electroweak oblique parameter constraints on the QCD-like technicolor models. See their Fig. 28.

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.

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.

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.

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.

²¹ ABAZOV 2010A search for a vector techni-resonance decaying into ${{\mathit W}}{{\mathit Z}}$ . The limit assumes ${{\mathit M}}_{{{\mathit \rho}_{{T}}}}<$ ${{\mathit M}}_{{{\mathit \pi}_{{T}}}}$ + ${{\mathit M}}_{W}$.

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.

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.

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 ${{\mathit j}}$ ).

²⁵ ABAZOV 2001B searches for vector techni-resonances (${{\mathit \rho}_{{{T}}}},{{\mathit \omega}_{{{T}}}}$) decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$ . The limit assumes $\mathit M_{{{\mathit \rho}_{{{T}}}}}$ = $\mathit M_{{{\mathit \omega}_{{{T}}}}}$ $<\mathit M_{{{\mathit \pi}_{{{T}}}}}+\mathit M_{{{\mathit W}}}$.

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.

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.

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.

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.

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.

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 ${{\mathit j}}$ ).

References:

2016W

PL B758 249

Search for Single Production of a Vector-Like Quark via a Heavy Gluon in the 4${\mathit {\mathit b}}$ Final State with the ATLAS Detector in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV

2016E

PR D93 012001

Search for Resonant ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV

2015AB

PR D92 012010

Search for Long-Lived, Weakly Interacting Particles that Decay to Displaced Hadronic Jets in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector

2015Q

PL B743 15

Search for Pair-Produced Long-Lived Neutral Particles Decaying in the ATLAS Hadronic Calorimeter in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV

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

2015AO

JHEP 1508 148

A Search for ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Resonances using Lepton-plus-Jets Events in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector

AAIJ

2015AN

EPJ C75 152

Search for Long-Lived Particles Decaying to Jet Pairs

2015W

PR D91 052012

Search for Long-Lived Particles that Decay into Final States Containing Two Electrons or Two Muons in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV

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

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

2014V

PR D90 052005

Search for High-Mass Dilepton Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector

2013AN

PR D87 112003

Measurements of ${{\mathit W}}{{\mathit \gamma}}$ and ${{\mathit Z}}{{\mathit \gamma}}$ Production in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector at the LHC

2013AQ

PR D88 012004

A Search for ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Resonances in the Lepton Plus Jets Final State with ATLAS using 4.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV

2013BM

PRL 111 211804

Searches for New Physics using the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Invariant Mass Distribution in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV

2013AP

PR D87 072002

Search for ${{\mathit Z}^{\,'}}$ Resonances Decaying to ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ in dilepton+jets Final States in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV

BAAK

2012

EPJ C72 2003

Updated Status of the Global Electroweak Fit and Constraints on New Physics

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

2011AD

PR D84 072003

Search for Resonant Production of ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Decaying to Jets in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV

2011AE

PR D84 072004

Search for Resonant Production of ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ pairs in 4.8 fb${}^{-1}$ of Integrated Luminosity of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV

2011A

PR D84 115025

Technipion Limits from LHC Higgs Searches

PR D84 095022

LHC Limits on the top-Higgs in Models with Strong Top-Quark Dynamics

2010I

PRL 104 111802

Search for Technicolor Particles Produced in Association with a ${{\mathit W}}$ Boson at CDF

2010A

PRL 104 061801

Search for a Resonance Decaying into ${{\mathit W}}{{\mathit Z}}$ Boson Pairs in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions

2007I

PRL 98 221801

Search for Techniparticles in ${{\mathit e}}$+jets Events at ${D0}$

ABULENCIA

2005A

PRL 95 252001

Search for New High-Mass Particles Decaying to Lepton Pairs in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ =1.96 TeV

CHEKANOV

2002B

PL B531 9

High Mass Dijet Cross Sections in Photoproduction at HERA

2001B

PRL 87 061802

Search for Heavy Particles Decaying into Electron-Positron Pairs in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions

ABDALLAH

2001

EPJ C22 17

Search for Technicolor with DELPHI

2000K

PRL 85 2056

Search for Second and Third Generation Leptoquarks Including Production via Technicolor Interactions in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV

2000F

PRL 84 1110

Search for Technicolor Particles in Lepton Plus Two Jets and Multijet Channels in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV

1999F

PRL 82 2038

Search for New Particles Decaying to ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.8 TeV

1999N

PRL 83 3124

Search for a Technicolor ${{\mathit \omega}_{{T}}}$ Particle in Events with a Photon and a ${\mathit {\mathit b}}$-Quark jet at CDF