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A Mixed-Model Approach to Mapping Quantitative Trait Loci in Barley on the Basis of Multiple Environment Data
Hans-Peter Piephoaa Institut für Nutzpflanzenkunde, FB 11, Universität Kassel, 37213 Witzenhausen, Germany
Corresponding author: Hans-Peter Piepho, Universität Kassel, Steinstrasse 19, 37213 Witzenhausen, Germany., piepho{at}wiz.uni-kassel.de (E-mail)
Communicating editor: J. B. WALSH
| ABSTRACT |
|---|
In this article, I propose a mixed-model method to detect QTL with significant mean effect across environments and to characterize the stability of effects across multiple environments. I demonstrate the method using the barley dataset by the North American Barley Genome Mapping Project. The analysis raises the need for mixed modeling in two different ways. First, it is reasonable to regard environments as a random sample from a population of target environments. Thus, environmental main effects and QTL-by-environment interaction effects are regarded as random. Second, I expect a genetic correlation among pairs of environments caused by undetected QTL. I show how random QTL-by-environment effects as well as genetic correlations are straightforwardly handled in a mixed-model framework. The main advantage of this method is the ability to assess the stability of QTL effects. Moreover, the method allows valid statistical inferences regarding average QTL effects.
THERE are several different strategies to map quantitative trait loci (QTL; ![]()
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Within a frequentist framework, two different model-fitting approaches can be distinguished among procedures for QTL mapping by CIM: those based on maximum-likelihood (ML) estimation (![]()
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In this article, I analyze the barley dataset by the North American Barley Genome Mapping Project (![]()
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| MATERIALS AND METHODS |
|---|
The data:
I use the six-row Steptoe/Morex mapping population by the North American Barley Genome Mapping Project (![]()
The model for a single environment:
The model will be adjusted to DH and backcross progeny data, but it is readily extended for F2 and other populations. Assume that the F1 cross is M1QM2/m1qm2 with respect to the two flanking markers bordering the interval of interest (M1 and M2) and the QTL (Q). Define a random variable gi from the ith genotype taking value gi = 1 if the F1 gamete carries the Q allele and gi = 0 if the F1 gamete carries the q allele. In the regression approach to QTL mapping (![]()
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(1) |
where yi is a phenotypic observation for the ith genotype (i = 1, ... , N); µ is an intercept term;
is the effect of the putative QTL; c1i, c2i, ... are cofactors corresponding to markers on the map, which control for other QTL;
1,
2 ... are the associated regression coefficients; and ei is a residual accounting for both environmental variation and unexplained genetic variation. The residual genetic variation modeled by ei is regarded as random. If the unexplained residual genetic variation captured by ei is made up of a sum of small genetic contributions, the normality assumption for ei may be a suitable approximation. Note, however, that ei will also contain a component due to the different genetic effects at the putative QTL, so a more realistic model is a mixture of normal distributions, with the number of components depending on the number of genotypes at the putative QTL. The normality assumption for ei is a matter of convenience, allowing model fitting by ordinary least squares in the familiar regression framework, rather than by ML. Several authors have pointed out that using least squares in place of ML tends to cause only a marginal loss of information (![]()
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(2) |
where ß = (µ,
,
')' with
= (
1,
2, ... )', x'i =(1, zi, c'i), and c'i = (c1i, c2i, ... ). The parameter vector ß is easily extended to include multiple QTL and effects for epistasis (![]()
|
Model for data from multiple environments:
The basic model (1) may be taken as a building block for more refined modeling to account for the design. Here, I am particularly interested in modeling data from multiple-environment trials (METs). Specifically, I contend that a realistic model for genotype-by-environment effects is needed to make unbiased inferences regarding QTL effects and positions. Moreover, the problem of genetic correlation among environments needs to be taken into account in case the same set of genotypes is tested in the different environments (![]()
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(3) |
This model is derived by regarding all regression parameters in (1) as means across environments and allowing an environment-specific deviation. Thus, the environmental main effect uj corresponds to µ, aj is a deviation of the QTL effect from the average
in the jth environment, gkj (k = 1, 2, ... ) is a deviation from the average cofactor regression coefficient
k (k = 1, 2, ... ) in the jth environment, and dij is a random deviation for the ith genotype in the jth environment from the "average" residual effect ei. Note that as opposed to (1), ei in (3) is a residual genetic effect for the ith genotype, which is free of experimental error. The experimental error is now captured by dij, which models both error and residual genotype-by-environment interaction. An alternative way of deriving (3) is to allow a separate model of the form (1) for each environment, to then combine all models into a single model, and finally to partition model parameters into average effects across environments and environment-specific deviations.
