# Erlang renewal models for genetic recombination

**Part of the following topical collections:**

## Abstract

Erlang renewal models, also called chi-squared models, provide a tractable model for genetic recombination that exhibits positive interference. Closed form expressions for multilocus probabilities are derived for the crossover process when it is a renewal process with the distance between crossovers modeled by a Erlang distribution. These expressions yield explicit formulas for the map functions, coincidence functions and distributions of the identity-by-descent process, giving exact results for a class of models that better model observed biological data.

## Keywords

Erlang renewal processes Genetic recombination Multilocus probabilities Crossover interference Generalized hyperbolic functions Alternating renewal processes## Mathematics Subject Classification (2000)

60C05 60E15 92D10## Introduction

*n*+1 markers \({\mathcal {M}}_{1},\ldots,{\mathcal {M}}_{n+1}\) along a chromosome. For each of the inter-marker intervals, let

*i*

_{1},…,

*i*

_{ n }) of 0’s and 1’s is called a recombination pattern and the multilocus probabilities are:

These multilocus probabilities depend on inter-marker distances *d* _{1},…,*d* _{ n }, where *d* _{ j }= distance between markers \(\mathcal {M}_{j}\) and \(\mathcal {M}_{j+1}\). (Throughout this paper, distances will be expressed in Morgans, e.g. genetic units, not physical units.) Just as important, the multilocus probabilities depend on the model used to describe the way crossovers occur. The standard model is a Poisson process which is used because it was a reasonable first approximation and it is mathematically tractable. Its use in genetics was introduced by Haldane (1919), who knew it assumes no crossover interference.

It is widely accepted that there is positive crossover interference - a crossover at a point apparently inhibits crossovers at nearby points, see Kwiatkowski et al. (1993), Harushima et al. (1998), and Broman and Weber (2000). Various models have been proposed to represent that interference. A map function is a relation *r*=*r*(*d*) that expresses the recombination fraction *r* between two locations on a chromosome to the genetic distance *d* between them. Several authors have attempted to express multilocus probabilities in terms of map functions, e. g. Geiringer (1944); Karlin and Liberman (1994, 1979); Liberman and Karlin (1984); Risch and Lange (1983); Schnell (1961); Weeks et al. (1993). However, as Zhao and Speed (1996) point out, such efforts cannot accurately describe general multilocus probabilities because different models can yield the same map function. The root of the problem is that a map function can only describe what happens among loci and a multilocus probability requires more information. The “adjacent interval” coincidence coefficient (Muller (1916); Sturtevant (1915)) provides some information, and the “nonadjacent interval” coincidence coefficient of Foss et al. (1993) appears to provide more, but neither can fully characterize interference in general. The approach here is to specify a model for recombination and derive multilocus probabilities directly from that model. Expressions for map functions and coincidence functions follow from the multilocus probabilities.

The main results of this paper are closed form expressions for multilocus probabilities when the inter-event distribution is Erlang. These results in Section 2 are based on Zhao et al. (1995), where infinite series expressions for multilocus probabilities are given for the chiasma model on the four strand bundle. We show that the (infinite series) matrix functions they consider can also be used to specify the multilocus probabilities for the crossover process as well, and we give closed form expressions for both the crossover process and the four strand chiasma process. The next section derives closed form expressions for map functions and coincidence functions for Erlang models of recombination, filling in some gaps in the work of Cobbs (1978) and Foss et al. (1993). The description of the identity by descent process and the effect on genome wide thresholds are contained in the following section. Section 5 reviews our findings and makes some general comments about the plausibility of renewal models for recombination.

Since we hope that these results will be used by geneticists, we have attempted to make them more accessible by stating them without the standard lemma/theorem format and separating the proofs to Section 6. The interesting mathematical ideas are that one can explicitly write down the finite dimensional distributions of a counting renewal process with Erlang inter-arrival distances. The crossover process is a then an alternating renewal process that toggles between two states (recombination/no recombination), and its finite dimensional distributions are given in closed form. The result is a new class of probability distributions that are based on a novel use of generalized hyperbolic functions. These results can be used in other applications where a system alternates between an on-state and an off-state; some examples are mentioned at the end of the last section.

