pdgLive

${{\mathit c}_{{{WWW}}}}/\Lambda {}^{2}$, ${{\mathit c}_{{{W}}}}/\Lambda {}^{2}$, ${{\mathit c}_{{{B}}}}/\Lambda {}^{2}$

These couplings are used in EFT-based approaches to anomalous couplings. They are linearly related to the couplings discussed above.

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DOCUMENT ID

TECN

COMMENT

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

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 13 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 7+8 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 8 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 8 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 8 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 8 TeV

ATLS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 8 TeV

CMS

${\it{}E}^{\it{}pp}_{\rm{}cm}$ = 8 TeV

¹

TUMASYAN 2022AB study ${{\mathit W}}{{\mathit Z}}$ production, measuring cross sections and various distributions. Analysing the ${{\mathit W}}{{\mathit Z}}$ invariant mass distribution, the following 95$\%$ C.L. limits are derived in units of TeV${}^{-2}$: $-2.5$ $<$ c$_{W}/\Lambda {}^{2}$ $<$ 0.3, $-1.0$ $<$ c$_{WWW}/\Lambda {}^{2}$ $<$ 1.2, $-43$ $<$ c$_{b}/\Lambda {}^{2}$ $<$ 113, $-0.62$ $<$ ${{\widetilde{\mathit c}}}_{WWW}/\Lambda {}^{2}$ $<$ 0.53, $-32$ $<$ ${{\widetilde{\mathit c}}}_{W}/\Lambda {}^{2}$ $<$ 32.

²

TUMASYAN 2022E measure ${{\mathit W}}{{\mathit \gamma}}$ production where the ${{\mathit W}}$ boson decays to electrons or muons. Analysing the photon transverse momentum distribution in bins of lepton azimuth, the following 95$\%$ C.L. limit is derived in units of TeV${}^{-2}$: $-0.062$ $<$ c$_{3W}/\Lambda {}^{2}$ $<$ 0.052. This limit is derived including the non-SM, SM and their interference effects.

³

AAD 2021AC study the differential cross-section for the electroweak production of dijets in association with a ${{\mathit Z}}$ boson, where the ${{\mathit Z}}$ boson decays to electrons or muons. The number of events selected in the data is 10,870 (12,125) in the electron (muon) channel. Analyzing the distribution of the azimuthal separation of the two jets, the following 95$\%$ C.L. limits are derived in units of TeV${}^{-2}$: $-2.7$ $<$ c$_{ {{\mathit W}} {{\mathit W}} {{\mathit W}} }/\Lambda {}^{2}$ $<$ 5.8, $-1.6$ $<$ ${{\widetilde{\mathit c}}}_{ {{\mathit W}} {{\mathit W}} {{\mathit W}} }/\Lambda {}^{2}$ $<$ 2.0, $-0.19$ $<$ c$_{W}/\Lambda {}^{2}$ $<$ 0.41, $-0.11$ $<$ ${{\widetilde{\mathit c}}}_{W}/\Lambda {}^{2}$ $<$ 0.14, $-6.31$ $<$ c$_{ {{\mathit H}} {{\mathit W}} {{\mathit B}} }/\Lambda {}^{2}$ $<$ 1.01, 0.23 $<$ ${{\widetilde{\mathit c}}}_{ {{\mathit H}} {{\mathit W}} {{\mathit B}} }/\Lambda {}^{2}$ $<$ 2.35.

⁴

AAD 2021W analyze ${{\mathit W}^{+}}{{\mathit W}^{-}}$ production in association with at least one jet. Events with exactly one oppositely-charged electron-muon pair and at least one hadronic jet of transverse momentum larger than 30 GeV (120 GeV) are selected. In the data, 89,239 (5,825) events are found, with a total Standard-Model expectation of $91600$ $\pm2500$ ($5980$ $\pm150$). Analyzing the electron-muon invariant mass distribution, the following limit at 95$\%$ C.L. is obtained: $-0.33$ $<$ c$_{W}/\Lambda {}^{2}$ $<$ 0.33 ($-0.60$ $<$ c$_{W}/\Lambda {}^{2}$ $<$ 0.58), for a fixed choice of $\Lambda $ = 1 TeV.

