{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.135991.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2605178"}},{"@id":"https://doi.org/10.1007/JHEP07(2023)229","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":[{"@type":"Organization","name":"CMS Collaboration"},{"@type":"Organization","name":"TOTEM Collaboration"}],"creator":[{"@type":"Organization","name":"CMS Collaboration"},{"@type":"Organization","name":"TOTEM Collaboration"}],"datePublished":"2022","description":"A search is performed for exclusive high-mass $\\gamma\\gamma \\to WW$ and $\\gamma\\gamma \\to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets.  The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \\to pWWp$ and $pp \\to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)>1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 < \\xi < 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t1","@type":"Dataset","description":"Expected and observed upper limits on the AQGC operators $a^W_0/\\Lambda^2$, with no unitarization. The $y$ axis shows the limit on...","name":"$a_0^W$ Limit"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t2","@type":"Dataset","description":"Expected and observed upper limits on the AQGC operators $a^W_C/\\Lambda^2$, with no unitarization. The $y$ axis shows the limit on...","name":"$a_C^W$ Limit"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t3","@type":"Dataset","description":"Expected and observed upper limits on the AQGC operators $a^Z_0/\\Lambda^2$, with no unitarization. The $y$ axis shows the limit on...","name":"$a_0^Z$ Limit"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t4","@type":"Dataset","description":"Expected and observed upper limits on the AQGC operators $a^Z_C/\\Lambda^2$, with no unitarization. The $y$ axis shows the limit on...","name":"$a_C^Z$ Limit"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t5","@type":"Dataset","description":"Limits on LEP-like dimension-6 anomalous quartic gauge coupling parameters, with and without unitarization via a clipping procedure.","name":"Limits on LEP-like dimension-6 AQGC parameters"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t6","@type":"Dataset","description":"Conversion of limits on $a^W_0$ to dimension-8 $f_{M,i}$ operators, using the assumption of vanishing $WWZ\\gamma$ couplings to eliminate some parameters....","name":"Limits on dimension-8 operators - vanishing $WWZ\\gamma$ coupling"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t7","@type":"Dataset","description":"Conversion of limits on $a^W_0$ and $a^W_C$ to dimension-8 $f_{M,i}$ operators, using the assumption that all $f_{M,i}$ except one are...","name":"Limits on dimension-8 operators - all other couplings are zero."},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t8","@type":"Dataset","description":"{Expected and observed limits in the two-dimensional plane of $a^W_0/\\Lambda^2$ vs. $a^W_C/\\Lambda^2$. The limits are described by analytical ellipses of...","name":"WW 2D limit plot"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t9","@type":"Dataset","description":"{Expected and observed limits in the two-dimensional plane of $a^W_0/\\Lambda^2$ vs. $a^W_C/\\Lambda^2$ with unitarization imposed by clipping the signal model...","name":"WW 2D clipped limit plot"},{"@id":"https://doi.org/10.17182/hepdata.135991.v1/t10","@type":"Dataset","description":"{Expected and observed limits in the two-dimensional plane of $a^Z_0/\\Lambda^2$ vs. $a^Z_C/\\Lambda^2$. The limits are described by analytical ellipses of...","name":"ZZ 2D limit plot"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2605178?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/135991"}],"inLanguage":"en","name":"Search for high-mass exclusive $\\gamma\\gamma\\to WW$ and $\\gamma\\gamma\\to ZZ$ production in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2605178?version=1","version":1}