Abstract
Publisher’s Note: Search for supersymmetry in final states with jets, missing transverse momentum and one isolated lepton in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo mathvariant="bold">=</mml:mo><mml:mn>7</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>TeV</mml:mi></mml:math>pp collisions using<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>1</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:msup><mml:mi>fb</mml:mi><mml:mrow><mml:mo mathvariant="bold">−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup></mml:math>of ATLAS data [Phys. Rev. D<b>85</b>, 012006 (2012)
Highlights
On page 13, the second-to-last paragraph in the right-hand column should read as ‘‘Limits within the MSUGRA/CMSSM framework are derived from a second fit to signal and control regions, in ‘‘exclusion mode.’’ This fit mode tests for a specific new physics model, and uses signal predictions in the signal regions as well as in the control regions
Within the MSUGRA/CMSSM framework, and for equal squark and gluino masses, gluino masses below 820 GeV are excluded at 95% CL by this analysis
For higher values of tan, up to tan 1⁄4 40, the effect on the limits depends on m0 and m1=2; for regions in the ðm[0]; m1=2Þ plane with mq q % mq q, mass limits deteriorate by up to 10%.’’ on page 13, the first row of Table II was omitted
Summary
This paper was published online on 18 January 2012 with an omission of text on page 13. On page 13, the second-to-last paragraph in the right-hand column should read as ‘‘Limits within the MSUGRA/CMSSM framework are derived from a second fit to signal and control regions, in ‘‘exclusion mode.’’ This fit mode tests for a specific new physics model, and uses signal predictions in the signal regions as well as in the control regions.
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