⁵

SIRUNYAN 2021G measure ${{\mathit W}}{{\mathit \gamma}}$ production where the ${{\mathit W}}$ decays into electrons or muons. In the data, 385,224 (395,818) events are selected in the electron (muon) channel, with a total Standard-Model expectation of $396913$ $\pm54686$ ($396257$ $\pm22837$) events. Analysing the photon transverse momentum distribution, the following 95$\%$ C.L. limits are derived in units of TeV${}^{-2}$: $-0.90$ $<$ c$_{ {{\mathit W}} {{\mathit W}} {{\mathit W}} }/\Lambda {}^{2}$ $<$ 0.91, $-40$ $<$ c$_{B}/\Lambda {}^{2}$ $<$ 41, $-0.45$ $<$ c$_{ {{\overline{\mathit W}}} {{\mathit W}} {{\mathit W}} }/\Lambda {}^{2}$ $<$ 0.45, $-20$ $<$ c$_{{{\overline{\mathit W}}}}/\Lambda {}^{2}$ $<$ 20.

⁶

SIRUNYAN 2020BA study electroweak production of a ${{\mathit W}}$ boson in association with two jets, using ${{\mathit W}}$ decays in the electron or muon channel. The isolated muons (electrons) are required to have a transverse momentum larger than 25 (30) GeV, while the transverse momentum of the two jets has to be larger than 50 and 30 GeV. A total of 2.382 (1.051) million events are selected in the muon (electron) channel, with a Standard Model expectation of $2.39$ $\pm0.17$ ($1.054$ $\pm0.058$) million events. Analysing the transverse momentum distribution of the charged leptons from ${{\mathit W}}$ decay, the following 95$\%$ C.L. limits are obtained in units of TeV${}^{-2}$: $-2.3$ $<$ ${{\mathit c}_{{WWW}}}/{{\mathit \Lambda}}{}^{2}$ $<$ $2.5$, $-8.8$ $<$ ${{\mathit c}_{{W}}}/{{\mathit \Lambda}}{}^{2}$ $<$ $16$, $-45$ $<$ ${{\mathit c}_{{B}}}/{{\mathit \Lambda}}{}^{2}$ $<$ $46$. Combining these results with those from the closely-related electroweak ${{\mathit Z}}$-jet-jet production SIRUNYAN 2018BZ, the limits become: $-1.8$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ 2.0, $-5.8$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ 10, $-43$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ 45.

⁷

SIRUNYAN 2020BF study ${{\mathit W}^{+}}{{\mathit W}^{-}}$ production with the ${{\mathit W}}$ bosons decaying to electrons or muons. The leading (subleading) lepton is required to have a transverse momentum larger than 25 (20) GeV. Events with a same-flavor di-lepton invariant mass within 15 GeV of the ${{\mathit Z}}$ mass are rejected, as are event with a third lepton of transverse momentum larger than 10 GeV. In the same- (different-) flavor category a total of 9,604 (20,270) events are selected while the number of expected events is $9640$ $\pm490$ ($20280$ $\pm430$). Analyzing the different-flavor di-lepton invariant mass distribution, the following 95$\%$ C.L. limits are obtained in units of TeV${}^{-2}$: $-1.8$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ 1.8, $-3.6$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ 2.8, $-9.4$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ 8.5.

⁸

AABOUD 2019BA study ${{\mathit W}}{{\mathit W}}$ production in decay modes with an electron and a muon. The charged leptons are each required to have a transverse momentum larger than 27 GeV and rapidity less than 2.5. The electron-muon system is required to have a mass larger than 55 GeV and a transverse momentum larger than 30 GeV. The missing transverse energy must be larger than 20 GeV. Events containing a jet with transverse momentum exceeding 35 GeV and rapidity smaller than 4.5 are rejected. A total of 12,659 events are selected in the data, with an expected background of $4240$ $\pm477$ events. Analysing the transverse momentum spectrum of the leading charged lepton, the following 95$\%$ C.L. limits are derived in units of TeV${}^{-2}$: $-3.4$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ 3.3, $-7.4$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ 4.1, $-21$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ 18, $-1.6$ $<$ ${{\mathit c}}_{ {{\overline{\mathit W}}} {{\mathit W}} {{\mathit W}} }/\Lambda {}^{2}$ $<$ 1.6, $-76$ $<$ ${{\mathit c}}_{{{\overline{\mathit W}}}}/\Lambda {}^{2}$ $<$ 76.