All environment-specific deviations (uj, aj, gkj, and dij) and the residual genetic effect ei are regarded as random normal deviates. To fully state the model, I need to specify the variances and covariances of all random terms. The variance-covariance structure should allow sufficient generality to realistically model real data. Before stating the full second moment assumptions, model (3) is modified to allow more generality. Model (3) contains a residual genetic effect ei and a residual dij. This model corresponds to the usual factorial partitioning of main effects and interaction for genotype-by-environment data in plant breeding and quantitative genetics (![]()
2e,
2f, and
2h, respectively. This assumption is quite restrictive because it implies constancy of genetic correlation among pairs of environments as well as constancy across environments of genetic variances within environments. For this reason, I replace the term ei + dij by a term eij and initially assume that the random vector ei = (e1i, ... , eiM)' has unstructured variance-covariance matrix var(ei) = R, where R is symmetric and positive definite. I then explore various structured models for R, which have fewer parameters than in the unstructured case. The compound symmetry assumption is just a special case of this more general model with R = JM
2e + IM
2, where JM is a M x M matrix of ones everywhere, IM is the M-dimensional identity matrix, and
2 =
2f +
2h. The modified scalar model reads
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(4) |
In vector notation this can be written as
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(5) |
where ß is as defined in (1) and bj = (uj, aj, g'j)' with gj = (g1j, g2j, ... )'. The main interest of our analysis is in the average QTL effects in ß, while the random vector bj basically plays the role of an error term. To cater for generality, correlation among elements in bj is allowed. Details are discussed in the next paragraphs. A desirable feature of the model is this: instead of dropping certain genetic effects completely, I can choose whether to move them to ß and bj, or to eij. I now discuss suitable variance-covariance structures for eij and bj.
Genotype-by-environment effects:
I regard the genetic components in eij as random. When testing the same set of genotypes in the various environments, as has been assumed so far, genetic correlation among observations on the same genotype made in different environments needs to be allowed for. Many articles on the mapping of QTL based on multienvironment data corresponding to this design (![]()
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, where
21 and
22 are the variances of y1 and y2, respectively, and
is the correlation. Clearly, the variance of the mean is an increasing function of the correlation
. Similarly, in QTL mapping, accuracy of parameter estimates is expected to decrease with genetic correlation. Ignoring genetic correlation can therefore lead to overoptimistic inferences, i.e., to spurious detections and to inappropriate standard errors for parameter estimates. For this reason, I principally allow correlations among elements in ei. A variety of models for R = var(ei) can be considered. The most complex choice leaves R unstructured, and the simplest model is R = IM
2. While the unstructured model is often the most realistic one, it may entail an unnecessarily large number of parameters, when the number of environments (M) is large. Overparameterization may be avoided by imposing a certain variance-covariance structure. I consider models commonly used for the analysis of genotype-by-environment data, i.e., compound symmetry (R = JM
2e + IM
2), heteroscedastic (R = D and R = JM
2g + D, where D is a diagonal matrix; ![]()

', where
= (
1, ... ,
M)' is a vector of factor loadings associated with the individual environments (![]()

' + IM
2, corresponding to the model eij =
jui + wij, where ui is a standard normal score for the ith genotype and wij is normal with zero mean and variance
2. Environments with a large absolute value for the factor loading
j will have residuals eij more widely spread out than environments with small
j. I note in passing that model (3) is also applicable if a different set of genotypes is tested in each environment. In this case eij from different environments are stochastically independent; i.e., R is diagonal. The diagonal elements may be either homogeneous (R = IM
2) or heterogeneous (R = D).
