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Non-linear self-organizing epigenetic processes as a third source of developmental differences: implications for genetic analysis Universiteit van Amsterdam Faculteit der Psychologie Studieonderdeel: Scriptie Datum: 19 Mei 2006 Auteur: Kees-Jan Kan Studentnummer: 9881379 E-mail: [email protected] Begeleider: drs. A. Ploeger, dr. M. E. J. Raijmakers Abstract Behavior geneticists traditionally explain phenotypic variation as a result of genotypic differences and environmental influences acting upon it. The latter are usually subdivided into within-family and between family influences. Unfortunately, according to some empirical data a substantial portion of phenotypic variance can’t be explained by this model. It is argued that non-linear epigenetic processes, capable of self-organization, constitute a third factor of phenotypic differences in development. The possible role of chaos theory and its implications for the genetic analysis of phenotypic variation is illustrated by applying the discrete logistic function as a model for development. Finally, a twin simulation study employing a more biologically plausible model, e.g. for neuronal network development, is proposed. 2 Contents 1 Introduction 4 2 Empirical evidence of a third component causing random variability 7 3 Autonomous epigenetic processes as a third source of developmental differences 11 4 The discrete logistic equation as a simple model of development 18 5 Conclusions 22 6 References 24 3 1. Introduction Since the detection of genes as units of heredity, the seemingly never-ending naturenurture controversy took its recent form of the genes-versus-environment debate. The essential question of the debate is whether biological and behavioral individual differences are primarily resulting from genetic differences or from environmental differences. In investigating and understanding these individual differences and their sources of variation a few concepts are essential. Two of the most important concepts are the concepts of phenotype ( P ), which refers to apparent, observable, measurable characteristics of the individual, and the concept of genotype ( G ), which refers to the unobservable, latent characteristics of the same individual (Grigorenko, 1999). Traditionally, (behavior) geneticists make this distinction, while it is assumed that the difference between phenotype and the underlying genotype is influenced by the environment ( E ). Usually the environmental influences are subdivided into shared ( E1 ) and non-shared ( E2 ) environmental influences (e.g. Bouchard & McGue, 2003; Molenaar, Boomsma, & Dolan, 1993). Shared environmental influences result in family members becoming more alike for a given trait. In contrast, non-shared environmental influences make them different. This model can be expressed in quantitative terms, including the interactive term ( G × E ), referring to possible combinations of genetic and environmental effects, as follows, P = G + E1 + E2 + (G × E ) With variance, VP = VG + VE1 + VE 2 + 2Cov(G )( E ) + VG×E where 2Cov(G )( E) denotes the covariance between genetic and environmental effects. One example of such gene-environment correlations is the fact that one person’s own characteristics may have evocative influences on the ways other people respond. An example for the other type of interplay between genes and environment, interaction, is that only some people are genetically susceptible to a particular allergen. As long as the environment doesn’t contain the allergen, the individual won’t be affected; non- 4 susceptible individuals will be free from the allergic effect even in an allergenic environment (Rutter et al.,1997). Besides genotype and phenotype, another central concept in behavior genetic 2 research is important: the population statistic Heritability ( h ). Heritability is defined as the proportion of phenotypic variance in a particular trait attributable to genetic variation at a given time (Gray, 1999). As a formula, it is written. h2 = VG VP To estimate the heritability of a trait, correlations between certain types of close relatives can be compared. One method of determining each of the contributing components of the phenotypic variance, and eventually the estimate of h 2 , is the selective breeding of organisms for a given trait. Subsequently, the observed response to genetic selection can be explored. However, for obvious ethical and moral reasons, scientists cannot conduct such genetic experiments on humans. The same argument holds for the recently available method of cloning organisms. But, fortunately, researchers investigating human heritability can utilize “experiments done by nature” and assess the similarity between relatives. Twin studies are an especially valuable tool in behavior genetics. Monozygotic (MZ) twins share 100% of their genes, whereas dizygotic (DZ) twins, just as regular full siblings, share, on average, only 50% of their genetic makeup. Moreover, they can share the environment in which they are raised or can be adopted at an early age in different environments. By comparing sets of correlations ( r ) between MZ and DZ twin pairs it is able to estimate the relative contributions of genetic and environmental variance components (Plomin, Defries et al., 2000), rMZ = h 2 + c 2 rDZ = h2 + c2 2 where c 2 is the proportion of shared environmental variance. Solving the equations yields, h 2 = 2(rMZ − rDZ ) 5 c 2 = rMZ − h 2 Knowing that h 2 , c 2 and e 2 (the relative contribution of non-shared environmental variance) sum up to 1, while they represent proportions, the formula for e 2 yields, e 2 = 1 − rMZ In other words, any variance that is not shared between MZ twins must be due to