⁹

SIRUNYAN 2019AD study inclusive ${{\mathit W}}{{\mathit Z}}$ production, with ${{\mathit W}}$ and ${{\mathit Z}}$ decaying to electrons or muons. The leading (subleading) charged lepton candidate from the ${{\mathit Z}}$ boson decay is required to have a transverse momentum larger than 25 GeV (10 GeV). The charged lepton candidate from the ${{\mathit W}}$ boson decay is required to have a transverse momentum larger than 25 GeV. The invariant mass of the two leptons from ${{\mathit Z}}$ decay is required to be within 15 GeV of the ${{\mathit Z}}$ mass, while the invariant mass of the tri-lepton system is required to exceed 100 GeV. A total of 3,831 tri-lepton events are observed, with a fitted SM ${{\mathit W}}{{\mathit Z}}$ signal of $3166$ $\pm62$ events and a fitted background of $666$ $\pm45$ events. The approximated ${{\mathit W}}{{\mathit Z}}$ invariant mass distribution is analyzed to set 95$\%$ C.L. limits as follows: $-4.1$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ 1.1, $-2.0$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ 2.1, $-100$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ 160, in units of TeV${}^{-2}$.

¹⁰

SIRUNYAN 2019CL study ${{\mathit W}}{{\mathit W}}$ and ${{\mathit W}}{{\mathit Z}}$ production in lepton + jet events, with one ${{\mathit W}}$ boson decaying leptonically (electron or muon), and another ${{\mathit W}}$ or ${{\mathit Z}}$ boson decaying hadronically, reconstructed as a single massive large-radius jet. In the electron channel 2,456 (2,235) events are selected in the ${{\mathit W}}{{\mathit W}}$ ( ${{\mathit W}}{{\mathit Z}}$ ) category, while in the muon channel 3,996 (3572) events are selected in the ${{\mathit W}}{{\mathit W}}$ ( ${{\mathit W}}{{\mathit Z}}$ ) category. Analysing the di-boson invariant mass distribution, the following 95$\%$ C.L. limits are obtained in units of TeV${}^{-2}$: $-1.58$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ 1.59, $-2.00$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ 2.65, $-8.78$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ 8.54.

¹¹

AABOUD 2018Q study ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}}$ events at $\sqrt {s }$ = 13 TeV with ${{\mathit Z}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ or ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ . The number of events observed in the 4${{\mathit e}}$, 2${{\mathit e}}$ 2${{\mathit \mu}}$, and 4${{\mathit \mu}}$ channels is 249, 465, and 303 respectively. Analysing the $p_T$ spectrum of the leading ${{\mathit Z}}$ boson, the following the following 95$\%$ C.L. limits are derived in units of TeV${}^{-4}$: $-5.9$ $<$ ${{\mathit c}}_{ {{\widetilde{\mathit B}}} {{\mathit W}} }/\Lambda {}^{4}$ $<$ $5.9$, $-3.0$ $<$ ${{\mathit c}_{{WW}}}/\Lambda {}^{4}$ $<$ $3.0$, $-3.3$ $<$ ${{\mathit c}_{{BW}}}/\Lambda {}^{4}$ $<$ $3.3$, $-2.7$ $<$ ${{\mathit c}_{{BB}}}/\Lambda {}^{4}$ $<$ $2.8$.

¹²

SIRUNYAN 2018BZ study ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $~\mathit jet~jet$ events at 13 TeV where ${{\mathit Z}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ $/$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ . Isolated electrons and muons are selected with $p_T$ of the leading/sub-leading lepton $>$ 30/20 GeV and $\vert {{\mathit \eta}}\vert $ $<$ 2.4, with the di-lepton invariant mass within 15 GeV of the ${{\mathit Z}}$ mass. The two highest $p_T$ jets are selected with $p_T$ of the leading/sub-leading jet $>$ 50/30 GeV respectively and dijet invariant mass $>$ 200 GeV. Templates in the transverse momentum of the ${{\mathit Z}}$ are utilized to set limits on the triple gauge couplings in the EFT and the LEP parametrizations. The following 95$\%$ C.L. limits are obtained in units of TeV${}^{-2}$: $-2.6<{{\mathit c}_{{WWW}}}/\Lambda {}^{2}<$ $2.6$ and $-8.4<{{\mathit c}_{{W}}}/\Lambda {}^{2}<$ $10.1$.

¹³

AABOUD 2017S analyze electroweak production of a ${{\mathit W}}$ boson in association with two jets at high dijet invariant mass, with the ${{\mathit W}}$ boson decaying to electron or muon plus neutrino. In the signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600 GeV, 30 events are observed in the data with $39$ $\pm4$ events expected in the Standard Model, yielding the following limits at 95$\%$ CL for the form factor cut-off scale ${{\mathit \Lambda}_{{FF}}}\rightarrow\infty{}$: $-33$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ $30$, $-170$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ $160$, $-13$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ $9$, $-580$ $<$ ${{\mathit c}}_{{{\widetilde{\mathit W}}}}/\Lambda {}^{2}$ $<$ $580$, $-11$ $<$ ${{\mathit c}}_{{{\widetilde{\mathit W}}}WW}/\Lambda {}^{2}$ $<$ $11$, in units of TeV${}^{-2}$.

