Limits for ${{\mathit Z}}{}^{′}_{{\mathrm {SM}}}$ INSPIRE search

2023

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}^{\,'}_{SM}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$

$> 4400$

2022

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$\bf{> 5150}$

⁴

2021

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$\text{none 1133 - 2700}$

⁵

2020

ATLS

${{\mathit p}}{{\mathit p}}$, ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$

$\text{ none 1800 - 2900, 3100 - 3300}$

⁶

2020

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$\text{none 250 - 5100}$

⁷

2019

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$\text{none 600 - 2000}$

⁸

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$

$> 2420$

⁹

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$\text{none 200 - 4500}$

¹⁰

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$\text{none 600 - 2700}$

¹¹

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$> 4500$

¹²

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$> 2100$

¹³

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$> 3370$

¹⁴

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$\text{none 600 - 2100, 2300 - 2600}$

¹⁵

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$> 3360$

¹⁶

2016

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$>2900$

¹⁷

2015

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$\text{none 1200 - 1700}$

¹⁸

2015

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$> 2900$

¹⁹

2014

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

• • • We do not use the following data for averages, fits, limits, etc. • • •

²⁰

BOBOVNIKOV

RVUE

${{\mathit p}}{{\mathit p}}$, ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$

$>1900$

²¹

2016

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$>2020$

²²

2015

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$> 1400$

²³

2013

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$> 1470$

²⁴

2013

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$> 2590$

²⁵

2013

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$> 2220$

²⁶

2012

ATLS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$>1400$

²⁷

2012

CMS

${{\mathit p}}{{\mathit p}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$> 1071$

²⁸

2011

CDF

${{\mathit p}}{{\overline{\mathit p}}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$> 1023$

²⁹

2011

${{\mathit p}}{{\overline{\mathit p}}}$, ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$

$\text{none 247 - 544}$

³⁰

2010

CDF

${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$

$\text{none 320 - 740}$

³¹

CDF

${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$> 963$

²⁹

CDF

${{\mathit p}}{{\overline{\mathit p}}}$, ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$

$> 1403$

³²

RVUE

Electroweak

$> 1305$

³³

ABDALLAH

2006

DLPH

${{\mathit e}^{+}}{{\mathit e}^{-}}$

$> 399$

³⁴

ACOSTA

2005

CDF

${{\overline{\mathit p}}}{{\mathit p}}$: ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$

$\text{none 400 - 640}$

2004

${{\mathit p}}{{\overline{\mathit p}}}$: ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$>1018$

³⁵

ABBIENDI

2004

OPAL

${{\mathit e}^{+}}{{\mathit e}^{-}}$

$>670$

³⁶

2001

${{\mathit p}}{{\overline{\mathit p}}}$, ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$

$>1500$

³⁷

CHEUNG

2001

RVUE

Electroweak

$>710$

³⁸

ABREU

2000

DLPH

${{\mathit e}^{+}}{{\mathit e}^{-}}$

$>898$

³⁹

BARATE

2000

ALEP

${{\mathit e}^{+}}{{\mathit e}^{-}}$

$>809$

⁴⁰

1999

RVUE

Electroweak

$>690$

⁴¹

1997

CDF

${{\mathit p}}{{\overline{\mathit p}}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$>398$

⁴²

VILAIN

1994

CHM2

${{\mathit \nu}_{{{\mu}}}}$ ${{\mathit e}}$ $\rightarrow$ ${{\mathit \nu}_{{{\mu}}}}{{\mathit e}}$ and ${{\overline{\mathit \nu}}_{{{\mu}}}}$ ${{\mathit e}}$ $\rightarrow$ ${{\overline{\mathit \nu}}_{{{\mu}}}}{{\mathit e}}$

$>237$

⁴³

ALITTI

UA2

${{\mathit p}}{{\overline{\mathit p}}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$\text{none 260 - 600}$

⁴⁴

RIZZO

RVUE

${{\mathit p}}{{\overline{\mathit p}}}$; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$

$>426$

⁴⁵

1990

VNS

${{\mathit e}^{+}}{{\mathit e}^{-}}$

¹ HAYRAPETYAN 2025M search for resonances decaying to ${{\mathit \tau}^{+}}$ ${{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 4 for limits on $\sigma \cdot{}B$.