## Erlang renewal models

Renewal process models for genetic recombination have a long history in genetics, see Bailey (1961); Cobbs (1978); Fisher et al. (1947); Lange (1997); Owen (1949) and Stam (1979). In these models, the distance between crossovers is modeled by a random variable with some distribution. Once a crossover has occurred, the distance until the next crossover is an independent random variable with the same distribution. The choice of that distribution completely determines the properties of the crossover process, and hence the multilocus probabilities (Section 1). The mathematical complexity of these models comes from the fact that, except when an exponential distribution is used, the process is non-Markov.

*m*, a positive integer, and a scale parameter

*λ*>0, with density

*f*(

*x*)=

*λ*

^{ m }

*x*

^{ m−1}

*e*

^{−λ x }/(

*m*−1)!,

*x*>0, see Fig. 2. The name chi-squared model is used by the above paper, by Zhao et al. (1995), and by Armstrong et al. (2006), though they always assume an even number of degrees of freedom. Since it is essential that the shape parameter is an integer for the work below and Erlang laws have a long history in queueing theory, it seems appropriate to call these Erlang models. Erlang distributions include the exponential distribution as a special case (

*m*=1), and are in turn a subclass of the gamma distributions (as are the chi-squared distributions).

For our purposes it is convenient to parameterize the Erlang distributions in the form Erlang(*m*,*λ* *m*), where *m* is a positive integer and *λ* is a positive number. In Lin and Speed (1996) and Zhao et al. (1995), values of *m*=4 for Drosophila, *m*=2 for Neurospora, and *m*=3 for humans give the best fit. (For notational simplicity, our *m* is their *m*+1; in the notation of Foss, et al. (1993), we are using a *Cx*(*Co*)^{ m−1} model). Figure 2 of Harushima, et al. (1998) shows a plot of distances between 555 recombinations for a rice data set. It is poorly described by the Haldane model (*m*=1), but well described by an Erlang distribution with *m*=2. Likewise Figure 2 of Broman and Weber (2000) shows clear evidence of positive interference, with close recombinations visibly depleted. Broman et al. (2002) discusses the fit to mouse data.

The main point of biological interest in using an Erlang distribution is that as *m* increases, it is less likely to see two crossovers close to each other. The distance to the next crossover gets more concentrated around the mean, which has the same value, 1/*λ*, for all Erlang(*m*,*λ* *m*) distributions. There is an opposing shift in the probabilities for large distances, but that doesn’t appear to be significant until the genetic length of a chromosome exceeds 2/*λ* Morgans.

### 2.1 The crossover process

The renewal crossover process is a model for recombination in diploid individuals that involves two strands - maternal and paternal haploids. Crossovers occur between these two strands according to a renewal process, leading to the exchange of genetic material. These models do not appear to take into account the fact that diploid meiosis involves four strands. Lemma 2 shows that a chiasma model for all four strands is equivalent to a crossover model with a different inter-event distribution. In particular, Eq. (9) below gives an formula for the inter-event distribution for a crossover model that yields the same multilocus probabilities as the Erlang chiasma model considered below.

*m*,

*λ*

*m*) inter-event distribution is given by:

**1**=(1,…,1) is a row vector of

*m*1’s, and the

*m*×

*m*matrix functions \(M_{0}^{cross}(u)\) and \(M_{1}^{cross}(u)\) are given by

*generalized hyperbolic functions*

*f*

_{ r,q }are given by

where *q* is a positive integer, *r*=0,…,*q*−1, *a* _{ j }=*a* _{ j }(*q*)= cos(2*π* *j*/*q*) and *b* _{ j }=*b* _{ j }(*q*)= sin(2*π* *j*/*q*).

These matrices are given in Bailey (1961, pg. 203), in infinite series form. The derivation is given in Section 6, where a transition matrix interpretation is given for the above matrices. Note that when *m*=1, (2) simplifies to the Haldane no interference model.