nonshared environmental sources of variance. It is important to note that, as a result, the error variance in this model, partially due to imprecise measurement of the phenotype, is automatically subsumed under the non-shared environmental component (Grigorenko, 1999). Despite the seeming plausibility of this standard quantitative genetic model there remains an unresolved random variability in the process of development. Several authors, including Molenaar, Boomsma, & Dolan (1993), Finch & Kirkwood (2000), Gärtner (1990), Smith (1993), Lajus et al. (2004), have suggested the presence of a third source creating phenotypic variation, in addition to genetic and environmental factors. In this paper it is argued that this source requires separate and explicit recognition in order to resolve the nature of interindividual differences. In the next section an extensive list of empirical evidence of the existence of this third source of variance is examined, followed by theoretical considerations. Also, simulation studies of twin pairs by Eaves et al. (1999) and Molenaar & Raijmakers (1999) are presented, and their implications for behavior genetic modeling are discussed. Finally, some suggestions are made for a twin simulation study, applying a realistic, biological plausible model (see Van Ooijen, van Pelt & Corner, 1995) for neuronal network development. 6 2. Empirical evidence of a third component causing random variability As pointed out in the introduction there is empirical evidence, from both animal and human studies, suggesting that some phenotypic differences can’t be explained by genetic, environmental factors, or their interactions alone. One of the pioneers in addressing this question is the German researcher Gärtner. Gärtner (1990) reviews his own laboratory’s decades-long efforts to reduce the variability of biological traits in laboratory animals by standardization of environmental conditions and genotypes, initially in order to increase the validity of experiments. Using highly inbred rats under strict environmental control (standardization of components as food, temperature, group size, etc.) did not significantly decrease the randomly distributed variation in a number of quantitative traits, such as kidney weights, when compared with a group of rats living in a natural, wild setting. Apparently neither the postnatal environment nor genes did constitute the major source of phenotypic variation. Subsequent research was performed to measure the environmental variability directly. For this purpose eight-cell stage mice embryos were divided, thereby creating monozygotic twin pairs. Each twin pair was transplanted into the uterus of the same foster mother, which raised both twins. Several physical characteristics, including body weight for example, were measured after birth and compared with those of natural born mice. The coefficients of variation appeared to be similar in both groups and it was estimated that environmental influences caused only 3-30% of the variability. In a similar experiment with Friesian cattle, an additional comparison was made with a group of divided embryos, transferred into and raised by different uterine foster mothers. As well as in the previous described experiments, a large amount (70-97%) of the random phenotypic variability remained unexplained. From these studies, the conclusion was drawn that the remaining variance had to be attributed to a third component, in addition to genetic and environmental influences. According to Gärtner (1990) this component must be inborn and may stem from (molecular) cytoplasmic differences in the zygote. Since the recently technique of cloning animals is available (another technique of creating isogenic individuals), results in concordance with those of Gärtner (1990) are 7 demonstrated. For example, Archer et al. (2003) compared cloned pigs on several physical and physiological traits with naturally bred controls. Controls were matched for age, breed and sex and were held under identical conditions. Body weight, number of teats, hair growth pattern, skin type, and blood parameters, such as alkaline, glucose and calcium, were measured. Analysis of the degree of phenotypic variation between clones and controls indicated the existence of two classes of traits. In one class of traits cloned pigs showed, as expected, less variation in relation to controls. However, in the second class the cloned animals displayed equally high or even increased variability. Although environmental conditions can’t be controlled fully, it is highly unlikely that environmental effects could account for physical traits as, for instance, hair growth pattern or skin type. The experimenters suggested that these differences in traits could be caused by small deviations introduced during cloning, microenvironmental influences or minimal initial differences in uterine conditions. Besides phenotypic variation in genetically identical animals, another kind of variation reflects the incomplete ability of organisms to develop the same phenotype under the same environmental conditions. Bilaterally organisms can show small, random deviations in morphological structures between the right and left side. This intraindividual type of variation is known as fluctuating asymmetry and is found in various traits in various animals. For an example, Stige et al. (2005) repeatedly measured feather length and color pattern of wings and tail of the pied flycatcher, a type of bird. The values of feather asymmetry persisted from nestling stage to adulthood, even across moults. These findings suggest high heritability, while the asymmetry is determined early in life and is largely unchangeable. However, genetic analyses revealed heritability was almost