{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.110876.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1861688"}},{"@id":"https://doi.org/10.1140/epjc/s10052-021-09545-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2021","description":"The production of $\\phi$ mesons has been studied in pp collisions at LHC energies with the ALICE detector via the dimuon decay channel in the rapidity region $2.5 < y < 4$. Measurements of the differential cross section $\\mathrm{d}^2\\sigma/$\\mathrm{d}y $\\mathrm{d} p_\\mathrm{T}$ are presented as a function of the transverse momentum ($p_\\mathrm{T}$) at the center-of-mass energies $\\sqrt{s}=5.02$, 8 and 13 TeV and compared with the ALICE results at midrapidity. The differential cross sections at $\\sqrt{s}=5.02$ and 13 TeV are also studied in several rapidity intervals as a function of $p_\\mathrm{T}$, and as a function of rapidity in three $p_\\mathrm{T}$ intervals. A hardening of the $p_\\mathrm{T}$-differential cross section with the collision energy is observed, while, for a given energy, $p_\\mathrm{T}$ spectra soften with increasing rapidity and, conversely, rapidity distributions get slightly narrower at increasing $p_\\mathrm{T}$. The new results, complementing the published measurements at $\\sqrt{s}=2.76$ and 7 TeV, allow one to establish the energy dependence of $\\phi$ meson production and to compare the measured cross sections with phenomenological models.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t1","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=5.02$ TeV at forward rapidity in pp collisions.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t2","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=8$ TeV at forward rapidity in pp collisions.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t3","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=13$ TeV at forward rapidity in pp collisions.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t4","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $2.5<y<3$...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t5","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $3<y<3.25$...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t6","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $3.25<y<3.5$...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t7","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $3.5<y<4$...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t8","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=13$ TeV in pp collisions, in the $2.5<y<2.75$...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t9","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=13$ TeV in pp collisions, in the $2.75<y<3$...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t10","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=13$ TeV in pp collisions, in the $3<y<3.25$...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t11","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=13$ TeV in pp collisions, in the $3.25<y<3.5$...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t12","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of $p_\\mathrm{T}$ at $\\sqrt{s}=13$ TeV in pp collisions, in the $3.5<y<4$...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t13","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of rapidity at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $1<p_T<2$...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t14","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of rapidity at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $2<p_T<5$...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t15","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of rapidity at $\\sqrt{s}=5.02$ TeV in pp collisions, in the $5<p_T<8$...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t16","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of rapidity at $\\sqrt{s}=13$ TeV in pp collisions, in the $1<p_T<2$...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t17","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of rapidity at $\\sqrt{s}=13$ TeV in pp collisions, in the $2<p_T<5$...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t18","@type":"Dataset","description":"$\\phi$ meson production cross section $\\mathrm{d}^2\\sigma/(\\mathrm{d}y\\mathrm{d}p_\\mathrm{T})$ as a function of rapidity at $\\sqrt{s}=13$ TeV in pp collisions, in the $5<p_T<10$...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.110876.v1/t19","@type":"Dataset","description":"$\\phi$ meson production integrated cross section as a function of $\\sqrt{s}$ for $1.5 < p_\\mathrm{T} <5$ GeV/$c$ at forward rapidity...","name":"Table 19"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1861688?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/110876"}],"inLanguage":"en","name":"Energy dependence of $\\phi$ meson production at forward rapidity in pp collisions at the LHC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1861688?version=1","version":1}