In Table 4, we present a partial list of transition rates caused by recombination for a 4-locus haplotype model.
The increase in reaction rate causes a transition of the transport mechanism from p-type to n-type.
In Table 2, by each designed value of (left (theta,{sigma _{1}^{2}},{sigma _{2}^{2}}right)), we can check the transitions of FPRs (false positive rates) caused by increasing the number of iterations of sampling, where the FPR is defined by (#{,i | hat {boldsymbol {w}}cdot boldsymbol {phi }, boldsymbol {x}_{i})>0, y_{i}=-1}/#{i | y_{i}=-1}).
Instead, the high local transition rates must be caused by stresses propagated along the chain backbone as indicated by changes in neighbor correlations with stress.
In all of these cases, transition rates are so high that the ancestral states of all nodes examined are equivocal; their estimated transition rates range from 0.064 to 7.174; for comparison, the highest transition rate in our data not causing all nodes to be equivocal is 0.015 (fusion in Monocotyledoneae).
UCL enhancement and strong fluctuations both in intensity and intensity ratio can be ascribed to modulation of radiative transition rates in different degrees, caused by variation of photonic mode densities around the emission wavelengths in various cavities.
In the last section, I briefly discuss possible causes for history-dependent transition rates that have been identified in the labour literature.
This causes nodes sensitive to arbitrary transition rate change to be detectable a priori only via an observed change of most likely state depending on the transition rate.
Ignoring the deaths due to causes other than breast cancer can overestimate the transition rate to breast cancer incidence, since some women may die before even experiencing breast cancer.
λ ij means the transition rate from state i to state j, and μ means the repair rate of CM after failure caused by deterioration.