² TUMASYAN 2023AF search for resonance decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 4 for limits on $\sigma \cdot{}B$.

³ TUMASYAN 2022AE set limits on ${{\mathit Z}^{\,'}}$ from the measurements of the forward-backward asymmetry in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ and ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ events in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit is for the sequential SM ${{\mathit Z}^{\,'}}$. See their Fig. 6 for limits in mass-coupling plane.

⁴ SIRUNYAN 2021N search for resonance decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

⁵ AAD 2020T search for resonances decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig. 7(b) for limits on the product of the cross section, acceptance, ${{\mathit b}}$-tagging efficiency, and branching fraction.

⁶ SIRUNYAN 2020AI search for resonances decaying into dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

⁷ AAD 2019L search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

⁸ AABOUD 2018AB search for resonances decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

⁹ AABOUD 2018G search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

¹⁰ SIRUNYAN 2018BB search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. See their Fig.5 for limits on the ${{\mathit Z}^{\,'}}$ coupling strengths with light quarks.

¹¹ SIRUNYAN 2018BO search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

¹² AABOUD 2017AT search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

¹³ KHACHATRYAN 2017H search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

¹⁴ KHACHATRYAN 2017T search for resonances decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8, 13 TeV.

¹⁵ KHACHATRYAN 2017W search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

¹⁶ AABOUD 2016U search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

¹⁷ KHACHATRYAN 2015AE search for resonances decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.

¹⁸ KHACHATRYAN 2015V search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.

¹⁹ AAD 2014V search for resonances decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.

²⁰ BOBOVNIKOV 2018 use the ATLAS limits on $\sigma $( ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}})\cdot{}$B( ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$) to constrain the ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing parameter $\xi $. See their Fig. 11 for limits in $\mathit M_{{{\mathit Z}^{\,'}}}−\xi $ plane.

²¹ AABOUD 2016AA search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.

²² AAD 2015AM search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.

²³ AAD 2013S search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV.

²⁴ CHATRCHYAN 2013A use ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV.

²⁵ CHATRCHYAN 2013AF search for resonances decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV and 8 TeV.

²⁶ AAD 2012CC search for resonances decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV.

²⁷ CHATRCHYAN 2012O search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV.

²⁸ AALTONEN 2011I search for resonances decaying to ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV.

²⁹ ABAZOV 2011A, AALTONEN 2009T, AALTONEN 2007H, and ABULENCIA 2006L search for resonances decaying to ${{\mathit e}^{+}}{{\mathit e}^{-}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96$~$TeV.

³⁰ The quoted limit assumes $\mathit g_{{{\mathit W}} {{\mathit W}} {{\mathit Z}^{\,'}}}/\mathit g_{{{\mathit W}} {{\mathit W}} {{\mathit Z}}}$ = ($\mathit M_{{{\mathit W}}}/\mathit M_{{{\mathit Z}^{\,'}}}){}^{2}$. See their Fig.$~$4 for limits in mass-coupling plane.

³¹ AALTONEN 2009AC search for new particle decaying to dijets.

³² ERLER 2009 give 95$\%$ CL limit on the ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing $-0.0026<\theta <$ 0.0006.

³³ ABDALLAH 2006C use data $\sqrt {s }$ = $130 - 207$ GeV.

³⁴ ACOSTA 2005R search for resonances decaying to tau lepton pairs in ${{\overline{\mathit p}}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 1.96 TeV.

³⁵ ABBIENDI 2004G give 95$\%$ CL limit on ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing $−$0.00422 $<\theta <$0.00091. $\sqrt {s }$ = 91 to 207$~$GeV.

³⁶ ABAZOV 2001B search for resonances in ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ at $\sqrt {\mathit s }$=1.8 TeV. They find $\sigma \cdot{}$B( ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit e}}{{\mathit e}})<0.06~$pb for $\mathit M_{{{\mathit Z}^{\,'}}}>500$ GeV.

³⁷ CHEUNG 2001B limit is derived from bounds on contact interactions in a global electroweak analysis.