non-existent and shared environmental factors had little influence. Moreover, differences in within-nest conditions couldn’t explain the random variation in fluctuating asymmetry. The researchers concluded asymmetry is possibly determined by stochastic events during early stages of development, permanently affecting the feathers. In addition, according to Molenaar et al. (1993) (referring to a study of Mather & Jinks in which variation in numbers of chaetae between right and left sides of inbred fruit flies was found), it is not likely that the environment systematically influences the left and right side in a different way. 8 Fluctuating asymmetry is not limited to animals. In humans researchers observed small morphological asymmetries in various bilateral traits as well; in tooth size, skin patterns on the palms of the hands, ankle and foot breadth, elbow breadth, hand and wrist breadth, ear length and breadth, finger lengths, and facial features (see Kowner, 2001). Kowner too, puts forward that these bodily and facial variations emerge at a very young age, remain stable throughout the lifespan, and the direction is not under genetic control. A similar point of view is given in a study by Fink et al. (2004), in which it is furthermore argued that facial asymmetries seem to be the results of instabilities during the first stages in embryonic development. A related phenomenon, and another indication of developmental instability, is the development of so-called minor physical anomalies, small deviations in structural features of no functional significance (Kowner, 2001). The study of Townsend et al. (2005) illustrates nicely the role of developmental instability in creating phenotypic variability. These researchers examined the dental records and radiographs of 278 monozygotic twin pairs and found that 24 pairs had missing or extra teeth. However, 21 of these 24 pairs showed between-pair differences in patterns of expression. For example, one pair missed a premolar, one twin on the left side, the other on the right, showing a mirrored effect. In their view, the observed differences in dental features of monozygotic twins might stem from molecular interactions, leading to the initiation and ultimately the differentiation of developing teeth. So far, only studies investigating biological traits have been discussed, however there is no valid argument against the hypothesis that processes as described above could influence the organization and structure of the human brain. In fact, several studies (e.g. Thoma et al., 2002; Wright et al., 2002; Eckert et al., 2002; Steinmetz, 1996) have demonstrated the existence of atypical, non-genetically determined, asymmetries in human brain anatomy. Eckert et al. (2002) examined the heritability for asymmetry in the planum temporale in 27 monozygotic and 13 dizygotic male twins. Magnetic Resonance Imaging (MRI) measurements revealed significant dissimilarities in gyral and sulcal features between monozygotic twins. The authors hypothesized these intra-uterine effects could lead to divergent morphological development. When twins with birth weight 9 differences were excluded from genetic analysis the magnitude of asymmetry decreased, giving stronger evidence for such prenatal influences. Modern scientists believe that differences in brain structure can lead to differences in brain function and, since behavior is a reflection of brain function, can ultimately result in differences in manifest behavior (Benno, 1990, p.114). As mentioned earlier, there remains an unresolved variability in the process of development. This applies not only for (neuro-) biological data, but for behavioral data as well. For personality, intelligence and psychopathology, a substantial part of non-genetic variance has to be attributed to non-shared environmental influences, at least according to the classical behavior genetic model (Molenaar et al. 1993; Smith, 1993). Smith (1993) concentrates on a number of twin and familial studies investigating genetic and environmental contributions to intelligence. One of these studies is a study by Vroon, de Leeuw and Meester, who investigated the relationship in intelligence between sons and fathers in Holland, examined for military service at age 18. Scores of 2847 father-son pairs on the Raven Progressive Matrices test were available. Data analysis and path analysis led to the conclusion that only 3% of the variation in son's IQ was explained by IQ of the father and educational variables. Smith (1993) argues that some part of the variance in personality traits ascribed to the non-shared component is certainly due to errors in measurement, but it’s implausible to suppose measurement error accounts for an amount of variance as large as the variance caused by genetic and/or environmental factors. In the end, he concludes the intrinsic dynamics of the brain (indirect influences of spontaneous synaptic changes in activity) partially explain developmental variability. In sum, experiments with inbred and isogenic animals, studies of developmental instability in both humans and animals on bodily and brain morphology, as well as twin and familial studies present convincing evidence of the existence of a third component, in addition to genetic and environmental influences, in causing phenotypic variability in development. This component may consist of (stochastic) molecular or cellular processes creating seemingly random intra- and inter-individual phenotypic differences at both somatic and behavioral levels, and is subsumed under the non-shared environmental component in the standard behavior genetic model. In the next section some theoretical considerations by Molenaar et al. (1993) are introduced. 