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

INSPIRE   PDGID:
S056Z1C
${{\mathit Z}}{}^{′}_{{\mathrm {SM}}}$ is assumed to have couplings with quarks and leptons which are identical to those of ${{\mathit Z}}$, and decays only to known fermions. The most recent preliminary results can be found in the “${{\mathit Z}^{\,'}}$-boson searches” review above.
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$\bf{ > 5150}$ OUR LIMIT
$> 4400$ 95 1
TUMASYAN
2022AE
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$\bf{> 5150}$ 95 2
SIRUNYAN
2021N
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$\text{none 1133 - 2700}$ 95 3
AAD
2020T
 ATLS ${{\mathit p}}{{\mathit p}}$ , ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
$\text{ none 1800 - 2900, 3100 - 3300}$ 95 4
SIRUNYAN
2020AI
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 250 - 5100}$ 95 5
AAD
2019L
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$\text{none 600 - 2000}$ 95 6
AABOUD
2018AB
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
$> 2420$ 95 7
AABOUD
2018G
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$\text{none 200 - 4500}$ 95 8
SIRUNYAN
2018BB
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$\text{none 600 - 2700}$ 95 9
SIRUNYAN
2018BO
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 4500$ 95 10
AABOUD
2017AT
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$> 2100$ 95 11
KHACHATRYA..
2017H
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$> 3370$ 95 12
KHACHATRYA..
2017T
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$\text{none 600 - 2100, 2300 - 2600}$ 95 13
KHACHATRYA..
2017W
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 3360$ 95 14
AABOUD
2016U
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$>2900$ 95 15
KHACHATRYA..
2015AE
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$\text{none 1200 - 1700}$ 95 16
KHACHATRYA..
2015V
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 2900$ 95 17
AAD
2014V
 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. • •
18
BOBOVNIKOV
2018
RVUE ${{\mathit p}}{{\mathit p}}$ , ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit W}^{+}}{{\mathit W}^{-}}$
$>1900$ 95 19
AABOUD
2016AA
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$>2020$ 95 20
AAD
2015AM
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$> 1400$ 95 21
AAD
2013S
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$> 1470$ 95 22
CHATRCHYAN
2013A
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 2590$ 95 23
CHATRCHYAN
2013AF
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$> 2220$ 95 24
AAD
2012CC
 ATLS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$>1400$ 95 25
CHATRCHYAN
2012O
 CMS ${{\mathit p}}{{\mathit p}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$> 1071$ 95 26
AALTONEN
2011I
 CDF ${{\mathit p}}{{\overline{\mathit p}}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$> 1023$ 95 27
ABAZOV
2011A
 D0 ${{\mathit p}}{{\overline{\mathit p}}}$ , ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$\text{none 247 - 544}$ 95 28
AALTONEN
2010N
 CDF ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$
$\text{none 320 - 740}$ 95 29
AALTONEN
2009AC
 CDF ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$> 963$ 95 27
AALTONEN
2009T
 CDF ${{\mathit p}}{{\overline{\mathit p}}}$ , ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$> 1403$ 95 30
ERLER
2009
RVUE Electroweak
$> 1305$ 95 31
ABDALLAH
2006C
 DLPH ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$> 399$ 95 32
ACOSTA
2005R
 CDF ${{\overline{\mathit p}}}{{\mathit p}}$ : ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$
$\text{none 400 - 640}$ 95
ABAZOV
2004C
 D0 ${{\mathit p}}{{\overline{\mathit p}}}$ : ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$>1018$ 95 33
ABBIENDI
2004G
 OPAL ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$>670$ 95 34
ABAZOV
2001B
 D0 ${{\mathit p}}{{\overline{\mathit p}}}$ , ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$>1500$ 95 35
CHEUNG
2001B
 RVUE Electroweak
$>710$ 95 36
ABREU
2000S
 DLPH ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$>898$ 95 37
BARATE
2000I
 ALEP ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$>809$ 95 38
ERLER
1999
RVUE Electroweak
$>690$ 95 39
ABE
1997S
 CDF ${{\mathit p}}{{\overline{\mathit p}}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ , ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$>398$ 95 40
VILAIN
1994B
 CHM2 ${{\mathit \nu}_{{{\mu}}}}$ ${{\mathit e}}$ $\rightarrow$ ${{\mathit \nu}_{{{\mu}}}}{{\mathit e}}$ and ${{\overline{\mathit \nu}}_{{{\mu}}}}$ ${{\mathit e}}$ $\rightarrow$ ${{\overline{\mathit \nu}}_{{{\mu}}}}{{\mathit e}}$
$>237$ 90 41
ALITTI
1993
UA2 ${{\mathit p}}{{\overline{\mathit p}}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$\text{none 260 - 600}$ 95 42
RIZZO
1993
RVUE ${{\mathit p}}{{\overline{\mathit p}}}$ ; ${{\mathit Z}_{{{SM}}}^{\,'}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$
$>426$ 90 43
ABE
1990F
 VNS ${{\mathit e}^{+}}{{\mathit e}^{-}}$
1  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.
