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A General Statistical Framework for Mapping Quantitative Trait Loci in Nonmodel Systems: Issue for Characterizing Linkage Phases
Min Lina, Xiang-Yang Loua,b, Myron Changa, and Rongling Wua,ca Department of Statistics, University of Florida, Gainesville, Florida 32611,
b Department of Agronomy, Zhejiang University, Hangzhou, Zhejiang 310029, People's Republic of China
c Laboratory of Statistical Genetics, Zhejiang Forestry College, Lin'An, Zhejiang 311300, People's Republic of China
Corresponding author: Rongling Wu, 533 McCarty Hall C, University of Florida, Gainesville, FL 32611., rwu{at}stat.ufl.edu (E-mail)
Communicating editor: S. TAVARÉ
| ABSTRACT |
|---|
Because of uncertainty about linkage phases of founders, linkage mapping in nonmodel, outcrossing systems using molecular markers presents one of the major statistical challenges in genetic research. In this article, we devise a statistical method for mapping QTL affecting a complex trait by incorporating all possible QTL-marker linkage phases within a mapping framework. The advantage of this model is the simultaneous estimation of linkage phases and QTL location and effect parameters. These estimates are obtained through maximum-likelihood methods implemented with the EM algorithm. Extensive simulation studies are performed to investigate the statistical properties of our model. In a case study from a forest tree, this model has successfully identified a significant QTL affecting wood density. Also, the probability of the linkage phase between this QTL and its flanking markers is estimated. The implications of our model and its extension to more general circumstances are discussed.
RECENT developments of modern molecular marker technologies and statistical and computational tools have led to a great resurgence of interest in studying the inheritance and genetic architecture of a complex trait at the individual quantitative trait locus (QTL) level (![]()
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QTL mapping for model systems, in which homozygous inbred lines can be developed, is performed with well-designed experiments. One popular experimental design is to create a segregating progeny population, such as F2 or backcross, by using two complementary inbred lines. Statistical technologies for identifying QTL in these standard designs are relatively simple because there are only two segregating alleles for each genetic locus and because the allelic frequencies and linkage phases for both the markers and QTL are known. ![]()
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Unlike the model systems, it is difficult or impossible to generate inbred lines in nonmodel systems and, thus, QTL mapping for these species should be based on existing nondomesticated populations, such as a full-sib family derived from heterozygous parents (![]()
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In this article, we extend ![]()
| STATISTICAL MODEL |
|---|
Marker segregation types:
A commonly used mapping population for outcrossing species is one derived from a full-sib family generated by two heterozygous outbred parental lines. In such a full-sib family, many different marker segregation types can be expected given the heterozygosity of the two parents. ![]()
- A. Loci that are heterozygous in both parents and segregate in a 1:1:1:1 ratio, including four alleles, ab x cd; three nonnull alleles, ab x ac; three nonnull alleles and a null allele, ab x co; and two null alleles and two nonnull alleles, ao x bo.
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Table 1. Possible marker genotype cross combinations and observed marker band patterns for parents and their offspring - B. Loci that are heterozygous in both parents and segregate in a 1:2:1 ratio, which include three groups:
- B1. Three alleles form a nonsymmetrical cross type between the two parents. Of the three alleles, one is a null allele in one parent, e.g., ab x ao.
- B2. The reciprocal of B1.
- B3. Two alleles form a symmetrical type between the two parents, i.e., ab x ab.
- C. Loci that are heterozygous in both parents and segregate in a 3:1 ratio, i.e., ao x ao.
- D. Loci that are in the testcross configuration between the parents and segregate in a 1:1 ratio, which include two groups:
- D1. Heterozygous in one parent and homozygous in the other, including three alleles, ab x cc; two alleles, ab x aa, ab x oo, and bo x aa; and one allele ao x oo.
- D2. The reciprocals of D1.
A general statistical framework has been proposed for linkage analysis of different types of markers in nonmodel systems (![]()
A general framework:
Consider two outbred parental lines denoted as P and Q, each containing two homologous chromosomes 12 in a set. The cross between these two lines, 12 x 12, results in four possible parental chromosome pairings, 11, 12, 21, and 22. In this article, we used italic numbers to denote parental chromosomes.
As explained above and seen in Table 1, there may be many different marker types in a full-sib family derived from the two outbred parental lines. However, all observed markers, no matter which type they come from, can be described by two alleles, Mk1 and Mk2, at marker
k and two alleles, Mk+11 and Mk+12, at marker
k+1 for parent P. Similarly, the corresponding alleles for parent Q are described as Nk1 and Nk2 at marker
k and Nk+11 and Nk+12 at marker
k+1. Suppose there is a QTL between the two markers. The four alleles of the QTL are denoted by P1 and P2 for parent P and by Q1 and Q2 for parent Q. Analogous to the marker segregation as described in ![]()
k and the QTL and between the QTL and marker
k+1, are denoted by r, r1, and r2, respectively, with r = r1 + r2 - 2r1r2. Parent-specific difference of linkage is ignored. The alleles of these two markers and the QTL are arranged between the two homologous chromosomes in each of a total of four possible linkage phases for each parent. But the allelic linkage phases of the two markers can be known for both parents through linkage analyses of markers using a strategy proposed in ![]()
's) of linkage phase of the QTL relative to the two markers, schematically expressed, along with the order of the four QTL genotypes in the progeny, as