10 3. Autonomous epigenetic processes as a third source of developmental differences As described above, there is convincing empirical evidence indicating the existence of an independent source of phenotypic variation, in addition to genetic and environmental factors. Molenaar et al. (1993) argue that this third source may consist of autonomous non-linear epigenetic processes, having self-organizing properties. These endogenous processes are deterministic, yet give rise to chaotic output under constant genetic and environmental conditions. In order to understand what is implied by such a process, a few definitions and concepts have to be given or explained. First of all, it is useful to explain what is meant by chaos. In a meta-physical sense, chaos is the opposite of law and order. In a more scientific sense, chaos refers to some specific behavior found in certain nonlinear dynamical systems. A dynamical system is a system that changes over time. Dynamical Systems Theory, or simply Dynamics, refers to the study of these systems in the process of change1. Dynamics deals with mathematical objects that unambiguously describes (i.e. specified by a set of differential or difference equations) how the state of the system evolves over time (Beer, 2000, van Gelder & Port, 1995)). A dynamical system can change over time in either a 1 In conceptualizing how systems change over time, dynamical system theory employs geometrical representations. A system’s state corresponds with a point in an n -dimensional space ( n denotes the total number of variables), the state space. The path through which the system traverses over time is known as its trajectory or orbit and can be represented by a continuous curve or a sequence of points, depending on how time is defined; respectively in real time or in discrete time. Starting from some initial state, the state of many dynamical systems ultimately ends up into a small subset of the state space known as limit set or attractor (Bechtel & Abrahamsen, 2002). Equilibrium points and limit cycles are two examples of simple types of stable attractors producing constant, respectively endless rhythmic behavior. For stable attractors, all nearby trajectories converge to the attractor, so that small perturbations away from it will return to the identical attractor. However, some attractors are unstable, so that any perturbation away from it will drive the system away from the attractor (Beer, 2000). One example of such an unstable attractor is a chaotic trajectory, which means the bounded trajectory never repeats itself, and thus appears random. Yet, the trajectory is actually following a deterministic path, i.e. the next state of the system depends on the current state, fully determined by an algorithm (Beer, 2000; Bechtel & Abrahamsen, 2002). For that reason the functioning of such systems is generally known as deterministic chaos. 11 linear or a non-linear way. Linearity essentially means that effects are proportional to their causes. In contrast, the essence of non-linearity is that small causes, initial changes or differences, may result in large consequences. Furthermore, the presence of nonlinearity implies the possibility of very rapid changes, especially when the system in question is a feedback system. Chaos refers to these phenomena and can be defined as the unpredictability inherent in a system in which apparently random changes occur as a result of the system’s extreme “sensitive dependence on initial conditions” (Barton, 1994; Warren et al., 1998)). In popular science this phenomenon is named the butterfly effect: In theory a butterfly flapping his wings on one side of the earth can cause a heavy storm on the other side. In general, the weather is a good example of a chaotic system. It is important to note that the unpredictability of the system arises from the lack of absolute precision in the initial conditions (i.e. the values of the measurements at a given time) and not from any randomness in the equations, while they are completely deterministic, hence the random behavior is only apparent. In practice, since no measuring device can record its measurement with infinite precision, the measurement always includes a degree of uncertainty in the value. Even in theory, exact starting values of real processes would require an infinite amount of energy, which is physically impossible (Molenaar & Raijmakers, 1999). Hence, two nearly-indistinguishable sets of starting values for the same system could result in two extremely different predictions. Therefore, in the example of the weather as a chaotic system, predictions for the weather are only possible in the short-term. In general, in studying real chaotic systems long-term predictions are both theoretically and practically impossible to make, neither in advance nor in retrospect, or would be as inaccurate as any random chance prediction. A second notion concerns the non-linearity (the origin of sensitivity dependence on initial conditions) of some systems, the corresponding mathematical models and their solutions. Linear systems are most effectively modeled by a set of linear equations, which are additive. That is, solutions can be combined to obtain another solution. Non-linear systems, modeled by non-linear equations are not additive and therefore usually difficult to solve. Often, a single solution can’t be obtained and a pattern of solutions constitutes the answer. In finding such a pattern, a process called iteration is generally used: a data set is put in the set of equations and the ultimate output is fed back into the equation set 12 as new input and the whole process is repeated. Sometimes a bifurcation occurs in the pattern of solutions: a sudden jump from one set of solutions to the next. For