2  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.
3  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.
4  SIRUNYAN 2020AI search for resonances decaying into dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
5  AAD 2019L search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
6  AABOUD 2018AB search for resonances decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
7  AABOUD 2018G search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
8  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.
9  SIRUNYAN 2018BO search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
10  AABOUD 2017AT search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
11  KHACHATRYAN 2017H search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
12  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.
13  KHACHATRYAN 2017W search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
14  AABOUD 2016U search for resonances decaying to ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
15  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.
16  KHACHATRYAN 2015V search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.
17  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.
18  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.
19  AABOUD 2016AA search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
20  AAD 2015AM search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV.
21  AAD 2013S search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV.
22  CHATRCHYAN 2013A use ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$=7 TeV.
23  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.
24  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.
25  CHATRCHYAN 2012O search for resonances decaying to ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV.
26  AALTONEN 2011I search for resonances decaying to ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV.
27  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.
28  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.$~$4 for limits in mass-coupling plane.
29  AALTONEN 2009AC search for new particle decaying to dijets.
30  ERLER 2009 give 95$\%$ CL limit on the ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing $-0.0026<\theta <$ 0.0006.
31  ABDALLAH 2006C use data $\sqrt {s }$ = $130 - 207$ GeV.
32  ACOSTA 2005R search for resonances decaying to tau lepton pairs in ${{\overline{\mathit p}}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 1.96 TeV.
33  ABBIENDI 2004G give 95$\%$ CL limit on ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing $−$0.00422 $<\theta <$0.00091. $\sqrt {s }$ = 91 to 207$~$GeV.
34  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.
35  CHEUNG 2001B limit is derived from bounds on contact interactions in a global electroweak analysis.
36  ABREU 2000S uses LEP data at $\sqrt {\mathit s }$=90 to 189 GeV.
37  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 $=0. Bounds in the mass-mixing plane are shown in their Figure$~$18.
38  ERLER 1999 give 90$\%$CL limit on the ${{\mathit Z}}-{{\mathit Z}^{\,'}}$ mixing $-0.0041<\theta <0.0003$. $\rho _{0}$=1 is assumed.
39  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.
40  VILAIN 1994B assume ${\mathit m}_{{{\mathit t}}}$ = 150 GeV.
41  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.
42  RIZZO 1993 analyses CDF limit on possible two-jet resonances.
43  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:
TUMASYAN 2022AE
JHEP 2208 063
SIRUNYAN 2021N
JHEP 2107 208 Search for resonant and nonresonant new phenomena in high-mass dilepton final states at $ \sqrt{s} $ = 13 TeV
AAD 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
SIRUNYAN 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
AAD 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
AABOUD 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
AABOUD 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
BOBOVNIKOV 2018
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
SIRUNYAN 2018BB
JHEP 1806 120 Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
SIRUNYAN 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
AABOUD 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
KHACHATRYAN 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
KHACHATRYAN 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
KHACHATRYAN 2017H
JHEP 1702 048 Search for Heavy Resonances Decaying to Tau Lepton Pairs in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
AABOUD 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
AABOUD 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
AAD 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
KHACHATRYAN 2015V
PR D91 052009 Search for Resonances and Quantum Black Holes using Dijet Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2015AE
JHEP 1504 025 Search for Physics Beyond the Standard Model in Dilepton Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
AAD 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
AAD 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
CHATRCHYAN 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
CHATRCHYAN 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
AAD 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
CHATRCHYAN 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
AALTONEN 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
ABAZOV 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
AALTONEN 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
AALTONEN 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
AALTONEN 2009AC
PR D79 112002 Search for New Particles Decaying into Dijets in Proton-Antiproton Collisions at $\sqrt {s }$ = 1.96$~$TeV
ERLER 2009
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
ABAZOV 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
ABAZOV 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
ERLER 1999
PL B456 68 Constraints on Extended Neutral Gauge Structures
ABE 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 1993
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 1993
PR D48 4470 Constraints on New Physics from Fermilab Tevatron Dijet Data
ABE 1990F
PL B246 297 Experimental Limits on Extra ${{\mathit Z}}$ Bosons from ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Annihilation Data with the VENUS Detector at $\sqrt {s }$ = 50-64 GeV