Abstract
Adaptation and evolution are quasi synonymous in popular language and Darwinian evolution is a prime application of complex adaptive system theory. We will see that adaptation does not happen automatically and discuss the concept of “error catastrophe” as a possible root for the downfall of a species. Venturing briefly into the mysteries surrounding the origin of life, we will investigate the possible advent of a “quasispecies” in terms of mutually supporting hypercycles. The basic theory of evolution is furthermore closely related to game theory, the mathematical theory of interacting agents, viz of rationally acting economic persons.
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Notes
- 1.
Note that the term “macroevolution”, coined to describe the evolution at the level of organisms, is nowadays somewhat obsolete.
- 2.
The probability to find a state with energy E in a thermodynamic system with temperature T is proportional to the Boltzmann factor \(\exp(-\beta\,E)\). The inverse temperature is \(\beta=1/(k_B T)\), with k B being the Boltzmann constant.
- 3.
The energy of a state depends in classical mechanics on the values of the available degrees of freedom, like the position and the velocity of a particle. This function is denoted Hamiltonian. In Eq. (6.21) the Hamiltonian is a function of the binary variables s and \(\mathbf{s}'\).
- 4.
Any system of binary variables is equivalent to a system of interacting Ising spins, which retains only the classical contribution to the energy of interacting quantum mechanical spins (the magnetic moments).
- 5.
The concept of order parameters in the theory of phase transition is discussed in Chap. 5.
Further Reading
A comprehensive account of the earth’s biosphere can be found in Smil (2002); a review article on the statistical approach to Darwinian evolution in Peliti (1997) and Drossel (2001). Further general textbooks on evolution, game-theory and hypercycles are Nowak (2006), Kimura (1983), Eigen (1971), Eigen (1979) and Schuster (2001). For a review article on evolution and speciation see Drossel (2001), for an assessment of punctuated equilibrium Gould (2000).
The relation between life and self-organization is further discussed by Kauffman (1993), a review of the prebiotic RNA world can be found in Orgel (1998) and critical discussions of alternative scenarios for the origin of life in Orgel (1998) and Pereto (2005).
The original formulation of the fundamental theorem of natural selection was given by Fisher (1930). For the reader interested in coevolutionary games we refer to Ebel (2002); for an interesting application of game theory to world politics as an evolving complex system see Cederman (1997) and for a field study on the green world hypothesis Terborgh et al. (2006).
Cederman, L.-E. 1997 Emergent Actors in World Politics. Princeton University Press Princeton, NJ.
Drake, J.W., Charlesworth, B., Charlesworth, D. 1998 Rates of spontaneous mutation. Genetics 148, 1667–1686.
Drossel, B. 2001 Biological evolution and statistical physics. Advances in Physics 2, 209–295.
Ebel, H., Bornholdt, S. 2002 Coevolutionary games on networks. Physical Review E 66, 056118.
Eigen, M. 1971 Self organization of matter and the evolution of biological macromolecules. Naturwissenschaften 58, 465.
Eigen, M., Schuster, P. 1979 The Hypercycle – A Principle of Natural Self-Organization. Springer, Berlin.
Fisher, R.A. 1930 The Genetical Theory of Natural Selection. Dover, New York.
Gould, S.J., Eldredge, N. 2000 Punctuated equilibrium comes of age. In Gee, H. (ed.), Shaking the Tree: Readings from Nature in the History of Life University of Chicago Press, Chicago, IL.
Jain, K., Krug, J. 2006 Adaptation in simple and complex fitness landscapes. In Bastolla, U., Porto, M., Roman, H.E., Vendruscolo, M. (eds.), Structural Approaches to Sequence Evolution: Molecules, Networks and Populations AG Porto, Darmstadt.
Kauffman, S.A. 1993 The Origins of Order. Oxford University Press, New York.
Kimura, M. 1983 The Neutral Theory of Molecular Evolution. Cambridge University Press, Cambridge.
Nowak, M.A. 2006 Evolutionary Dynamics: Exploring the Equations of Life. Harvard University Press, Cambridge, MA.
