TY - JOUR
T1 - Measurement of the inelastic proton-proton cross-section at √s=7 TeV with the ATLAS detector
AU - Yang, Un-Ki
AU - Almond, John
AU - Oh, Alexander
AU - Loebinger, Frederick
AU - Schwanenberger, Christian
AU - Brown, Gareth
AU - Da Via, Cinzia
AU - Pilkington, Andrew
AU - Aad, Georges
PY - 2011
Y1 - 2011
N2 - The dependence of the rate of proton - proton interactions on the centre-of-mass collision energy, √s, is of fundamental importance for both hadron collider physics and particle astrophysics. The dependence cannot yet be calculated from first principles; therefore, experimental measurements are needed. Here we present the first measurement of the inelastic proton - proton interaction cross-section at a centre-of-mass energy, √s, of 7 TeV using the ATLAS detector at the Large Hadron Collider. Events are selected by requiring hits on scintillation counters mounted in the forward region of the detector. An inelastic cross-section of 60.3±2.1 mb is measured for ξ>5×10-6, where ξ is calculated from the invariant mass, MX, of hadrons selected using the largest rapidity gap in the event. For diffractive events, this corresponds to requiring at least one of the dissociation masses to be larger than 15.7 GeV. © 2011 Macmillan Publishers Limited. All rights reserved.
AB - The dependence of the rate of proton - proton interactions on the centre-of-mass collision energy, √s, is of fundamental importance for both hadron collider physics and particle astrophysics. The dependence cannot yet be calculated from first principles; therefore, experimental measurements are needed. Here we present the first measurement of the inelastic proton - proton interaction cross-section at a centre-of-mass energy, √s, of 7 TeV using the ATLAS detector at the Large Hadron Collider. Events are selected by requiring hits on scintillation counters mounted in the forward region of the detector. An inelastic cross-section of 60.3±2.1 mb is measured for ξ>5×10-6, where ξ is calculated from the invariant mass, MX, of hadrons selected using the largest rapidity gap in the event. For diffractive events, this corresponds to requiring at least one of the dissociation masses to be larger than 15.7 GeV. © 2011 Macmillan Publishers Limited. All rights reserved.
U2 - 10.1038/ncomms1472
DO - 10.1038/ncomms1472
M3 - Article
SN - 2041-1723
VL - 2
JO - Nature Communications
JF - Nature Communications
IS - 1
M1 - 463
ER -