¹⁴

AABOUD 2017U analyze production of ${{\mathit W}}{{\mathit W}}$ or ${{\mathit W}}{{\mathit Z}}$ boson pairs with one ${{\mathit W}}$ boson decaying to electron or muon plus neutrino, and the other ${{\mathit W}}$ or ${{\mathit Z}}$ boson decaying hadronically. The hadronic decay system is reconstructed as either a resolved two-jet system or as a single large jet. Analysing the transverse momentum distribution of the hadronic system above 100 GeV yields the following limits at 95$\%$ CL for the form factor cut-off scale ${{\mathit \Lambda}_{{FF}}}$ $\rightarrow$ $\infty{}$: $-3.1$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ $3.1$, $-19$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ $20$, $-5.1$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ $5.8$, in units of TeV${}^{-2}$.

¹⁵

KHACHATRYAN 2017O analyse ${{\mathit W}}{{\mathit Z}}$ production where each boson decays into electrons or muons. Events are required to have a tri-lepton invariant mass larger than 100 GeV, with one of the lepton pairs having an invariant mass within 20 GeV of the ${{\mathit Z}}$ boson mass. The ${{\mathit Z}}$ transverse momentum spectrum is analyzed to set 95$\%$ C.L. limits of: $-260$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ $210$, $-4.2$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ $8.0$, $-4.6$ $<$ ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ $<$ $4.2$, in units of TeV${}^{-2}$.

¹⁶

SIRUNYAN 2017X study ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}}$ / ${{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ production at 8 TeV where ${{\mathit \ell}}$ is an electron or muon with $p_T$ $>$ 30 or 25 GeV respectively. Suitable cuts are put on the $p_T$ of the dijet system and the missing $\mathit E_{T}$ of the event yielding a total of 285 and 204 ${{\mathit W}}{{\mathit V}}$ events observed in the electron and muon channels. The following 95$\%$ C.L. limits in units of TeV${}^{-2}$ are obtained: $-2.7$ $<$ ${{\mathit c}_{{W W W}}}/\Lambda {}^{2}$ $<$ 2.7, $-14$ $<$ ${{\mathit c}_{{B}}}/\Lambda {}^{2}$ $<$ 17, $-2.0$ $<$ ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ $<$ 5.7.

¹⁷

AAD 2016AR study ${{\mathit W}}{{\mathit W}}$ production in ${{\mathit p}}{{\mathit p}}$ collisions and select 6636 ${{\mathit W}}{{\mathit W}}$ candidates in decay modes with electrons or muons with an expected background of $1546$ $\pm157$ events. Assuming an EFT formulation, a fit to the transverse momentum distribution of the leading charged lepton, leads to 95$\%$ C.L. ranges of: $-4.61<{{\mathit c}_{{WWW}}}/\Lambda {}^{2}<$ 4.60, $-5.87<{{\mathit c}_{{W}}}/\Lambda {}^{2}<$ 10.54 and $-20.9<{{\mathit c}_{{B}}}/\Lambda {}^{2}<$ 26.3,in units of TeV${}^{-2}$.

¹⁸

AAD 2016P study ${{\mathit W}}{{\mathit Z}}$ production in ${{\mathit p}}{{\mathit p}}$ collisions and select 2091 ${{\mathit W}}{{\mathit Z}}$ candidates in 4 decay modes with electrons and muons, with an expected background of $1825$ $\pm7$ events. Analyzing the ${{\mathit W}}{{\mathit Z}}$ transverse momentum distribution, the resulting 95$\%$ C.L. limits are: $-3.9<{{\mathit c}_{{WWW}}}/\Lambda {}^{2}<$ 4.0, $-4.3<{{\mathit c}_{{W}}}/\Lambda {}^{2}<$ 6.8, and $-320<{{\mathit c}_{{B}}}/\Lambda {}^{2}<$ 210, in units of TeV${}^{-2}$.

