Erratum to: Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √s=8 TeV with the ATLAS detector (Eur. Phys. J. C (2015) 75:299, 10.1140/epjc/s10052-015-3517-3)

2015 
Eur. Phys. J. C (2015) 75:1–14:408 DOI 10.1140/epjc/s10052-015-3639-7 Erratum Erratum to: Search for new phenomena in final states with an energetic jet √ and large missing transverse momentum in pp collisions at s = 8 TeV with the ATLAS detector ATLAS Collaboration CERN, 1211 Geneva 23, Switzerland Published online: 3 September 2015 © CERN for the benefit of the ATLAS collaboration 2015. This article is published with open access at Springerlink.com Erratum to: Eur. Phys. J. C (2015) 75:299 DOI 10.1140/epjc/s10052-015-3517-3 95% CL Upper Bound on σ × BR(H → inv) [pb] In the published paper, Fig. 16 was wrongly replaced by another figure and it did not correspond to the caption. In the correct Fig. 16 shown here, the 95 % CL upper limit on σ × BR(H → invisible) as a function of the boson mass m H is presented. Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecomm ons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. Funded by SCOAP 3 . σ H Observed Expected ATLAS s = 8 TeV, 20.3 f b -1 miss E T > 2 5 0 G e V m H [GeV] Fig. 16 The observed (solid line) and expected (dashed line) 95 % CL upper limit on σ × BR(H → invisible) as a function of the boson mass m H . The shaded areas around the expected limit indicate the expected ±1σ and ±2σ ranges of limits in the absence of a signal. The expectation for a Higgs boson with BR(H → invisible) = 1, σ H , is also shown The online version of the original article can be found under doi:10.1140/epjc/s10052-015-3517-3. e-mail: atlas.publications@cern.ch
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