³⁸ ABREU 2000S uses LEP data at $\sqrt {\mathit s }$=90 to 189 GeV.

³⁹ BARATE 2000I search for deviations in cross section and asymmetries in ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ fermions at $\sqrt {\mathit s }$=90 to 183 GeV. Assume $\theta $=0. Bounds in the mass-mixing plane are shown in their Figure$~$18.

⁴⁰ ERLER 1999 give 90$\%$CL limit on the ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing $-0.0041<\theta <0.0003$. $\rho _{0}$=1 is assumed.

⁴¹ ABE 1997S find $\sigma\mathrm {({{\mathit Z}^{\,'}})}{\times }B({{\mathit e}^{+}}{{\mathit e}^{-}},{{\mathit \mu}^{+}}{{\mathit \mu}^{-}})<40~$fb for ${\mathit m}_{{{\mathit Z}^{\,'}}}>600$ GeV at $\sqrt {\mathit s }$= 1.8 TeV.

⁴² VILAIN 1994B assume ${\mathit m}_{{{\mathit t}}}$ = 150 GeV.

⁴³ ALITTI 1993 search for resonances in the two-jet invariant mass. The limit assumes B( ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}})=0.7$. See their Fig.$~$5 for limits in the ${\mathit m}_{{{\mathit Z}^{\,'}}}−B({{\mathit q}}{{\overline{\mathit q}}}$) plane.

⁴⁴ RIZZO 1993 analyses CDF limit on possible two-jet resonances.

⁴⁵ ABE 1990F use data for $\mathit R$, $\mathit R_{{{\mathit \ell}} {{\mathit \ell}}}$, and $\mathit A_{{{\mathit \ell}} {{\mathit \ell}}}$. They fix ${\mathit m}_{{{\mathit W}}}$ = $80.49$ $\pm0.43$ $\pm0.24$ GeV and ${\mathit m}_{{{\mathit Z}}}$ = $91.13$ $\pm0.03$ GeV.

References:

HAYRAPETYAN

2025M

PR D111 112004

Search for heavy neutral resonances decaying to tau lepton pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV

2023AF

PR D108 012009

Search for narrow resonances in the

b

-tagged dijet mass spectrum in proton-proton collisions at

\sqrt{s} = 13 ? ? TeV

2022AE

JHEP 2208 063

Measurement of the Drell-Yan forward-backward asymmetry at high dilepton masses in proton-proton collisions at $\sqrt{s} = 13$ TeV

2021N

JHEP 2107 208

Search for resonant and nonresonant new phenomena in high-mass dilepton final states at $ \sqrt{s} $ = 13 TeV

2020T

JHEP 2003 145

Search for new resonances in mass distributions of jet pairs using 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

2020AI

JHEP 2005 033

Search for high mass dijet resonances with a new background prediction method in proton-proton collisions at $\sqrt{s} =$ 13 TeV

2019L

PL B796 68

Search for high-mass dilepton resonances using 139 fb$^{-1}$ of $pp$ collision data collected at $\sqrt{s}=$13 TeV with the ATLAS detector

2018AB

PR D98 032016

Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

2018G

JHEP 1801 055

Search for Additional Heavy Neutral Higgs and Gauge Bosons in the ditau Final State Produced in 36 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector

BOBOVNIKOV

PR D98 095029

Improved constraints on the mixing and mass of $Z'$ bosons from resonant diboson searches at the LHC at $\sqrt{s}=13$ TeV and predictions for Run II

2018BB

JHEP 1806 120

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

2018BO

JHEP 1808 130

Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles

2017AT

JHEP 1710 182

Search for New High-Mass Phenomena in the Dilepton Final State using 36 ${\mathrm {fb}}{}^{-1}$ of Proton-Proton Collision Data at $\sqrt {s }$ = 13 TeV with the ATLAS Detector

2017T

PL B768 57

Search for Narrow Resonances in Dilepton Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV and Combination with 8 TeV Data

2017W

PL B769 520

Search for Dijet Resonances in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV and Constraints on Dark Matter and other Models

2017H

JHEP 1702 048

Search for Heavy Resonances Decaying to Tau Lepton Pairs in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV

