The issues about an unevenness of a genome arose in particular in a distribution of coverage of sequencing reads mapped to a genome ¹ . There, the deviations of a reads’ coverage from a 'classical' Lange-Waterman model, which was constructed following a Poisson distribution for short genome fragments, reflects some features of self-affinity for most frequent genome fragments in addition to the previously observed over-dispersion of a ''Poisson'' peak. There, the effect was observed stably in several analyzed genomes and is to be treated as a robust enough phenomenon to be discovered further and in depth.

The features of self-affinity in DNA sequences were detected at the very early days of genomics, in a classical work of Peng et al. ² ; a definition of the fractal dimension for the one-dimensional series was proposed there, and DNA sequences were a model of ''fractal''-like series.

The self-affinity features in a phenomenon imply the influence of perturbations with infinite dispersion, or the presence of a so-called 'fat-tail' in their probability distribution, and these features are difficult to detect and describe.

Here, an approach is proposed to detect and apply a measure to these 'perturbations' focusing on the phenomenon mentioned, which was observed in coverage distributions. The relevance of a proposed research project is demonstrated on a model of evolution of humans restored from some of the present-day human genomes; confusions which are accumulated in solving of this scientific problem were in fact a motif to drive out the research.

Self-affinity features are a property of 'transitional' period, and a description of these features is borrowed from approaches to a so-called 'Ising model', the model where a phase transition in a mutual orientation of spins in a crystal is explained. The heating of magnetic crystal leads to abrupt disappearance of magnetic momentum, and an approximation of this phenomenon is simulated in the Ising model. In a very simplified form, the interactions in crystal are presented there as an increase of energy if two spins in a linear chain are oriented in the same direction, and a critical temperature of phase transition ( T _c ) is derived from a strength of these interactions ('coupling constant').

The cooling led in turn to a sudden appearance of magnetic momentum, and a decrease of a temperature close to a critical temperature leads to accumulation of 'islands', long enough fragments where spins are oriented in the same order. Ordered fragments in a one-dimensional spin chain can be compared to identical fragments of genome sequences, and a distribution of these fragments allows to describe there the features of self-affinity.

In the frames of statistical physics, an expression for the probability of island of length k was obtained by Dziamagra ³ , as an applied case of the so-called 'Landau-Zener' transition'':

p ( k , τ ) ~ e τ k 2

This is a point where a distribution with infinite dispersion can be introduced, assuming that a power coefficient 2 in this Gaussian-like distribution is substituted to some floating power coefficient D < 2, a dimension of 'intrinsic' self-affinity of the underlaid process. The model constructed above depends on the two flexible parameters; intrinsic dimension D and a parameter τ, a rate of cooling, or a rate of approaching a transitional phase. This model allows us to explain over-dispersion of the genome coverage distributions mentioned above ( Figure 1) and to fit the parameters to a measure of unevenness of human genomes, trying to reconstruct their evolution most precisely . The distribution of 'islands' for human genomes can be obtained as distribution of lengths of completely identical fragments in the genomes; lists of polymorphic positions (SNP) from ''1000 genomes'' project ⁴ were used as a representation of genomes. A similar distribution of fragment sizes is observed for this data ( Figure 2A; Table 1). The clusters for the three races are clearly seen for both genetic distance and for tails of 'island' sizes in genome-genome comparison ( Figure 2B). To interpret this, higher unevenness relative to same genetic distance means higher 'equilibration rate', higher mutation rates, and a lesser slope of a fitting line.

For the two independent populations, the distance does not depend on heterogeneity in populations; a simple model of exponential development can provide a dependency of average genetic distance within population.

p x ≈ p 0 x + t r x 1 N 0 ∑ n N g ( n α n ) k ~ e m ≈ 1 + m d x = p 0 + t r x N g + t r y N g

The simplified model of evolution of human ethnic groups is shown in Figure 3, and for further consideration it was reduced to just clarify a separation between three human races. In this case, the model can be further reduced to a system of equations (2). The events which are assumed here as events of separation between races are (a) separation between modern Asians and modern Europeans, which happened nearly just after an expansion to America, about ten thousand years ago; and (b) expansion of modern humans to Eurasia, about fifty thousand years ago.

p a = b a p a e + t k a r p e = b e p a e + t k e r d a e = p a e + 2 t r p A = b A p 0 + ( t + T ) k A r p a e = b a e p 0 + T k a e r d A e = p 0 + 2 ( T + t ) r

The mutation rate 10 ^-9 per nucleotide per year can be transformed as 3 per genome per year = 3000 per genome per thousand years, 3000 mutations per 700000 SNP, so that r in the equations above should be about 0.004.

Having a requirement that p ₀ ≥ 0, the r should be less than 0.0029. Rates of development are assumed to be unknown, what is only known is a dependency between a rate of development and a linear coefficient m. Values of b _a, b _e, b _A, p _ae, k _ae which are attributes of a passed history are also assumed to be unknown.

For a marginal but the most confident assumption , p ₀ = 0, p _ae = 0.21 , k _A = 1.65 and k _ae = 1.81. Unevenness in a comparison between groups is a weighted average of evolutionary paths from a time of separation, so that if kA ~ mA, k _e ~ m _e , then k _ae ~ (m _AeT + m _A(T + t) + m _e t)/2(T + t); k _ae ≈ 0.0141. Following a log-linear approximation, k _a and k _e , for modern Asians and Europeans, should be about 1.74 and 1.76.

The genetic diversity of Asians in a time of separation is than estimated as 0.15, much lower than a pool of genotypes just before the separation ( p _ae = 0.21). For Europeans, the pool of genotypes was wider, about 0.20.

What is known is that Eurasia is a continent with good communications, and that it was populated mostly by ancestors of present-day Asian race before the time of last separation, or 'crash', in better words. It is also known that ancestors of modern Europeans began to expand to Europe mostly after that 'crash'; the founders of the latest expansion originated from tribes which developed slowly for a long time somewhere in an area of central Asia mountains. The wide expansion to Eurasia for the ancient pre-Asian race was characterized, instead, by a substantive increase of genome unevenness. Some of it now is lost, some are kept in native Americans, and, for modern Asians, the instabilities in diverged genomes were neutralized by a long enough period of stable slow development after the crash.

Selection of individuals was almost the same as in Schiffels and Durbin ⁵ , the difference with that model is that non-Gaussian features in genomes are considered here explicitly. This has a substantial influence on a reconstructed history of the three human races. Dealing with self-affine phenomena is difficult and risky, but it by no way can be ignored in any of valuable challenges to a present-day science.