where the first and second subscripts of
denote two possible phases of parents P and Q, respectively, and the vertical lines for each phase combination denote two parental chromosomes 12 for each parent. Each parent, no matter which possible phase combination it has, will generate eight three-locus haploid gametes, with the gamete probabilities depending on the phase. Under phase combination
11, the eight gamete probabilities are calculated as

where we use the subscripts to denote the marker and QTL alleles. The eight gametes from parent P unite randomly with the eight gametes from parent Q, which will generate a total of 64 zygotic genotypes. The probabilities of the joint genotypes for the two markers and the QTL are calculated on the basis of the g's, which are expressed in matrix Gk(k+1) (Table 2). This joint probability matrix is composed of four vectors, gk(k+1)11, gk(k+1)12, gk(k+1)21, and gk(k+1)22, each corresponding to a different parental chromosomal pairing. The probabilities of the 2-marker gametic genotypes are expressed as

|
These 4 marker gametic probabilities are used to calculate 16 marker zygotic probabilities denoted by vector Mk(k+1). Thus, according to Bayes theorem, the matrix (Hk(k+1)) for the conditional probabilities of different QTL genotypes, conditional upon the marker interval genotypes, can be derived as

where
stands for the division of the corresponding elements of each column in a matrix by a column vector. Correspondingly, the conditional probability matrix Hk(k+1) is composed of four vectors, hk(k+1)11, hk(k+1)12, hk(k+1)21, and hk(k+1)22, each represented by a different parental chromosomal pairing.
Because of different gamete probability combinations, the joint probabilities of the 64 zygotic genotypes (and therefore the conditional probabilities of the QTL genotypes given marker genotypes) will be different among the four phase combinations. However, regardless of the difference among these four phase combinations, these conditional probabilities under different phase combinations can be obtained just by changing the order of the QTL genotypes corresponding to a particular phase combination (Table 2).
Let u and v denote the QTL alleles that an offspring i has received from parent P and Q, respectively. The conditional probability of the QTL genotype for this individual under parental-phase combination
11 is denoted by huvi expressed in one of the four vectors, hk(k+1)11, hk(k+1)12, hk(k+1)21, and hk(k+1)22. The probability with which a particular phase occurs is denoted as p for parent P and q for parent Q. Without loss of generality, let
11 = pq,
12 = p(1 - q),
21 = (1 - p)q, and
22 = (1 - p)(1 - q). Thus, the conditional probability of a QTL genotype PuQv in the full-sib family should be a mixture of the corresponding conditional probabilities under these four phase combinations, weighted by
11,
12,
21, and
22.
Assume that the phenotypic values y of a QTL genotype PuQv are normally distributed with mean µuv and variance
2, expressed as
The likelihood function of the phenotypic values (y) for all N offspring in the full-sib family is expressed in terms of a normal mixture model:
![]() |
(1) |
where
= (µuv,
2, p, q)T is the vector for unknown parameters contained within the mixture model, and
11i = h11i
11 + h12i
12 + h21i
21 + h22i
22,
12i = h12i
11 + h11i
12 + h22i
21 + h21i
22,
21i = h21i
11 + h22i
12 + h11i
21 + h12i
22, and
22i = h22i
11 + h21i
12 + h12i
21 + h11i
22 are the mixture of the conditional probabilities of different QTL genotypes over different phase combinations. The parameters contained in
can be estimated by implementing the expectation-maximization (EM) algorithm (![]()
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(2) |
with a derivative for any unknown 

