• No se han encontrado resultados

Properties of jets measured from tracks in proton proton collisions at center of mass energy root s=7 TeV with the ATLAS detector

N/A
N/A
Protected

Academic year: 2020

Share "Properties of jets measured from tracks in proton proton collisions at center of mass energy root s=7 TeV with the ATLAS detector"

Copied!
27
0
0

Texto completo

Loading

Figure

TABLE I. Summary of systematic uncertainties for selected bins in selected cross section and p rel T distributions, for R ¼ 0:6
FIG. 1 (color online). The cross section for anti-k t charged particle jets as a function of p T , with jyj < 0:5 and radius parameter R as indicated
FIG. 3 (color online). Multiplicity of particles per charged particle jet, over the full measured rapidity range jyj < 1:9, with anti-k t radius parameter R as indicated
FIG. 4 (color online). The distribution of the fragmentation variable z for anti-k t jets with radius parameter R as indicated, in the rapidity range jyj < 1:9
+4

Referencias

Documento similar

35 ( a ) Institute of High Energy Physics, Chinese Academy of Sciences, Beijing; ( b ) Department of Modern Physics, University of Science and Technology of China, Anhui; ( c

Institute of High Energy Physics, Chinese Academy of Sciences, Beijing; (b) Department of Modern Physics, University of Science and Technology of China, Anhui; (c) Department

ATLAS Collaboration, Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in √.. s = 7 TeV

Because of the high number of b quarks in the final state, the factorization method, which provides a background estimate for events with at least three identified b jets, has

50b High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia. 51 II Physikalisches Institut, Justus-Liebig-Universita¨t Giessen,

Stepanov Institute of Physics, National Academy of Sciences of Belarus, Minsk, Belarus 93 National Scientific and Educational Centre for Particle and High Energy Physics, Minsk,

51b High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia. 52 II Physikalisches Institut, Justus-Liebig-Universit¨at Giessen,

The mass distributions observed in data together with the background estimate, its system- atic uncertainty and examples of expected signal are shown in figures 2–4 for the