2016U

PL B761 372

Search for High-Mass New Phenomena in the Dilepton Final State using Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector

2016AA

EPJ C76 585

Search for Minimal Supersymmetric Standard Model Higgs Bosons $\mathit H/\mathit A$ and for a ${{\mathit Z}^{\,'}}$ Boson in the ${{\mathit \tau}}{{\mathit \tau}}$ Final State Produced in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector

2015AM

JHEP 1507 157

A Search for High-Mass Resonances Decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector

2015V

PR D91 052009

Search for Resonances and Quantum Black Holes using Dijet Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV

2015AE

JHEP 1504 025

Search for Physics Beyond the Standard Model in Dilepton Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV

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

2013S

PL B719 242

A Search for High-Mass Resonances Decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector

2013A

JHEP 1301 013

Search for Narrow Resonances and Quantum Black Holes in Inclusive and ${\mathit {\mathit b}}$-Tagged Dijet Mass Spectra from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV

2013AF

PL B720 63

Search for Heavy Narrow Dilepton Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV and $\sqrt {s }$ = 8 TeV

2012CC

JHEP 1211 138

Search for High-Mass Resonances Decaying to Dilepton Final States in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector

2012O

PL B716 82

Search for High Mass Resonances Decaying into ${{\mathit \tau}}$-Lepton Pairs in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV

2011I

PRL 106 121801

Search for High Mass Resonances Decaying to Muon Pairs in $\sqrt {s }$ = 1.96 TeV ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions

2011A

PL B695 88

Search for a Heavy Neutral Gauge Boson in the Dielectron Channel with 5.4 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 1.96$~$TeV

2010N

PRL 104 241801

Search for ${{\mathit W}}{{\mathit W}}$ and ${{\mathit W}}{{\mathit Z}}$ Resonances Decaying to Electron, Missing $\mathit E_{T}$, and Two Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 1.96 TeV

2009T

PRL 102 031801

Search for High-Mass ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Resonances in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96$~$TeV

2009AC

PR D79 112002

Search for New Particles Decaying into Dijets in Proton-Antiproton Collisions at $\sqrt {s }$ = 1.96$~$TeV

JHEP 0908 017

Improved Constraints on ${{\mathit Z}^{\,'}}$ Bosons from Electroweak Precision Data

ABDALLAH

2006C

EPJ C45 589

Measurement and Interpretation of Fermion-Pair Production at LEP Energies above the ${{\mathit Z}}$ Resonance

ACOSTA

2005R

PRL 95 131801

Search for New Physics Using High-Mass Tau Pairs from 1.96 TeV ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions

2004C

PR D69 111101

Search for New Particles in the Two Jet Decay Channel with the ${D0}$ Detector

ABBIENDI

2004G

EPJ C33 173

Tests of the Standard Model and Constraints on New Physics from Measurements of Fermion Pair Production at 189 to 209 GeV at LEP

2001B

PRL 87 061802

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

CHEUNG

2001B

PL B517 167

Constraints on Electron Quark Contact Interactions and Implications to Models of Leptoquarks and Extra ${{\mathit Z}}$ Bosons

ABREU

2000S

PL B485 45

Measurement and Interpretation of Fermion-Pair Production at LEP Energies of 183 and 189 GeV

BARATE

2000I

EPJ C12 183

Study of Fermion Pair Production in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collisions at $130 - 183$ GeV

1999

PL B456 68

Constraints on Extended Neutral Gauge Structures

1997S

PRL 79 2192

Search for New Gauge Bosons Decaying into Dileptons in ${{\overline{\mathit p}}}$ ${{\mathit p}}$ Collisions at $\sqrt {s }$ = 1.8 TeV

VILAIN

1994B

PL B332 465

Constraints on Additional ${{\mathit Z}}$ Bosons Derived from Neutrino Electron Scattering Measurements

ALITTI

NP B400 3

A Search for New Intermediate Vector Bosons and Exited Quarks Decaying to Two Jets at CERN ${{\mathit p}}$ ${{\overline{\mathit p}}}$ Collider

RIZZO

PR D48 4470

Constraints on New Physics from Fermilab Tevatron Dijet Data