Orgel, L.E. 1998 The origin of life: A review of facts and speculations. Trends in Biochemical Sciences 23, 491–495.
Peliti, L. 1997 Introduction to the Statistical Theory of Darwinian Evolution. ArXiv preprint cond-mat/9712027.
Pereto, J. 2005 Controversies on the origin of life. International Microbiology 8, 23–31.
Schuster, H.G. 2001 Complex Adaptive Systems – An Introduction. Scator, Saarbrücken.
Schweitzer, F., Behera, L., Mühlenbein, H. 2002 Evolution of cooperation in a spatial prisoner’s dilemma. Advances in Complex Systems 5, 269–299.
Smil, V. 2002 The Earth’s Biosphere: Evolution, Dynamics, and Change. MIT Press, Cambridge, MA.
Terborgh, J., Feeley, K., Silman, M., Nunez, P., Balukjian, B. 2006 Vegetation dynamics of predator-free land-bridge islands. Journal of Ecology 94, 253–263.
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Exercises
Exercises
6.1.1 The One-Dimensional Ising Model
Solve the one-dimensional Ising model
by the transfer matrix method presented in Sect. 6.3.2 and calculate the free energy \(F(T,\!B)\), the magnetization \(M(T,B)\) and the susceptibility \(\chi(\!T)= \lim_{B\to0}\frac{\partial M(T,B)}{\partial B}\).
6.1.2 Error Catastrophe
For the prebiotic quasispecies model Eq. (6.51) consider tower-like autocatalytic reproduction rates \(W_{jj}\) and mutation rates \(W_{ij}\) (\(i\ne j\)) of the form
with \(\sigma,u_\pm\in[0,1]\). Determine the error catastrophe for the two cases \(u_+=u_-\equiv u\) and \(u_+=u\), \(u_-=0\). Compare it to the results for the tower landscape discussed in Sect. 6.3.3.
Hint: For the stationary eigenvalue equation (6.51), with \(\dot x_i=0\) (\(i=1,\ldots\)), write \(x_{j+1}\) as a function of x j and \(x_{j-1}\). This two-step recursion relation leads to a \(2\times 2\) matrix. Consider the eigenvalues/vectors of this matrix, the initial condition for x 1, and the normalization condition \(\sum_i x_i<\infty\) valid in the adapting regime.
6.1.3 Models of Life
Go to the Internet, e.g. http://cmol.nbi.dk/javaapp.php, and try a few JAVA applets simulating models of life. Select a model of your choice and study the literature given.
6.1.4 Competition for Resources
The competition for scarce resources has been modelled in the quasispecies theory, see Eq. (6.48), by an overall constraint on population density. With
one models the competition for the resource f explicitly, with a \((fr_i)\) being the regeneration rate of the resource f (species i) and d the mortality rate. Eq. (6.64) does not contain mutation terms \(\sim W_{ij}\) describing a simple ecosystem. Which is the steady-state value of the total population density \(C= \sum_i x_i\) and of the resource level f? Is the ecosystem stable?
6.1.5 Hypercycles
Consider the reaction equations (6.52) and (6.53) for \(N=2\) molecules and a homogeneous network. Find the fixpoints and discuss their stability.
6.1.6 The Prisoner’s Dilemma on a Lattice
Consider the stability of intruders in the prisoner’s dilemma Eq. (6.62) on a square lattice, as the one illustrated in Fig. 6.10. Namely, the case of just one and of two adjacent defectors/cooperators in a background of cooperators/defectors. Who survives?
6.1.7 Nash Equilibrium
Examine the Nash equilibrium and its optimality for the following two-player game:
Each player acts either cautiously or riskily. A player acting cautiously always receives a low pay-off. A player playing riskily gets a high pay-off if the other player also takes a risk. Otherwise, the risk-taker obtains no reward.
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Gros, C. (2011). Darwinian Evolution, Hypercycles and Game Theory. In: Complex and Adaptive Dynamical Systems. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-04706-0_6
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