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91̽»¨
Black Hole

Lensing of space time around a black hole. At 91̽»¨ we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

DR Babak Abi

Research Assistant

Research theme

  • Accelerator physics
  • Instrumentation
  • Fundamental particles and interactions

Sub department

  • Astrophysics

Research groups

  • Astronomical instrumentation
  • About
  • Publications

Search for a heavy neutral particle decaying into an electron and a muon using 1 fb^-1 of ATLAS data

ArXiv 1109.3089 (2011)

Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS

ArXiv 1109.2242 (2011)

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.

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