example, such a transition is found in finger tapping. If one alternately taps the index fingers and increases the frequency gradually, one suddenly jumps into in-phase tapping once a certain limit frequency is exceeded. A small, but critical, smooth change made to the parameter values of a system causes a sudden qualitative change in the system's long-run stable dynamical behavior. In a bifurcation diagram, the geometric representation of the pattern of solutions, a bifurcation can be recognized as a splitting of the solution. Ultimately, the solutions can jump to very complex chaotic behavior. (Warren et al., 1998; Barton, 1994). Surprisingly, chaotic systems can attain certain levels of order, structure, and stability. This process is known as self-organization. Camazine (2001, p.8) provides the following definition: “Self-organization is a process in which pattern at the global level of a system emerges solely from numerous interactions among the lower-level components of the system. Moreover, the rules specifying interactions among the system’s components are executed using only local information, without reference to the global pattern.” Here, pattern (or structure) refers to a particular organized spatiotemporal arrangement of objects; something nonrandom in form, something that recurs in time, or both. It is an emergent property of the system, formatted through internal interactions of the system. That is, the order is not imposed by external shaping forces. Hence, a self-organizing process is autonomous and self-regulating. To be able to generate these highly structured patterns from homogeneous initial states the system must satisfy a few conditions (Bonabeau et al., 1997; see also Meinhardt, 1982). First, strong positive feedback (autocatalysis) must occur in order to promote changes in the system. Positive feedback reinforces change in the same direction as the initial change, so that perturbations are amplified. Second, the short-range positive feedback must trigger and be coupled with negative feedback (lateral inhibition). Negative feedback will serve as a stabilizing mechanism by promoting change in the opposite direction to a perturbation. Without negative feedback the structure would become amorphous. Third, the system must involve large numbers of components, so numerous actions and interactions will be possible. The rules specifying the interactions are based upon local information. Fourth, 13 randomness (external or internal fluctuations, perturbations, errors, noise) is crucial, generating local heterogeneities in structure which become amplified by positive feedback. Furthermore, self-organizing systems are open systems and require an influx of energy, matter or information from the environment. Self-organization and pattern formation are found in both living and non-living systems (Meinhardt, 1982; Camazine et al., 2001). A little stone can serve as a small wind shelter; thereby producing a sand deposit; this deposit increases the wind shelter and more sand is deposited. The process continues and accelerates until nature is out of resources or some physical law is playing the limiting factor. The ultimate result is a large sand dune. Other examples of patterns and pattern formation in the physical world are, among others, spiral waves produced by the Belusov-Zhabotinsky chemical reaction, star and galaxy formation, snow flakes, cloud streets, ocean waves and hurricanes. In plants one can find the branching structure of trees, the venation of leaves, the pattern of leaves in a cross-section of red cabbage, and the head of a morel mushroom. Well known examples of patterns believed to involve self-organization are found on skins, coats and shells of various animals: zebras, giraffes, tigers, leopards, snakes, seashells, etc. Patterns might be the result of animal behavior; a colony of termites is able to build complex nests and bees develop honey combs. Also animal behavior can exhibit structure in time or space; the movements of a flock of birds, fish swimming in schools and synchronized flashing of fireflies are typical examples. In animals, including humans, examples of self-organization have been described in the process of morphogenesis (Meinhardt, 1982; Camazine, 2001) the development of tissues, organs and overall body anatomy. During, embryogenesis, the embryonic development of an organism, organized spatial distributions of cells arise, which give rise to the typical structures. Skin and coat patterns as mentioned above, and also the formation of vertebrate limbs and segments of insects are, at least in part, the result of self-organizing processes. Organs, such as lungs, display a branching structure, as well as the cardiac muscle network and the blood circulatory system. Last but not least, the brain is a highly spatial organized neural network. Self-organization may provide an explanation for the puzzling fact that the total amount of information stored in the genome is far too small to describe the structure of 14 the adult brain (Molenaar et al, 1993; Benno, 1990), not to mention the entire individual (Camazine, 2001). Genes only need to carry a set of rules to generate that information. Stated somewhat differently, self-organizing processes are considered to be a factor in the ways genotypes develop into phenotypes. Here, the terms epigenetics and epigenesis come into play. Epigenetics, a term invented by C.H. Waddington, originally referred to the study of epigenesis, “the way genes and their products bring the phenotype into being” (Jablonka & Lamb, 2002). Waddington visualized the developmental system as a landscape (the epigenetic landscape2) in which multiple bifurcating and deepening valleys and hills run down from a plateau, which