The whole genome correlations of the same cell-type between different genotypes are extremely high (Pearson r above 0.98, Figure 2A B), indicating a strong common order parameter influencing the expression level of the entire genome, correspondent to the cell-type characterization [17].
As expected, given we are dealing with samples of the same general cell-type, genome-wide correlations are extremely high (Pearson r around 0.90), indicating a strong common order parameter influencing the expression level of the entire genome.
Steinhardt-Nelson order parameters and common neighbour analysis shows that the aluminium atoms organize in fcc {111} facet at interface and fcc far away from graphene interface.
The most likely explanation for this is, first, that any direct coupling is weak and, second, that m couples only very weakly with strain, e. Weak coupling between e and m means that the possibilities for indirect coupling with any other order parameters via common strains are strictly limited.
Many standard structural quantities, such as order parameters and correlation functions, exist for common condensed matter systems, such as spherical and rod-like particles.
The nonzero strains couple with each order parameter as λeq, λeqod, λep, and λem, whereas coupling between the order parameters themselves, either directly or indirectly through common strains, is biquadratic (i.e., λqqod, λqp, λqm, λqodp, λqodm, and λpm).
The order parameters were very similar implying that a common order tensor can be used to analyze the structure of I. Using one order tensor, RDCs of both hexosamine rings were used as restraints in molecular dynamics simulations.
Figure 6: Orientational order parameters.
Figure 5: Distribution of orientational order parameters.
The color bar indicates the values of the superconducting order parameters.