### 2.2 The chiasma process

In the biological process of meiosis in diploid organisms, each haploid replicates itself, and a four stranded bundle is formed. In a renewal chiasma process, crossovers occur among these four strands according to a renewal process, and the bundle pulls apart to form four gametes. The crucial difference between this model and the crossover process is that a crossover among sister chromatids does not result in a genetically observable exchange of material, although it does interfere with the location of nearby chiasma. Karlin and Libermann (1984) and Speed (1999) discuss a mathematical model for this, based on work of Mather (1936, 1937) and others. This approach allows one to model more concretely what goes on in the biological process of recombination. First we will focus on a multilocus probabilities for a single gamete produced by an individual; then tetrad multilocus probabilities will be derived. In what follows, we assume no chromatid interference (NCI), that is, which chromatids crossover at a given point are not dependent on which chromatids crossover at other points.

*m*,

*λ*

*m*), then with the NCI model, there are an average of

*λ*/2 genetically observable crossovers in a distance of one Morgan. Hence to keep this model comparable to the crossover process, which has an average of

*λ*crossovers per Morgan, an Erlang(

*m*,2

*λ*

*m*) inter-event distribution should be used. For a gamete formed by a renewal chiasma process with Erlang(

*m*,2

*λ*

*m*) inter-event distribution, the multilocus probabilities are given by

*m*×

*m*matrix functions

*D*

_{ ∞ }and

*D*

_{0}are

The matrices \(M_{0}^{NCI}\) and \(M_{1}^{NCI}\) are called *N* and *R* respectively in Zhao et al. (1995), where they are given as infinite series. Lin and Speed (1996) have implemented a numerical approximation to these matrices.

in Section 6. Graphs of this distribution are shown in the bottom plot of Fig. 2.

### 2.3 The tetrad case

^{ n }recombination patterns for

*n*+1 markers, each represented by a pattern (

*i*

_{1},…,

*i*

_{ n }), where

*i*

_{ j }∈{0,1,2}. The same notation can be used as before, with the multilocus probabilities for tetrads, assuming NCI, given by

*h*

_{ r,m },

*r*=0,1,…,2

*m*−1 are given by

*α*=(1/2)

^{1/m },

*aj*′=

*a*

_{ j }(2

*m*)= cos(

*π*

*j*/

*m*),

*bj*′=

*b*

_{ j }(2

*m*)= sin(

*π*

*j*/

*m*) and

The matrices \(M_{0}^{tetrad}\), \(M_{1}^{tetrad}\) and \(M_{2}^{tetrad}\) correspond to the matrices *P*, *T* and *N* respectively in Zhao et al. (1995).

## Map functions and coincidence functions

*d*is the genetic distance between two loci, then for a crossover renewal process with Erlang(

*m*,

*λ*

*m*) inter-event distribution, the recombination fraction between them is

*m*,2

*λ*

*m*) inter-event distribution, the recombination fraction is,

where the last equality uses (15) in Section 6. This last result is Eq. (30) of Cobbs (1978), and Eq. (7) of Foss et al. (1993).

*m*. As expected, the functions start from the no interference model (Haldane distance,

*m*=1) and get closer and closer to the complete interference model

*θ*=

*d*. Note that recombination fractions for the crossover models exceed the level

*r*=1/2 when

*m*>1. In fact, for the crossover model, the recombination fraction oscillates around 1/2 as

*d*→

*∞*. In contrast, under the chiasma model with NCI, Mather’s formula shows that the recombination fraction cannot exceed 1/2. In our case, this follows from (11) because the sum in the last term is always less than

*e*

^{2λ md }, and thus the term in parentheses is less than 1. While not shown here, the graphs of the other commonly used map functions (Kosambi, Binomial with

*N*=2, Sturt with any

*L*>0.79) generally lie between the crossover

*m*=1 and the crossover

*m*=2 curves shown. (One can get above the

*m*=2 curve by taking

*L*small enough in the Sturt map function, or by making

*N*large enough in Binomial map function.) Furthermore both recombination fractions are approximately linear for small distances. This is because (13) shows

*f*

_{ r,q }(

*u*)=

*u*

^{ r }/

*r*!+

*o*(

*u*

^{ r }) as

*u*→0 and therefore the dominant terms in \(r_{m}^{cross}(\cdot)\) and \(r_{m}^{NCI}(\cdot)\) are of order

*λ*

*d*+

*o*(

*d*) as

*d*→0.