where we define
![]() |
(3) |
which could be thought of as a posterior probability that the ith offspring has a QTL genotype PuQv. We then implement the EM algorithm with the expanded parameter set {
,
}, where
= {
uvi}. Conditional on
, we solve for the zeros of (
/

)log L(
|y) (Appendix A) to get our estimates of
(the M step). The estimates are then used to update
(the E step), and the process is repeated until convergence. The values at convergence are the maximum-likelihood estimates (MLEs).
Because marker information for each offspring has been incorporated into the mixture model of Equation 1, one unknown parameter r1 or r2 (that determines the location of the QTL on the interval) should be estimated along with vector
. But in practice, the QTL location is estimated by treating r1 (and therefore r2) as fixed. Using a grid approach, we can obtain the MLE of the QTL location from the peak of the profile of the log-likelihood ratio test statistics across a chromosome.
On the basis of quantitative genetic theory, the genotypic value of a QTL can be partitioned into the additive and dominant effects as

where µ is the overall mean,
u and ßv are the allelic (additive) effects of alleles u and v, respectively, and
uv is the interaction (dominant) effect at the QTL. Considering all possible alleles and allele combinations between the two parents, there are a total of four additive effects (
1 and
2 from parent P and ß1 and ß2 from parent Q) and four dominant effects (
11,
12,
21, and
22). But these additive and dominant effects are not independent and, therefore, are not estimable. After parameterization, there are two independent additive effects,
=
1 = -
2 and ß = ß1 = -ß2, and one dominant effect,
=
11 = -
12 = -
21 =
22, to be estimated.
Let m = (µuv)4x1 and a = (µ,
, ß,
)T, which can be connected by a design matrix D. We have

where

The MLE of a can be obtained from the MLE of m by

Fitting marker phenotypes:
We have built a general framework for QTL mapping based on the two-marker zygote genotypes. But in practice only the phenotypes of the marker zygotes can be observed. The numbers of the zygote phenotypes of a marker are 4, 3, 3, 3, 2, 2, and 2 for marker types A, B1, B2, C, D1, and D2, respectively (Table 1). We have designed different incidence matrices I (![]()

where
is the Kronecker product, and Ik and Ik+1 are the incidence matrices for markers
k and
k+1. For some marker types, the pattern and structure of the incidence matrices are dependent on the linkage phases of the two flanking markers. Hence, the conditional probability matrix for an observed marker type is calculated as

which is used as a basis for QTL mapping in outcrossing species.
Hypothesis tests:
The existence of a QTL of significant effect within a marker interval can be tested by calculating a log-likelihood ratio (LR) test statistic under the null (H0, there is no QTL) and alternative hypotheses (H1, there is a QTL), expressed as
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(4) |
The LR under the null hypothesis is asymptotically
2-distributed with 4 d.f. However, because the position of a QTL is not identifiable, the assumption of the
2 distribution of the LR is violated. ![]()
In a full-sib family derived from two outbred parents, it is possible that a putative QTL does not segregate in a 1:1:1:1 ratio. The genetic model (1) proposed in this article has power to test if the QTL detected is diallelic segregating 1:2:1 (like marker type B) or 1:1 (like marker type D1 or D2; see Table 1). The hypothesis that a significant QTL conforms to segregation type B can be tested by formulating

Similarly, the hypothesis for testing for the consistency of the QTL segregation to type D can be formulated as