QTL-by-environment effects and environmental main effect: In my analysis inferences are to be drawn with respect to a target population of environments. I regard the testing environments as a random sample from the target. The purpose of a mixed-model analysis is to reveal mean QTL effects across environments. Here, random QTL-by-environment interaction essentially plays the role of an error term. Moreover, the stability of QTL effects across environments is an important aspect. The larger the variance of QTL-by-environment effects the lower the stability. Finally, I can make environment-specific inferences, employing best linear unbiased predictions (BLUPs) of QTL-by-environment effects.
It is necessary to allow for correlation among the effects in bj. For example, a perfect correlation must be assumed for regression coefficients pertaining to adjacent markers, since both are linear in the additive genetic effect of the flanked QTL (![]()
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(6) |
where G is symmetrical and positive definite, but otherwise unstructured. Note that this assumption also ensures scale invariance, i.e., invariance to the particular coding for markers (0/1, 1/2, -1/1). Again, explicit modeling of the variance-covariance structure is worthwhile to keep the number of parameters low, although many parsimonious structures suffer from lack of scale invariance. I can consider the same structures as for R. It should be stressed that G does not contain genetic effects, but merely QTL-by-environmental effects and an environmental main effect.
The effect of the putative QTL in the jth environment is given by (
+ aj). The diagonal element in G corresponding to aj can therefore be interpreted as a measure of stability of the effect of the putative QTL. The larger the variance of aj, the more variable/less stable are the environment-specific QTL effects (
+ aj). The breeder will seek a large absolute value for
and a small variance for aj, i.e., a high stability. This interpretation of a variance component as a measure of QTL effect stability is akin to approaches for assessing yield stability in MET data (![]()
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It is convenient to write the full model for yij in matrix form as
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(7) |
where y = (y11, ... , yN1, y12, ... , yNM)', 1M is a vector of M ones, X = (x1, ... , xN)', ß = (µ,
,
')', IM is the M-dimensional identity matrix, b = (b'1, ... , b'M)', and e = (e11, ... , eN1, e12, ... , eNM)'. Apart from the residual variance, this model is similar to the random effects model for longitudinal data (![]()
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(8) |
and
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(9) |
Why analysis of means across environments is problematic:
If the same set of genotypes is tested in different environments, it is tempting to compute genotype means across environments and subject these to standard CIM. Such an analysis assumes that means of different genotypes,
= M-1(1'M
IN)y, are stochastically independent and have homoscedastic errors (M is the number of environments). This assumption is problematic with model (5), under which I have for the means
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(10) |
and
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(11) |
where
2R = M-21'MR1M. The important point to note here is that all elements in
are correlated among one another due to the term M-1XGX' on the right-hand side of (11). Thus, the means
violate the assumptions underlying a standard QTL analysis. An appropriate means analysis could be based on generalized least squares using (11), but this is not recommended for two reasons. First, using (11) requires an estimate of G, which necessitates an analysis of replicate data, thus annihilating the computational advantages of the means analysis. Second, and more importantly, the means themselves are unweighted and thus ignore the genetic correlation structure. Therefore the means analysis is not optimal.
Model selection:
In what follows I assume random environments and consider CIM for mean QTL effects across environments. Model selection is necessary regarding three aspects: (1) the markers to be used as cofactors, (2) the variance-covariance structure for R, and (3) the model for QTL-by-environment interaction, i.e., for G. These selection problems are briefly discussed. Unfortunately, the three problems cannot be tackled in an entirely independent manner. For example, in a joint analysis of the data, the chosen variance-covariance model will have an effect on the selected set of markers and vice versa. From a theoretical point of view it seems desirable to handle these three model components simultaneously. Due to the large number of candidate models (i.e., combinations of choices for 13), however, this simultaneous approach is not usually feasible in practice. Thus, some form of sequential approach is preferable. While this may entail the risk of missing some good-fitting models, it has the important advantage of reducing the total number of models to be considered. I suggest to first select the markers, then the variance-covariance structure for R, and finally the model for QTL-by-environment interaction (G). At each step, I use the Schwarz Bayesian Criterion (SBC) to choose among options (![]()
![]()
p log(n), where L is the maximized likelihood, p is the number of parameters, and n is the number of observations. Models with large values for SBC are preferred.