*p*(1,∗)=

*p*(1,0)+

*p*(1,1), etc. The classical “adjacent interval” coincidence coefficient is defined by taking three markers, separated by inter-marker distances

*d*

_{1}and

*d*

_{2}:

*d*

_{1},

*d*

_{2}and

*d*

_{3}:

*S*

_{3}and

*S*

_{4}of Foss et al. (1993) are given by

*S*

_{3}can be computed using the formulas for map functions above. For

*S*

_{4}, Section 6 shows that

## Identity-by-descent process

*X*(

*t*) is a model for these shared segments. For simplicity, consider two half-sibs and compare the chromosomes that they inherited from their common parent. Let

*t*denote position along the chromosome and define

The places where *X*(*t*) changes value are precisely the points where a crossover has occurred.

Note that this equality always holds, regardless of what model is used (crossover, chiasma, NCI or chromatid interference, etc.). The awkward looking absolute value signs are explained by the fact that |*i* _{ j+1}−*i* _{ j }|=1 or 0, depending on whether or not a recombination has or has not occurred in the *j* ^{ th } interval.

### 4.1 Thresholds for dense markers

Lander and Kruglyak (1995) used the no interference model to derive appropriate thresholds for an infinitely dense scan of the genome. We show that the thresholds don’t change when the Erlang renewal processes described above are used instead of the Haldane model.

where *r*(*d*) is the recombination fraction. Given a sample of *n* relative pairs, sum over all pairs and normalize to get \(Z(t)=2 \sqrt {n}\sum \left (X_{j}(t)-{1 \over 2}\right)\). When *n* is large, this is approximately a (stationary) Gaussian process. When *X* is based on the no interference model, the large sample limit is an Ornstein-Uhlenbeck process; but when *m*>1 the crossover and chiasma models considered above do not have an Ornstein-Uhlenbeck process as the limit.

*Z*(

*t*),

*Z*(

*t*+

*d*))→1 as

*d*→0. Using (12),

As we noted above, all Erlang renewal processes have *r*(*d*)=*λ* *d*+*o*(*d*) (for any *m*) as *d*→0, so Cov(*Z*(*t*),*Z*(*t*+*d*))=1−2*λ* *d*+*o*(*d*) as *d*→0. In fact, any plausible model of recombination will have the map function approximately linear near the origin, so it will yield the same thresholds as the no interference model for a dense map.

When a finite set of markers are used, there is a change in the threshold. The reason is that with positive interference, nearby markers are less dependent, and the multiple comparison problem is heightened. Quantifying this difference precisely depends on being able to accurately compute cumulative probabilities for multivariate normal distributions with dependence given by (12).

## Discussion

We have used Erlang renewal processes to model both the crossover process and the chiasma process with NCI. Closed form expressions are given for multilocus probabilities in both cases, completing the work of Bailey (1961); Cobbs (1978); Owen (1949); Stam (1979) and Zhao et al. (1995). These formulas lead to expressions for map functions, coincidence functions, IBD probabilities as well as closed form expressions for tetrad multilocus probabilities.

The fact that crossover models with *m*>1 yield recombination fractions above 1/2 may be desirable in certain cases. This apparently can happen in prokaryotes, so these models may be directly applicable there. In fact, the observance of recombination fractions above 1/2 in mouse data, e.g. Falconer (1947) and Wright (1947), was seen as a deficiency of the Haldane, Kosambi, etc. map functions. The second cited source is a careful study involving 453 offspring in a balanced block design. Convinced that *r*>1/2 was possible, Bailey (1961); Fisher et al. (1947) and Owen (1949) specifically tried to develop models that had this property. We do not know whether such fractions have been seen in other data sets or whether other factors, e.g. differential viability of the organisms, may have caused the observed values of *r*>1/2 in those older studies.