In each of the two hypotheses above, the LR is calculated similarly to Equation 4. In practice, the segregation pattern of a significant QTL should be tested because this is important for designing an efficient breeding strategy.
| MONTE CARLO SIMULATION |
|---|
Extensive simulation studies are performed to test the statistical properties of our method for simultaneously estimating QTL position and effects and linkage phase between the QTL and markers in an outcrossed population. Suppose a full-sib family is derived from two outcrossed parents. This full-sib family is genotyped at six equally spaced (20-cM) fully informative markers (type A), forming five intervals. A QTL is hypothesized at 26 cM from the first marker (located within the second interval).
The phenotypic values for this full-sib family are simulated by giving a particular set of unknown QTL effect parameters under the linkage phase combination
11 for the two parents. These simulated data are subject to mapping analysis using our model that considers a mixture of all possible linkage phases. Thus, if the MLEs of the phase probabilities p and q are near one, this indicates that our model can precisely characterize the linkage phase for a practical phase-unknown data set. Of course, if the data are simulated under the other linkage phase combination, the values of p and q reflecting this correct linkage phase should be changed correspondingly.
The critical thresholds for declaring a significant QTL are determined from the distribution of the LR values calculated from the simulated phenotypic data assuming no QTL. The simulated data under this null hypothesis are analyzed by the statistical model proposed. The distribution of the LR values over 1000 simulation replicates can be approximated by a
2 distribution. The 99th percentile of the distribution of the maximum is used as empirical critical values to declare chromosome-wide existence of a significant QTL at the significance level
= 0.01.
Our simulation schemes include different gene action modes (additive, dominant, or overdominant), different heritabilities (H2 = 0.1 or 0.4), and different sample sizes (N = 200 or 400; Table 3). Given a heritability and the genetic variance calculated from hypothesized genetic effect values, we estimate the residual variance (
2). The accuracy and precision of parameter estimates are affected by gene action modes in three ways (Table 3). First, an overdominant QTL tends to have a more precise estimate of location than does a dominant or additive QTL. For example, the standard error (SE) of the location MLE for an overdominant QTL is 1420% smaller than those for other QTL when the heritability is 0.4 and sample size is 400. Second, for a small heritability trait, the MLEs of additive effects for an overdominant QTL are less biased than those for additive or dominant QTL. Third, the dominant effect is overestimated to a larger extent than the additive effect, especially for an overdominant QTL.
|
The estimation accuracy and precision of all parameters can be improved when heritabilities and sample sizes are increased (Table 3). For example, it is difficult to estimate the position of QTL for a low heritability (H2 = 0.1) trait when N = 200 (Fig 1A). An increased sample size (N = 400) can lead to more precise estimation of the QTL location. For a high heritability (H2 = 0.4) trait, the QTL can be precisely localized, especially when a larger sample size is used (Fig 1B). Similar trends also hold for the estimates of other QTL parameters, such as additive and dominant effects, and model parameters (overall means and residual variance; Table 3). It appears that there are more substantial improvements in the accuracy and precision of parameter estimates due to an increased heritability level from 0.1 to 0.4 than to an increased sample size from 200 to 400.
|
It is interesting to note that our model can well estimate the linkage phase between the QTL and the markers. The MLEs of phase probabilities are close to 0.90 for a small heritability trait and
0.95 for a high heritability trait (Table 3). Unlike the estimation of other parameters, the power of detecting a significant QTL seems to be more sensitive to sample sizes than to heritabilities (Table 3). For a small mapping population, the power of detecting a significant QTL is considerably reduced.
We also performed an additional simulation experiment to test the influence of incorrectly characterizing a linkage phase on QTL detection and parameter estimation. The simulated data, given H2 = 0.4 and N = 400, under linkage phase combination
11 are analyzed using models based on this phase and three other different phases,
12,
21, and
22. Because different linkage phases change only the order of the parental chromosomal pairings, the maximums of the LR values from the correct linkage phase
11 and the three incorrect linkage phases
12,
21, and
22 will be identical (see Fig 2), suggesting that phase-separate analyses have no power to select a most likely linkage phase. Also as shown by flat, crooked curves, the maximum LR value from a single linkage phase model cannot be used to precisely determine the QTL position. Fig 2 also illustrates the LR values across the linkage group calculated when all linkage phase combinations are considered simultaneously on the basis of the same simulated data set. A higher peak of the curve for a mixed-phase analysis (see also Fig 1B) indicates that our model has a greater advantage in detecting a significant QTL than usual phase-separate analyses do. When an incorrect linkage phase is used, the signs of the MLEs of the additive and dominant effects of a QTL will be reversed (results not shown).
