Figure 
Caption 


Measurements in dependency of ΔR_qqbar: (top left) Number of permutations per ΔR_qqbar bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of pT of the top: (top left) Number of permutations per top pT bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of eta of the top: (top left) Number of permutations per top eta bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of HT: (top left) Number of permutations per HT bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of invariant mass of the ttbar pair: (top left) Number of permutations per ttbar invariant mass bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of pT of the ttbar system: (top left) Number of permutations per ttbar pT bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of the numbers of jets: (top left) Number of permutations per jet multiplicity bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of pT of the b jet assigned to the hadronic decay branch: (top left) Number of permutations per bjet pT bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of eta of the b jet assigned to the hadronic decay branch: (top left) Number of permutations per bjet eta bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of ΔR_bbbar: (top left) Number of permutations per ΔR_bbbar bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of pT of the leading light jet assigned to the hadronic decay of the W boson: (top left) Number of permutations per leading light jet pT bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of eta of the leading light jet assigned to the hadronic decay of the W boson: (top left) Number of permutations per leading light jet eta bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of pT of the hadronically decaying W boson: (top left) Number of permutations per W pT bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 


Measurements in dependency of eta of the hadronically decaying W boson: (top left) Number of permutations per W eta bin; (top right) m_top from the 1D analysis; (bottom left) JSF and (bottom right) m_top from the 2D analysis, respectively. The systematic uncertainties are added in quadrature to the statistical uncertainties of the data. The hatched areas indicate the statistical uncertainty on the ttbar simulation. 