model dependence is encountered once the quark masses reach their physical values. While in [@Semke:2011ez; @Semke:2012gs; @Lutz:2012mq] the $\chi-$MS scheme of [@Semke2005; @Semke:2006hd] was used, the EOMS of [@Gegelia:1999gf] was used in [@Ren:2013dzt; @Ren:2013oaa]. Both schemes protect the analytic structure of the one-loop contributions in the baryon self energies as requested by micro causality. In contrast, the IR scheme of [@Becher:1999he] was applied in [@Bruns:2012eh].

The target of our present study is to scrutinize and further improve the most comprehensive analysis of the QCD lattice data set in the isospin limit [@Lutz:2014oxa]. A quantitative description of more than 220 lattice data points for the baryon octet and decuplet states of five different lattice groups, PACS-CS, LHPC, HSC, NPLQCD and QCDSF-UKQCD [@PACS-CS2008; @LHPC2008; @HSC2008; @NPLQCD:2011; @Bietenholz:2011qq], was achieved in terms of a 12 parameter fit. The number of parameters was reduced significantly by large-$N_c$ sum rules [@Lutz:2010se; @Lutz:2011fe; @Lutz:2014jja]. More recent lattice simulation data from the ETM collaboration [@Alexandrou:2014sha] for the baryon decuplet and octet masses were predicted by this approach. The analysis was based on the relativistic chiral Lagrangian and the use of physical meson and baryon masses in the one-loop expressions that include effects up to N$^3$LO. A conventional 