|
| A CASE STUDY |
|---|
We use an example of an outcrossed forest tree to demonstrate the power of our statistical model for mapping QTL affecting a quantitative trait. The study material used was derived from the hybridization between two poplar species, Populus deltoides and P. euramericana. A genetic linkage map was constructed using a so-called pseudo-testcross strategy (![]()
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Our model can successfully identify a significant QTL for wood density on linkage group D17 as reported in ![]()
|
The additive effect of this significant QTL detected is 0.033, or equivalent to 7% relative to the overall mean. This QTL was found to explain
30% of the phenotypic variance for wood density in hybrid poplars. The MLE of phase probability p is 0.82, thus suggesting that there is quite a high probability to have a linkage phase
11. This indicates that the positive allele of this QTL that increases wood density is, at a probability of 0.82, in coupling phase with dominant alleles of the two markers AG/CGA-480 and AG/CGA-330 flanking the QTL.
The same material was analyzed using a traditional interval-mapping approach that assumes a possible QTL-marker linkage phase at one time. This phase-separate approach can also identify a significant QTL for wood density (data not shown), but cannot determine a correct linkage phase because the maximums of the LR values are identical between two possible linkage phases. Our method provides important information about nonallelic arrangements on the homologous chromosomes.
| DISCUSSION |
|---|
Statistical strategies for mapping QTL segregating in an inbred population have been well established (reviewed in ![]()
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Our model is advantageous over current QTL mapping methods in a full-sib family derived from outcrossing species in three aspects (![]()
![]()
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Second, our model can analyze all possible different types of markers and can test how a QTL is segregating in a family. Most of the current studies consider only fully informative markers. For example, ![]()
![]()
The correct characterization of a linkage phase between the QTL and markers for a practical data set is not only important for parameter estimation and model selection, but also essential for the application of molecular results to genetic improvement programs. For a genetic breeding program, we need to know the direction of genetic effects to make an efficient marker-assisted selection. Suppose a dominant marker allele is in a coupling phase with the positive allele of a QTL. Thus, the selection for dominant marker alleles can lead to improved phenotypes due to favorable QTL alleles. Without this knowledge, however, it is possible to select the negative allele of this QTL by using the marker allele if it is based only on the significant relationship between the marker and QTL.
The robustness and performance of our statistical method has been examined through extensive simulations. One of the most important findings is that improvements in the accuracy and precision of QTL parameters can be more substantial with increased heritabilities than with increased sample sizes (Table 2). In practice, this conclusion will have important implications for framing an optimal experiment design for precise estimation of QTL parameters. To increase parameter precision, for example, special care should be paid to the use of silvicultural measurements to increase site homogeneity, rather than planting a huge sample size on large-scale, nonuniform sites.
The model proposed is based on simple interval mapping for a single QTL affecting a quantitative trait using a mixed set of marker types. The theory extended to capture information provided by other markers outside interval markers considered is straightforward (see ![]()
![]()
![]()
![]()
![]()
| ACKNOWLEDGMENTS |
|---|
This work is partially supported by an Outstanding Young Investigators Award of the National Science Foundation of China (30128017), a University of Florida Research Opportunity Fund (02050259), and a University of South Florida Biodefense grant (7222061-12) to R.W., and National Science Foundation of China grant (30000097) to X.-Y.L. The publication of this manuscript is approved as journal series no. R-09202 by the Florida Agricultural Experiment Station.
Manuscript received July 13, 2002; Accepted for publication June 17, 2003.
| APPENDIX A |
|---|
We present the formulas for obtaining the MLEs of the unknown parameters
= (µuv,
2,
j)T in the M step. For the distribution parameters within the mixture model, we have

For the phase probabilities, we have

where

| APPENDIX B |
|---|
The pattern and structure of an incidence matrix (Ik) relating the zygotic genotypes to phenotypes for marker Mk depend on the type of this marker (Table 1). When marker Mk is from marker types A, B1, B2, B3, C, D1, and D2, we have

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