{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.130960.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2165920"}},{"@id":"https://doi.org/10.1016/j.physletb.2023.137849","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t1","@type":"Dataset","description":"Jet shapes, $\\rho(\\Delta r)$, for inclusive and b jets as function of $\\Delta r$ from pp and PbPb collisions at...","name":"Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t2","@type":"Dataset","description":"Jet shapes, $\\rho(\\Delta r)$, for inclusive and b jets as function of $\\Delta r$ from pp and PbPb collisions at...","name":"Figure 1b"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t3","@type":"Dataset","description":"Jet shapes, $\\rho(\\Delta r)$, for inclusive and b jets as function of $\\Delta r$ from pp and PbPb collisions at...","name":"Figure 1c"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t4","@type":"Dataset","description":"Jet shape ratios ($\\rho(\\Delta r)_{\\mathrm{PbPb}}/\\rho(\\Delta r)_{\\mathrm{pp}}$) for inclusive and b jets as function of $\\Delta r$ at $\\sqrt{s_{NN}} = 5.02$...","name":"Figure 1d"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t5","@type":"Dataset","description":"Jet shape ratios ($\\rho(\\Delta r)_{\\mathrm{PbPb}}/\\rho(\\Delta r)_{\\mathrm{pp}}$) for inclusive and b jets as function of $\\Delta r$ at $\\sqrt{s_{NN}} = 5.02$...","name":"Figure 1e"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t6","@type":"Dataset","description":"Jet shape ratios ($\\rho(\\Delta r)_{\\mathrm{PbPb}}/\\rho(\\Delta r)_{\\mathrm{pp}}$) for inclusive and b jets as function of $\\Delta r$ at $\\sqrt{s_{NN}} = 5.02$...","name":"Figure 1f"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t7","@type":"Dataset","description":"Transverse momentum profile difference $P(\\Delta r)_{\\mathrm{PbPb}}-P(\\Delta r)_{\\mathrm{pp}}$ vs. $\\Delta r$ for inclusive and b jets at $\\sqrt{s_{NN}} = 5.02$ TeV.","name":"Figure 1g"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t8","@type":"Dataset","description":"Transverse momentum profile difference $P(\\Delta r)_{\\mathrm{PbPb}}-P(\\Delta r)_{\\mathrm{pp}}$ vs. $\\Delta r$ for inclusive and b jets at $\\sqrt{s_{NN}} = 5.02$ TeV.","name":"Figure 1h"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t9","@type":"Dataset","description":"Transverse momentum profile difference $P(\\Delta r)_{\\mathrm{PbPb}}-P(\\Delta r)_{\\mathrm{pp}}$ vs. $\\Delta r$ for inclusive and b jets at $\\sqrt{s_{NN}} = 5.02$ TeV.","name":"Figure 1i"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t10","@type":"Dataset","description":"Jet shape ratios ($\\rho(\\Delta r)_{\\mathrm{b}}/\\rho(\\Delta r)_{\\mathrm{incl.}}$) as function of $\\Delta r$ from pp and PbPb collisions at $\\sqrt{s_{NN}}= 5.02$ TeV.","name":"Figure 1j"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t11","@type":"Dataset","description":"Jet shape ratios ($\\rho(\\Delta r)_{\\mathrm{b}}/\\rho(\\Delta r)_{\\mathrm{incl.}}$) as function of $\\Delta r$ from pp and PbPb collisions at $\\sqrt{s_{NN}} = 5.02$...","name":"Figure 1k"},{"@id":"https://doi.org/10.17182/hepdata.130960.v1/t12","@type":"Dataset","description":"Jet shape ratios ($\\rho(\\Delta r)_{\\mathrm{b}}/\\rho(\\Delta r)_{\\mathrm{incl.}}$) as function of $\\Delta r$ from pp and PbPb collisions at $\\sqrt{s_{NN}} = 5.02$...","name":"Figure 1l"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2165920?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/130960"}],"inLanguage":"en","name":"Search for medium effects using jets from bottom quarks in PbPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2165920?version=1","version":1}