Cofactor selection:
I select cofactors by multiple linear regression of means
on marker types using the marker pair selection (MPS) approach by H.-P. PIEPHO and H. G. GAUCH (unpublished results). This procedure has three distinctive features: (i) markers are selected in adjacent pairs to increase the chance of selecting flanking markers while reducing the risk of selecting markers not linked to QTL; (ii) an exhaustive search per chromosome is used in place of simple forward selection, which reduces the risk of missing the best fitting model; (iii) a model selection criterion such as SBC is employed to select the final model among a sequence of models. Among a selected pair, I use the marker that fits best as a cofactor for CIM. The procedure was developed for models with a single error term. Extension to the mixed model (4) for the replicate data is straightforward in principle but not generally feasible at present, mainly because of the prohibitive workload of having to fit a multitude of complex models by ML or restricted maximum likelihood (REML). This is the reason for my suggestion to apply MPS to means
. The approach is of an ad hoc nature, considering the fact that strictly speaking the means violate the independence assumption. As more efficient software becomes available, applying MPS to the replicate data using a mixed-model framework is preferable.
Genotype-by-environment interaction (R):
I initially assume the most general model for QTL-by-environment interaction on the basis of the genetic model corresponding to the selected cofactors (![]()
QTL-by-environment interaction and environmental main effect (G): I now take QTL-by-environment interactions and the environmental main effect as random. Thus, I have the task of selecting an appropriate variance-covariance structure for G. The need for invariance under recoding of the markers dictates the unstructured model for G, while the parsimony principle suggests that simpler approximating structures may be worth considering. I propose to generally fit an unstructured model, except when the dimension of G is large and an unstructured model is difficult to fit.
Scanning the genome:
The same model as selected for both R and G in the previous steps is used when scanning the genome for QTL. Of course, R and G are reestimated at each putative QTL position. Note that G is extended at the scanning stage by the covariate zi for the two flanking markers. Assuming the same structure as selected for the case where xi contains only the cofactors may not be optimal. It would not be practicable, however, to select a different model at each step during the genome scan. Also, the type of model finally chosen for R and G not only depends on model fit but also on ease of estimation. Some structures for R and G may be well fitting but difficult to estimate (convergence problems, difficulty in choosing good starting values, etc.), thus making them infeasible for automated QTL scans, where the same model has to be estimated a large number of times.
| EXAMPLE |
|---|
I used the barley data to exemplify the proposed methods. MPS picked the marker pair M81/M82. Between these two, M82 had a better fit than M81 if fitted alone. Subsequently, the cofactor M82 and the interactions with environments were included in the fixed part of the model and various structures were fitted to R by the REML method. At this stage, xi did not yet contain a covariate zi for the putative QTL. All mixed-model analyses were done using ASREML (![]()
= 136 parameters for the unstructured model. The results for different models are shown in Table 2. On the basis of SBC the factor-analytic model R = JM
2e + 
' + D was selected.
|
The Wald F-statistic for cofactor(M82)-by-environment interaction in b was 10.84, which is significant at
= 5%. Thus, the interaction term was retained. In the next model-building step, the environmental main effect and interaction with M82 was regarded as random and different structures were fitted to G, using the model R = JM
2e + 
' + D. The results are given in Table 3. The unstructured model was selected for G, although D fitted slightly better according to SBC. The unstructured model is preferred based on the a priori reasoning that it ensures invariance to shifts in the covariates xi. This invariance is also useful when G is augmented by a covariate for the putative QTL.
|
I computed parameter estimates and standard errors of the fixed effects based on the selected models for R and G. For comparison, I also computed parameter estimates and standard errors on the basis of a multiple linear regression with means
. The results are reported in Table 4. The parameter estimates do not differ much in the two analyses, but the standard errors are larger with the mixed-model analysis. The analysis shows that it is not appropriate to ignore correlations among genotypes as is done in a simple analysis of means.
