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The steady state concentrations of F6P and S7P are now 6- and 4.8-fold higher, respectively, if we compare the original [ 3] and corrected Appendix A model (additional file 1).
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The transformed system reduces to a two-dimensional undriven simple harmonic oscillator in the limit E ( t ) = 0. Our result in Equation 44 is exact, and in this limit, we can easily confirm that some errors in Equation 45 in [30] are corrected (see Appendix Appendix 2).
The results can be seen in the corrected versions of appendix 4 and 5 available online.
Some numerical errors in the Tables in part I are also corrected in the present appendix.
Specifically, we use an inverse probability weighting (IPW) method that, under certain assumptions detailed in Additional file 1 (Technical appendix), corrects for potential biases attributable to differential survival distributions between those with and without missing covariates [ 18].
The online appendix has been corrected.
One of the major problems in developing and evaluating predictors is avoiding the similarity between training and testing sets; usually random splitting is not a correct procedure (Appendix 1).
Appendix contains the Klinkenberg corrected permeability for all samples tested in this study.
We have taken the model A (corrected Zhu model - version from Appendix A; additional file 1), particularly the modified subversion for cyanobacteria (sinks only for PGA and F6P) and used this model as a template for our further modeling efforts.
The steeper slope of the N-region after correction reflects the reduced cross correlation between the corrected PM- and MM-probe level data (see appendix B).
We use corrected individual weights to calculate these fractions (see Appendix A for details).
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