topology is determined by the genetic makeup (Saunders, 1993; Jablonka & Lamb, 2002). An organism’s dynamic development from genotype to phenotype can be seen as a ball making its way downhill. The course of development is able to follow many, but limited, pathways, or chreods. On the one hand, branches may rejoin further on, so that different paths will nevertheless lead to the same phenotype (canalization). On the other hand, certain paths will branch off from one another to be separated by hills so that different phenotypes can be reached from the same starting point (plasticity). Environmental influences, as well as external and internal perturbations tend to push development from its normal pathway (or may bring about a change in the landscape). Depending on the magnitude of the disturbance and the steepness and deepness of the valley, development may return to the original pathway or will be diverted to an alternative pathway. One can imagine that especially at branching points and early in development, even small perturbations may have large consequences in the end. Through time, epigenetics changed in the meaning given, and at present it is used in a different sense than Waddington applied it (Jablonka & Lamb, 2002; Haig, 2004). During the 1990’s the scope was narrowed further and further while the understanding of the molecular mechanisms that control gene activity during embryonic development and cell differentiation increased. Epigenetics became defined as “the study of mitotically and/or meiotically heritable changes in gene function that cannot be explained by changes 2 Clearly, the epigenetic landscape represents a class of dynamical systems. In Dynamical Systems Theory terms, the landscape itself is the state space, phenotypes are attractors, and chreods are trajectories. Reversely, Waddington called the state of the system epigenotype. 15 in DNA sequence” (van Speybroeck, 2002; Haig, 2004). Despite differences in meaning and explanation, both the Waddingtonian and the molecular biological sense focus on alternative developmental pathways and on the influence of environmental conditions and their consequences for the organism. As an example in line with this modern sense of epigenetics, consider the study of Fraga et al. (2005), in which the authors indicate the existence of epigenetic differences as one possible explanation for phenotypic discordances observed in monozygotic twins, such as susceptibilities to disease and differences in anthropomorphic features. The global and locus-specific differences in DNA methylation and histone acetylation of a large number of MZ twins were examined. The results demonstrated that MZ twins are epigenetically indistinguishable during early lifetime, whereas older twins display substantial differences in the patterns of DNA methylation and histone acetylation. A possible and partly explanation of this divergence is that small defects in transmitting epigenetic information through successive cell divisions accumulate during aging. This process, known as epigenetic drift, may have an important impact on gene expression, and thus on phenotype. According to the researchers these findings also support the differences found in the discordant frequency/onset of diseases between MZ twin pairs. At this point, after a highly modest introduction in chaos theory, self-organization and epigenetics, one can imagine how an organism (a non-linear dynamical system) possibly develops from genotype to phenotype. After fertilization, the non-linear mechanisms, determined by the genetic makeup, give rise to autonomous self-organizing growth processes leading to structure and patterns. However, the environment, the selforganizing process itself and their interactions with each other and with the genes tend to perturb development away from the original pathway. At critical points (bifurcation points), these perturbations may direct development following a different pathway, resulting in an alternative structure or pattern at both somatic and behavioral levels. According to Molenaar et al. (1993) it are these autonomous self-organizing processes during epigenesis that constitute the independent third source of developmental differences. Even under constant genetic and environmental influences these processes are able to create variability. The authors propose that if such a process would be computer simulated twice, where all initial conditions, genetical influences and 16 environmental influences would be identical, still different outputs would be obtained. In general, the application of the relative recent available technique of computer simulations is an interesting and welcome supplement in developmental psychology and particularly in the discussion of the third source of phenotypic variability as the next section will illustrate. 17 4. The discrete logistic equation as a simple model of development As pointed out in the previous section, intrinsic, non-linear epigenetic processes can result in chaotic time courses and might be a source of both intra- and inter-individual phenotypic variability. Eaves et al. (1999) present twin pair simulation studies using a simple non-linear developmental model capable of producing such chaotic or nearchaotic behavior. MZ and DZ twin time series were simulated under various assumptions concerning starting value and parameters. Following Eaves et al. (1999), Molenaar & Raijmakers (1999) carried out a simulation, using the same model, but applying an alternative design. Eaves et al. (1999) consider the behavior of the logistic equation xn +1 = kxn (1 − xn ) on the unit interval [0,1] as a simple non-linear model for development. The current value of x ( xn +1 ) depends on its previous value ( xn ), and, ultimately (after n iterations), on the starting value of x ( x0 ). The value of parameter k and the form3 of the logistic equation were considered to model the epigenetic process of trait x , the observed phenotype. In each of the series of simulations the phenotypic correlation between 500 twin pairs was calculated for a total of n = 50 iterations. Starting values were normally distributed with mean µ and standardized total variance (between-pairs ( σ w2 ) + within-pair variance ( σ b2 ) = 1). 