Measurement of the cross section for the production of a W boson in association with b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector

ArXiv 1109.147 (2011)

Measurement of the cross-section for b-jets produced in association with a Z boson at sqrt(s)=7 TeV with the ATLAS detector

ArXiv 1109.1403 (2011)

Measurement of the inelastic proton-proton cross-section at root s=7 TeV with the ATLAS detector

Nature Communications Springer Nature 2 (2011) 463

Authors:

K Cranmer, F Crescioli, PVM Da Silvaa, C Da Via, W Davey, T Davidek, N Davidson, R Davidson, R De Asmundis, S De Castro, PEDCF Salgado, J De Graat, U De Sanctis, A De Santo, JBDV De Regie, S Dean, J Degenhardt, PA Delsart, C Deluca, D Derendarz, JE Derkaouid, A Dewhurst, B Dewilde, J Ernwein, S Errede

Abstract:

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.

Measurements of the electron and muon inclusive cross-sections in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector

ArXiv 1109.0525 (2011)

A new model for the infrared emission of IRAS F10214+4724

Proceedings of the International Astronomical Union 7:S284 (2011) 205-209

Authors:

A Efstathiou, N Christopher, A Verma, R Siebenmorgen

Abstract:

We present a new model for the infrared emission of the high redshift hyperluminous infrared galaxy IRAS F10214+4724 which takes into account recent photometric data from Spitzer and Herschel that sample the peak of its spectral energy distribution. We first demonstrate that the combination of the AGN tapered disc and starburst models of Efstathiou and coworkers, while able to give an excellent fit to the average spectrum of type 2 AGN measured by Spitzer, fails to match the spectral energy distribution of IRAS F10214+4724. This is mainly due to the fact that the ν S ν distribution of the galaxy falls very steeply with increasing frequency (a characteristic of heavy absorption by dust) but shows a silicate feature in emission. We propose a model that assumes two components of emission: clouds that are associated with the narrow-line region and a highly obscured starburst. The emission from the clouds must suffer significantly stronger gravitational lensing compared to the emission from the torus to explain the observed spectral energy distribution. © 2012 International Astronomical Union.