WHY SOME FITNESS LANDSCAPES ARE FRACTAL

被引:36
作者
WEINBERGER, ED
STADLER, PF
机构
[1] UNIV VIENNA, INST THEORET CHEM, WAHRINGERSTR 17, A-1090 VIENNA, AUSTRIA
[2] MAX PLANCK INST BIOPHYS CHEM, W-3400 GOTTINGEN, GERMANY
[3] SANTA FE INST, SANTA FE, NM 87501 USA
关键词
D O I
10.1006/jtbi.1993.1120
中图分类号
Q [生物科学];
学科分类号
07 ; 0710 ; 09 ;
摘要
Many biological and biochemical measurements, for example the "fitness" of a particular genome, or the binding affinity to a particular substrate, can be treated as a "fitness landscape", an assignment of numerical values to points in sequence space (or some other configuration space). As an alternative to the enormous amount of data required to completely describe such a landscape, we propose a statistical characterization, based on the properties of a random walk through the landscape and, more specifically, its autocorrelation function. Under assumptions roughly satisfied by two classes of simple model landscapes (the N-k model and the p-spin model) and by the landscape of estimated free energies of RNA secondary structures, this autocorrelation function, along with the mean and variance of individual points and the size of the landscape, completely characterize it. Having noted that these and other landscapes of estimated replication and degradation rates all have a well-defined correlation length, we propose a classification of landscapes depending on how the correlation length scales with the diameter of the landscape. The landscapes of some of the kinetic parameters of RNA molecules scale similarly to the model landscapes introduced into evolutionary studies from other fields, such as quadratic spin glasses and the traveling salesman problem, but the correlation length of RNA landscapes are considerably smaller. Nevertheless, both the model and some of the RNA landscapes satisfy a test of self-similarity proposed by Sorkin (1988). © 1993 Academic Press. All rights reserved.
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页码:255 / 275
页数:21
相关论文
共 46 条
[1]   POPULATION-DYNAMICS IN A SPIN-GLASS MODEL OF CHEMICAL EVOLUTION [J].
AMITRANO, C ;
PELITI, L ;
SABER, M .
JOURNAL OF MOLECULAR EVOLUTION, 1989, 29 (06) :513-525
[2]   SUGGESTED MODEL FOR PREBIOTIC EVOLUTION - THE USE OF CHAOS [J].
ANDERSON, PW .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA-BIOLOGICAL SCIENCES, 1983, 80 (11) :3386-3390
[3]   COEVOLUTION IN A RUGGED FITNESS LANDSCAPE [J].
BAK, P ;
FLYVBJERG, H ;
LAUTRUP, B .
PHYSICAL REVIEW A, 1992, 46 (10) :6724-6730
[4]   KINETICS OF RNA REPLICATION - PLUS-MINUS ASYMMETRY AND DOUBLE-STRAND FORMATION [J].
BIEBRICHER, CK ;
EIGEN, M ;
GARDINER, WC .
BIOCHEMISTRY, 1984, 23 (14) :3186-3194
[5]  
BREIMAN L, 1986, PROBABILITY
[7]   RANDOM-ENERGY MODEL - AN EXACTLY SOLVABLE MODEL OF DISORDERED-SYSTEMS [J].
DERRIDA, B .
PHYSICAL REVIEW B, 1981, 24 (05) :2613-2626
[8]   SELFORGANIZATION OF MATTER AND EVOLUTION OF BIOLOGICAL MACROMOLECULES [J].
EIGEN, M .
NATURWISSENSCHAFTEN, 1971, 58 (10) :465-+
[9]  
EIGEN M, 1989, ADV CHEM PHYS, V75, P149
[10]  
EIGEN M, 1985, EMERGING SYNTHESIS S, P25