¹⁹

KHACHATRYAN 2016BI determine the ${{\mathit W}^{+}}{{\mathit W}^{-}}$ production cross section using unlike sign di-lepton (${{\mathit e}}$ or ${{\mathit \mu}}$) events with high $p_T$. The leptons have $p_T$ $>$ 20 GeV/c and are isolated. Events are required to have no jets above $p_T$ of 30 GeV/c. 4847 (2233) events are selected with different (same) flavor leptons, with an expected total background of $1179$ $\pm123$ ($643$ $\pm73$) events. Analysing the di-lepton invariant mass spectrum, the following values are obtained: ${{\mathit c}_{{WWW}}}/\Lambda {}^{2}$ = $0.1$ $\pm3.2$, ${{\mathit c}_{{W}}}/\Lambda {}^{2}$ = $-3.6$ ${}^{+5.0}_{-4.5}$ and ${{\mathit c}_{{B}}}/\Lambda {}^{2}$= $-3.2$ ${}^{+15.0}_{-14.5}$, in units of TeV${}^{-2}$. The limits at 95$\%$ C.L. are: $-5.7<{{\mathit c}_{{WWW}}}/\Lambda {}^{2}<$5.9, $-11.4<{{\mathit c}_{{W}}}/\Lambda {}^{2}<$5.4 and $-29.2<{{\mathit c}_{{B}}}/\Lambda {}^{2}<$23.9, in units of TeV${}^{-2}$.

References:

PR D105 052003

Measurement of W$^\pm\gamma$ differential cross sections in proton-proton collisions at $\sqrt{s}$ = 13 TeV and effective field theory constraints

JHEP 2207 032

Measurement of the inclusive and differential WZ production cross sections, polarization angles, and triple gauge couplings in pp collisions at $ \sqrt{s} $ = 13 TeV

JHEP 2106 003

Measurements of $W^+W^-+\ge 1~$jet production cross-sections in $pp$ collisions at $\sqrt{s}=13~$TeV with the ATLAS detector

EPJ C81 163

Differential cross-section measurements for the electroweak production of dijets in association with a $Z$ boson in proton?proton collisions at ATLAS

PRL 126 252002

Measurement of the W$\gamma$ Production Cross Section in Proton-Proton Collisions at $\sqrt {s}$=13??TeV and Constraints on Effective Field Theory Coefficients

EPJ C80 43

Measurement of electroweak production of a $\mathrm{W} $ boson in association with two jets in proton?proton collisions at $\sqrt{s}=13\,\text {Te}\text {V} $

PR D102 092001

W$^+$W$^-$ boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV

EPJ C79 884

Measurement of fiducial and differential $W^+W^-$ production cross-sections at $\sqrt{s}=13$ �TeV with the ATLAS detector

JHEP 1904 122

Measurements of the pp $\to$ WZ inclusive and differential production cross section and constraints on charged anomalous triple gauge couplings at $\sqrt{s} =$ 13 TeV

JHEP 1912 062

Search for anomalous triple gauge couplings in WW and WZ production in lepton + jet events in proton-proton collisions at $\sqrt{s} =$ 13 TeV

PR D97 032005

$ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector

EPJ C78 589

Electroweak production of two jets in association with a Z boson in proton?proton collisions at $\sqrt{s}= $ 13 $\,\text {TeV}$

EPJ C77 474

Measurements of Electroweak $\mathit Wjj$ Production and Constraints on Anomalous Gauge Couplings with the ATLAS Detector

EPJ C77 563

Measurement of ${{\mathit W}}{{\mathit W}}/{{\mathit W}}{{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\mathit q}^{\,'}}$ Production with the Hadronically Decaying Boson Reconstructed as One or Two Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with ATLAS, and Constraints on Anomalous Gauge Couplings

EPJ C77 236

Measurement of the ${{\mathit W}}{{\mathit Z}}$ Production Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV and Search for Anomalous Triple Gauge Couplings at $\sqrt {s }$ = 8 TeV

PL B772 21

Search for Anomalous Couplings in Boosted ${{\mathit W}}{{\mathit W}}/{{\mathit W}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}{{\mathit q}}{{\overline{\mathit q}}}$ Production in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV

PR D93 092004

Measurements of ${{\mathit W}^{\pm}}{{\mathit Z}}$ Production Cross Sections in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector and Limits on Anomalous Gauge Boson Self-Couplings

JHEP 1609 029

Measurement of Total and Differential ${{\mathit W}^{+}}{{\mathit W}^{-}}$ Production Cross Sections in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector and Limits on Anomalous Triple-Gauge-Boson Couplings

EPJ C76 401

Measurement of the ${{\mathit W}^{+}}{{\mathit W}^{-}}$ Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV and Limits on Anomalous Gauge Couplings

Except where otherwise noted, content of the 2023 Review of Particle Physics is licensed under a Creative Commons Attribution-NonCommercial 4.0 International (CC BY-NC 4.0) license. The publication of the Review of Particle Physics is supported by US DOE, MEXT (Japan), INFN (Italy), JPS and CERN. Individual collaborators receive support for their PDG activities from their respective institutes or funding agencies. © 2023. See LBNL disclaimers.