|
The next step is to scan the genome for a QTL by CIM. For this purpose, xi needs to be augmented by the covariate zi for the putative QTL. This again raises the question of how to model G. A priori, the unstructured model seems most appropriate, especially since there is only one cofactor so that parsimony is not a pressing issue. Thus, I used the unstructured model. The window size was 10 cM; i.e., for putative QTL within 10 cM of a cofactor, the cofactor was dropped from the model. The step size of the chromosome scan was 1 cM. During the chromosome scan, parameter estimates for G and R from the present putative QTL position were used as starting values at the next position. This resulted in convergence of the REML algorithm within a few iterations (typically 510). [One referee noted that this choice of starting values may cause convergence to a local, but not the global maximum of the (restricted) log-likelihood. In my experience the likelihood of this problem is small with a short step size. In the present example the problem was not observed. The same referee indicated that using fixed starting values gives more stable results.] At each position, I computed a Wald statistic (F) for the test of the null hypothesis of no QTL. Conditionally on the position, F asymptotically follows a
2 distribution with 1 d.f. On chromosome segments with the same set of cofactors for CIM, the type I error rate was controlled using the quick method proposed by ![]()
![]()
. The critical value was 13.01. The profiles are similar in shape, though there are some notable differences to the mixed-model analysis. The peak on chromosome 3 is much more pronounced, reaching a maximum of
80, while for the mixed-model analysis the maximum value was
20. At the estimated QTL position on chromosome 3 (58.9 cM), the estimated QTL effect was
= -0.475(±0.105) based on the mixed-model analysis. Since the estimated QTL position is within 10 cM of the cofactor M82, this cofactor was dropped for the analysis at this position. The estimate for G was

|
Thus, the variance of environmental main effects was 2.14, which is notably larger than the variance of the QTL effects across environments (0.137). The variance of QTL effects corresponds to a standard deviation of 0.370, which is fairly large relative to the average QTL effect
. This shows that the detected QTL is not very stable across environments. For example, assuming normality, the probability that the QTL effect in a randomly chosen environment (given by
+ aj) has positive sign (and thus the opposite sign of
) is
(-0.475/0.370) = 0.10, where
is the cumulative density function of the standard normal distribution. Table 5 gives BLUPs of aj. For 1 out of the 16 environments (SKg92), the resulting estimate of
+ aj has a positive sign. This finding is in good agreement with the estimated probability of 10%. Thus, despite the relatively large average QTL effect, some surprises are possible in specific environments.
|
| DISCUSSION |
|---|
A common feature of QTL analyses is that QTL effects depend on environment. Many researchers have dealt with this problem by analyzing each environment separately. This approach is quite useful, if one is interested in the particular test environments. As pointed out by ![]()
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A simple alternative to a mixed-model analysis of MET QTL data is to proceed in two steps as follows: first, the quantitative trait is analyzed by ANOVA techniques to obtain (adjusted) genotype means across environments. Second, the means together with the marker data are submitted to a routine for QTL analysis. My theoretical considerations and analysis of a real dataset led me to conclude that such analyses may lead to inappropriate inferences, mainly because standard error estimates are inappropriate. A mixed-model framework allows more valid inferences to be obtained by incorporation of different random components of variance that appropriately account for the environmental and genetic structure of the data.
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In this article I have demonstrated how to use mixed models for assessing mean and stability of QTL effects based on genotype-by-environment means from MET data. My mixed-model framework is easily extended to other settings, e.g., when spatial heterogeneity needs to be modeled at the plot level (nearest neighbor analyses; ![]()
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My analysis has assumed random environments. In a model with fixed environments, the focus is on studying QTL-by-environment interactions. It has been stressed by ![]()
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| ACKNOWLEDGMENTS |
|---|
Thanks are due to Hugh Gauch Jr. and Susan McCouch for inspiring discussions. H.F. Utz (University of Hohenheim, Germany) is thanked for helpful comments on an earlier draft. Support of the Heisenberg Programm of the Deutsche Forschungsgemeinschaft is gratefully acknowledged. Part of the research for this article was conducted while the author was visiting the Department of Biometrics and the Department of Plant Breeding, College of Agriculture and Life Sciences, Cornell University, Ithaca, NY.
Manuscript received March 22, 2000; Accepted for publication July 25, 2000.
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