{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.72303.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1346551"}},{"@id":"https://doi.org/10.1016/j.physletb.2015.05.075","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2016","description":"BNL-RHIC.  Dihadron angular correlations in $d$+Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV are reported as a function of the measured zero-degree calorimeter neutral energy and the forward charged hadron multiplicity in the Au-beam direction. A finite correlated yield is observed at large relative pseudorapidity ($\\Delta\\eta$) on the near side (i.e. relative azimuth $\\Delta\\phi\\sim0$). This correlated yield as a function of $\\Delta\\eta$ appears to scale with the dominant, primarily jet-related, away-side ($\\Delta\\phi\\sim\\pi$) yield. The Fourier coefficients of the $\\Delta\\phi$ correlation, $V_{n}=\\langle\\cos n\\Delta\\phi\\rangle$, have a strong $\\Delta\\eta$ dependence. In addition, it is found that $V_{1}$ is approximately inversely proportional to the mid-rapidity event multiplicity, while $V_{2}$ is independent of it with similar magnitude in the forward ($d$-going) and backward (Au-going) directions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t1","@type":"Dataset","description":"Correlated dihadron yield, per radian per unit of pseudorapidity, as a function of $\\Delta\\phi$ for 1.2 < $|\\Delta\\eta|$ < 1.8...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t2","@type":"Dataset","description":"Correlated dihadron yield, per radian per unit of pseudorapidity, as a function of $\\Delta\\phi$ for 1.2 < $|\\Delta\\eta|$ < 1.8...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t3","@type":"Dataset","description":"Correlated dihadron yield, per radian per unit of pseudorapidity, as a function of $\\Delta\\phi$ for -4.5 < $\\Delta\\eta$ < -2...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t4","@type":"Dataset","description":"Correlated dihadron yield, per radian per unit of pseudorapidity, as a function of $\\Delta\\phi$ for -4.5 < $\\Delta\\eta$ < -2...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t5","@type":"Dataset","description":"Correlated dihadron yield, per radian per unit of pseudorapidity, as a function of $\\Delta\\phi$ for 2 < $\\Delta\\eta$ < 4.5...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t6","@type":"Dataset","description":"Correlated dihadron yield, per radian per unit of pseudorapidity, as a function of $\\Delta\\phi$ for 2 < $\\Delta\\eta$ < 4.5...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t7","@type":"Dataset","description":"The $\\Delta\\eta$ dependence of the near-side (|$\\Delta\\phi$| < $\\pi/3$) correlated yield. Positive(negative) $\\eta$ corresponds to d(Au)-going direction. Only high ZDC-Au...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t8","@type":"Dataset","description":"The $\\Delta\\eta$ dependence of the away-side (|$\\Delta\\phi - \\pi$| < $\\pi/3$) correlated yield. Positive(negative) $\\eta$ corresponds to d(Au)-going direction. Only...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t9","@type":"Dataset","description":"The $\\Delta\\eta$ dependence of the ratio of the near- to away-side correlated yields in d+Au collisions. Positive(negative) $\\eta$ corresponds to...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t10","@type":"Dataset","description":"The $\\Delta\\eta$ dependence of the second harmonic Fourier coefficient, V2, in low ZDC-Au activity d+Au collisions.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t11","@type":"Dataset","description":"The $\\Delta\\eta$ dependence of the second harmonic Fourier coefficient, V2, in high ZDC-Au activity d+Au collisions.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t12","@type":"Dataset","description":"Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by FTPC-Au. Trigger particles are from...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t13","@type":"Dataset","description":"Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC. Trigger particles are from...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t14","@type":"Dataset","description":"Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC. Trigger particles are from...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t15","@type":"Dataset","description":"Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t16","@type":"Dataset","description":"Fourier coefficient V2 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by FTPC-Au. Trigger particles are from...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t17","@type":"Dataset","description":"Fourier coefficient V2 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t18","@type":"Dataset","description":"Fourier coefficient V2 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t19","@type":"Dataset","description":"Fourier coefficient V2 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t20","@type":"Dataset","description":"Fourier coefficient V3 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selections is by FTPC-Au. Trigger particles are from...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t21","@type":"Dataset","description":"Fourier coefficient V3 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t22","@type":"Dataset","description":"Fourier coefficient V3 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.72303.v1/t23","@type":"Dataset","description":"Fourier coefficient V3 versus the measured mid-rapidity charged particle $dN_{ch}/d\\eta$. Event activity selection is by ZDC-Au. Trigger particles are from...","name":"Table 23"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1346551?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/72303"}],"inLanguage":"en","name":"Long-range pseudorapidity dihadron correlations in $d$+Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1346551?version=1","version":1}