Measurements of long-range azimuthal anisotropies and associated Fourier coefficients for pp collisions at s√=5.02 and 13 TeV and p+Pb collisions at sNN−−−√=5.02 TeV with the ATLAS detector
ATLAS measurements of two-particle correlations are presented for √ s = 5.02 and 13 TeV pp collisions and for √ sNN = 5.02 TeV p+Pb collisions at the LHC. The correlation functions are measured as a function of relative azimuthal angle ∆φ, and pseudorapidity separation ∆η, using charged particles de...
| Autores: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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| Formato: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2016 |
| País: | Argentina |
| Recursos: | Consejo Nacional de Investigaciones Científicas y Técnicas |
| Repositorio: | CONICET Digital (CONICET) |
| Idioma: | inglés |
| OAI Identifier: | oai:ri.conicet.gov.ar:11336/70172 |
| Acesso em linha: | http://hdl.handle.net/11336/70172 |
| Access Level: | acceso abierto |
| Palavra-chave: | ATLAS CERN HEP LHC https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
| Resumo: | ATLAS measurements of two-particle correlations are presented for √ s = 5.02 and 13 TeV pp collisions and for √ sNN = 5.02 TeV p+Pb collisions at the LHC. The correlation functions are measured as a function of relative azimuthal angle ∆φ, and pseudorapidity separation ∆η, using charged particles detected within the pseudorapidity interval |η|<2.5. Azimuthal modulation in the long-range component of the correlation function, with |∆η|>2, is studied using a template fitting procedure to remove a “back-to-back” contribution to the correlation function that primarily arises from hard-scattering processes. In addition to the elliptic, cos (2∆φ), modulation observed in a previous measurement, the pp correlation functions exhibit significant cos (3∆φ) and cos (4∆φ) modulation. The Fourier coefficients vn,n associated with the cos (n∆φ) modulation of the correlation functions for n = 2–4 are measured as a function of charged-particle multiplicity and charged-particle transverse momentum. The Fourier coefficients are observed to be compatible with cos (nφ) modulation of per-event single-particle azimuthal angle distributions. The single-particle Fourier coefficients vn are measured as a function of charged-particle multiplicity, and charged-particle transverse momentum for n= 2–4. The integrated luminosities used in this analysis are, 64 nb−1 for the √ s = 13 TeV pp data, 170 nb−1 for the √ s = 5.02 TeV pp data and 28 nb−1 for the √ sNN = 5.02 TeV p+Pb data. |
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