3 The behavior of the logistic equation can display dramatic differences, depending on the value of k and, in some cases, on the value of x0 . For values of k ≤ 3 x converges to a fixed value, irrespective of the value of x0 . For values of k ≤ 1 the equilibrium state is always 0. For values of 3 < k < kcrit ( kcrit ≈ 3.5699 ) x will oscillate between 2 or more bifurcation points, and x0 has some influence on the order of linear and chaotic periods. Above values of kcrit , the critical value of k , the equation shows true chaotic behavior and small initial differences in starting values can lead to extreme differences in the sequential course of the function. For values of k > 4 , the iterated value of x may lie outside the unit interval, with the consequence that the value of x will approach infinity after further iteration. From an epigenetic/behavior genetic point of view, only values of 3 < k ≤ 4 were used in the simulations. 18 When the values of xn +1 (with parameter values of k = 3.9 and x0 = 0.5 for example) are plotted against the series of iterations, the points are aperiodic and hence appear random, yet they are the result of a deterministic mathematical function. The hidden order reveals itself when xn +1 is plotted against xn (autocorrelation) and all of the apparently random output from the logistic equation get arranged and fall along a strange attractor. In this case the strange attractor is shaped as a parabola (Warren et al., 1998). From the simulations of Eaves et al. (1999) it appeared that for the applied values of k = 3.4 , as well as for values of k = 3.84 , correlations remain relatively high during the process of iteration for small within-pair variances, whereas for higher within-pair variances the correlations decrease rapidly. For a value of k = 3.4 the convergence occurs in a relative smooth fashion, compared with the oscillating convergence, to approximately the same limiting values, for a value of k = 3.57 . A greater value of k ( k = 3.84 ), causes a rapid decrease in phenotypic correlation coefficients during iteration, regardless of the size of the within-pair variance. Eaves et al. (1999) draw some specific conclusions from their simulation experiments. Firstly, they conclude that, as a result of non-linear epigenetic processes small variations in initial conditions can have considerable phenotypic consequences which may look like occasion-specific environmental effects. Thus, under a linear genetic model researchers may be vainly looking for (short term) exogenous variables explaining their data, whilst in reality no environmental influences are being effective. Secondly, for genetic effects a similar argument may apply. That is, under the classical linear model one might be inclined to presume for example that specific loci are responsible for a genetic effect during the process of development, whilst in fact non-linear epigenetic processes are accountable. Finally, they conclude that when in twin and family research correlations between dizygotic twins are found to be approaching zero, whilst correlations between monozygotic twins remain high, these findings form an indication of the presence of non-linear developmental processes. According to Eaves et al. (1999), taking the actual developmental data in consideration, these processes do occur (As demonstrated by EEG spectra for example), yet these occurrences are relatively rare and may not be universally present. In other words, the suggestion is made that chaotic processes play just a rather limited part in the development of an individual. By 19 discussing the design and results from their own twin simulation studies, Molenaar & Raijmakers (1999) argue that this suggestion needs further qualification. Whereas Eaves et al. (1999) kept the values of the parameter k identical for each individual, Molenaar & Raijmakers (1999) let this parameter vary under complete genetic control (heritability = 1) with mean k = 3.8 and a between-subjects variance of 0.01. In addition, variation in the starting value was induced under near complete genetic control (heritability = 0.999999) with mean x0 = 0.5 and a between-subjects variance of 0.01. Within-pair correlations were calculated for 100 MZ and 100 DZ simulated twin pairs over a total of 200 iterations. From this alternatively designed simulation it was found that after a finite time interval, the within-pair correlations of both MZ and DZ pairs will decrease significantly to about zero, although at different rates: DZ twin-pair correlation decrease almost immediately, whilst MZ within-pair correlation is high at an early stage and decreases just at a later stage and more slowly. Applying standard behavior genetic analyses yields different estimated heritabilities and different fits to the data for separate time intervals. During an early time interval the model yields high heritability estimates and acceptable fits, whereas during intermediate intervals the model yields unacceptable low likelihood ratios. After a certain amount of time the standard model yields acceptable fits again, yet estimated heritabilities are approaching zero. Overall, it was concluded that after a finite time interval the estimations of heritability become