There is a mathematical explanation for *r*>1/2 in terms of the underlying renewal process. When *m*>1, the Erlang densities are concentrated around the mean of 1/*λ*, which means a recombination is most likely to occur approximately 1/*λ* Morgans away from the first crossover. Equivalently, for the associated IBD process, (12) shows that the covariance becomes negative when *r*>1/2, so that the process is most likely to be in opposite states at that distance. This is not restricted to Erlang models; any renewal process model for the crossover process whose inter-event distribution has a strong enough peak will have *r*>1/2.

Crossover models are all that are strictly necessary in mammalian genetics (excluding oocyte mapping), because we only observe the single gamete that was used at conception. For example, the renewal chiasma model with NCI described above is a crossover process with inter-event distribution given by (9). In general, any chiasma renewal process is equivalent to a crossover renewal process with inter-event distribution that is a geometric mixture of the chiasma inter-event distribution.

It is an open question whether or not a renewal process is an appropriate model for recombination. First we address some technical issues, then make a general comment.

One criticism of renewal processes is that they are not generally “multilocus feasible” in the sense of Liberman and Karlin (1984). On this issue, we agree with Speed (1999), where it is pointed out that Liberman and Karlin define what might be called “nonadjacent interval multilocus feasibility”. While mathematically elegant, their definition puts conditions on recombinations in intervals separated by an arbitrary distance, which does not agree with the basic intuition of interference being a local phenomenon. Zhao and Speed (1996) show that most of the common map functions can arise from renewal processes, even though some are not “nonadjacent interval multilocus feasible.”

Another criticism of the use of renewal processes is that multiple chiasma apparently can occur simultaneously, making a serial renewal process inappropriate. As Bailey (1961, pg. 178) points out, we do not necessarily need a serial explanation for using Erlang inter-event distributions - they may just describe what’s going on in the spatial point process (ignoring the temporal dimension). Molecular interactions may act spatially, not temporarly, inhibiting nearby crossovers. The counting model of Foss et al. (foss1) assumes intermediates (C’s) being distributed according to a Poisson point process, and then some of these convert to crossovers. They focus on a fixed number (*m*−1 in our notation) of non-crossover events (*Co*’s) between crossovers (*Cx*’s), but also mention a variable number of *Co*’s. Lange et al. (1997) and Lange (1997) analyze this “random-skip” process and give infinite series for multilocus probabilities and derived quantities for that model.

In the end, experimentation will have to resolve whether Erlang (or any) renewal process realistically models recombination. A more relevant question is whether these models, which incorporate positive interference, do a better job than the commonly used Haldane model. The results of Foss et al. (1993), e. g. Figure 4, Copenhaver et al. (2002); Housworth and Stahl (2003) and McPeek and Speed (1995), indicate that that they do. A maximum likelihood fit to Figure 2 of Harushima et al. (1998) shows that an Erlang distribution with *m*=2,*λ*=1/2 fits rice data well. Better models for recombination, even if not exactly correct, may help detect disease or trait loci and build genetic maps.

## Mathematical proofs

The key idea in what follows is the observation that *N*(*t*)=*d*⌊*N* ^{∗}(*t*)/*m*⌋= the integer part of *N* ^{∗}(*t*)/*m*, i. e. the Erlang renewal process *N*(*t*) increases by 1 every time *m* events have occurred for the Poisson process *N* ^{∗}(*t*). The Markov nature of *N* ^{∗}(*t*) then allows an analysis of *N*(*t*). The phrase “ *N*(*t*) is in phase *i*” will be used as shorthand for *N* ^{∗}(*t*)=*i* (mod *m*). In the terminology of Foss, et al. (1993), this means that *i* *Co* events have occurred since the last *Cx* event. Another key idea is that *X*(*t*)=*dN*(*t*) (mod 2), i.e. the alternating renewal process switches state every time *N*(*t*) increases.