close to zero. This result may seem surprising, while the phenotypic time series were generated by means of the discrete logistic equation in which parameter k and starting value x0 were under complete, or near complete control, meaning the initially present genetic structure has seemingly disappeared. The authors propose an estimation scheme in which the genetic structure in chaotic developmental processes can be recovered, and thereupon heritabilities can be estimated. After studying the details of the developmental process (i.e. taking the type of dynamics, elapsed time, parameter values, genetic structure etc. in consideration), time series for each single-subject should be analyzed, yielding parameter estimates for each subject. Subsequently, these individual parameter estimates can be analyzed under the standard behavior genetic model. In case of their twin simulation, this was accomplished 20 by Kalman-filtering, a technique for time series analysis, yielding individual estimates for k . Heritability of the estimated k was then estimated 1.0, and the likelihood ratio was found acceptable. Molenaar & Raijmakers (1999) further point out that in EEG spectra-analyses (the earlier discussed example given by Eaves et al., 1999) a procedure resembling the introduced estimation scheme is followed. The general conclusion drawn from the results of Eaves et al (1999) and Molenaar & Raijmakers (1999) would be that, when in fact non-linear chaotic processes could explain their phenotypic data, the application of a standard linear behavior genetic model may tempt researchers to unnecessarily seek for specific environmental and/or genetic effects, or, maybe even worse, may lead them to unwarranted conclusions concerning these data. 21 Conclusions In order to resolve the nature of interindividual differences, a potential third source of phenotypic differences in development, in addition to genetic and environmental factors has to be recognized explicitly. This independent source may consist of non-linear epigenetic processes, which can be considered to be of chaotic origin and is the result of autonomous self-organizing processes. The use of the discrete logistic equation as a chaotic model for development has showed its importance by alerting behavior geneticists to the fact that they might allocate phenotypic differences in terms of (short-term) changes in the environment or by (occasion specific) genetic effects. Therefore, recognizing the third source of variation does not only have consequences for the quantitative genetic analysis of research data, as argued below, but would also save science large amounts of time and money, which in turn can be put in more fruitful research. For quantitative behavior genetics the existence of a non-linear third source of developmental differences has far reaching consequences. The straightforward traditional model P = G + E1 + E2 + (G × E ) appears no longer adequate, while it incorrectly subsumes non-linear epigenetic effects under environmental influences, and should therefore be replaced with a model that incorporates an additional term. A proposal for the latter would be EP , which denotes Epigenesis, Epigenotype or Epigenetic influences. Hence the model including interaction effects can be formulated as P = G + E1 + E2 + EP + (G × E ) + (G × EP) + ( E × EP) Perhaps in most (longitudinal) analysis individual parameters, applying advanced mathematical techniques (e.g. Kalman filtering), have to be estimated first. Subsequently, these estimates can be subjected to the just proposed model for further analysis. Despite the major theoretical and practical importance and its implications for geneticists, the discrete logistic equation as a model for development suffers from a serious deficiency concerning psychology. The model is considerable biologically implausible. First of all, one can argue that a discrete function is a relative poor 22 description of (human) development if it is considered a real dynamical system. Dynamical processes unfold continuously in real time and not in steps as modeled by the discrete logistic equation. Secondly, this equation is a highly abstract model of development. The equation only represents “a current state dependent on the previous state”, but what biological or psychological state it denotes remains arbitrary. A more biological or psychological plausible model for development and which is able to create chaotic time series would be of additional merit. Furthermore, a model capable of self-organization would be highly interesting in view of the discussion of epigenetics. A good example of such a model, is the model of van Ooyen, van Pelt & Corner (1995) in which initially disconnected neurons organize themselves into a neuronal network under the influence of their intrinsic activity. Simulation studies in line with the design of Molenaar & Raijmakers (1999) are recommended. Their results should be analyzed with the proposed behavior genetic model (maybe by using individual parameter estimates). If these data fit well to the behavior genetic model, the implications are farreaching. It would mean that the empirical evidence of a third source of variation is supported by theory and simulations; non-linear epigenetic processes are indeed a third source of phenotypic variability and that deterministic chaos does play a role (and maybe a highly important one). It would mean that the so-called intangible variation can be (partly) tangled after all and that estimated heritabilities from previous research have to be reexamined. Finally, it would mean that the traditional nature-nurture debate has to be broadened to a nature-nurture-epigenetics debate. 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