*D*

_{0}(

*u*) was defined in (8) (the zeros below the main diagonal correct a misprint there). For

*k*=1,2,3,…, define the sequence of

*m*×

*m*matrix functions

*D*

_{ k }(

*u*) with (

*i,j*)

^{ th }entry

*e*

^{−u }

*u*

^{ mk+j−i }/(

*mk*+

*j*−

*i*)!. The

*D*

_{ k }(·) matrices have an interpretation as transition matrices: for

*k*>0, the (

*i,j*)

^{ th }entry of

*D*

_{ k }(

*u*) is

*D*

_{0}. If

**p**

_{0}is the distribution of the phase of

*N*(0), then

**p**

_{0}

*D*

_{ k }(

*u*) is the distribution of the phase of

*N*(

*u*) given that

*k*renewal events occurred in [0,

*u*]. In particular, for an Erlang renewal process with

*N*(0) having initial distribution

**p**

_{0},

This gives a closed form expression for the finite dimensional distributions of a counting process with Erlang inter-arrival distances. The memoryless property of *N* ^{∗}(*t*) is what makes the multiplication of matrices give the correct probabilities for *N*(*t*). The choice **p** _{0}=(1/*m*)**1**=(1/*m*,…,1/*m*) used in the formulas for multilocus probabilities represents the equiprobable initial distribution for the phase of *N*(0) in the stationary case.

*M*

_{0}takes into account all possibilities with an even number of crossovers, whereas

*M*

_{1}takes into account all possibilities with an odd number of crossovers. Like the

*D*

_{ k }matrices above, the entries of these matrices have a transition matrix interpretation. For example, the

*i,j*

^{ th }entry of

*M*

_{0}(

*u*) is the probability of starting in phase

*i*, having an even number of crossovers in distance u, and ending in phase

*j*.

*D*

_{ k }, some algebra shows that

*M*

_{0}and

*M*

_{1}have the form claimed in (3) and (4) respectively, where

A closed form expression for these follows from the next lemma.

### *Proof*

*f*

_{ r,q }with respect to

*uq*times shows that \(f_{r,q}^{(q)}(u)= f_{r,q}(u)\). The initial conditions for this

*q*

^{ th }order differential equation are \(g^{(i)}_{r,q}(0)=1\) if

*i*=

*r*; and =0 otherwise. After solving this equation, we discovered that these differential equations are known in the mathematical literature. The solutions are

*ω*= exp(2

*π*

*i*/

*q*) is a

*q*

^{ th }root of unity. This is given in Erdélyi et al. (1955, pg. 212), where

*f*

_{ r,q }are called generalized hyperbolic functions of order

*q*. A survey of these functions is given in Muldoon and Ungar (1996). To eliminate the complex terms in this expression, set

*Δ*=2

*π*/

*q*, then the constants from (5) are

*a*

_{ j }= cos(

*j*

*Δ*) and

*b*

_{ j }= sin(

*j*

*Δ*). Since

*ω*= exp(

*i*

*Δ*),

*ω*

^{ j }=

*a*

_{ j }+

*ib*

_{ j }and

It remains to be shown that the imaginary term above is zero. When *q* is odd, say *q*=2*m*+1, then the *j*=0 term is zero because *b* _{0}=0. For *j*=1,…,*m*, *a* _{ q−j }=*a* _{ j }, *b* _{ q−j }=−*b* _{ j }, and sin(*b* _{ q−j } *u*−*r*(*q*−*j*)*Δ*)= sin(−*b* _{ j } *u*−2*π* *r*+*rj* *Δ*)=− sin(*b* _{ j } *u*−*rj* *Δ*). Hence the imaginary term is zero. When *q* is even, say *q*=2*m*, then the *j*=0 and *j*=*m* terms in the sum are zero, and the *j* ^{ th } and (*q*−*j*)^{ th } terms will cancel as above. □

*r*=0,1,…,

*q*−1, all powers appear in the series, leading to

We next consider the chiasma process on the four strand bundle. Theorem 1 of Zhao et al. (1995) gives an infinite series expression for (1) for the single gamete case: \(M_{i}^{NCI} = (1-i) D_{0} + (1/2) \sum _{k=1}^{\infty } D_{k}=(1/2)\left (\sum _{k=0}^{\infty } D_{k} + (-1)^{i+1} D_{0}\right)\). Straightforward algebra shows that \(D_{\infty }(u) = \sum _{k=0}^{\infty } D_{k}(u)\) has the form claimed in (7).

Next the derivation of (9) is given. A *p*-thinning of a point process is when successive points are retained with probability *p* or eliminated with probability 1−*p*, with independent decisions being made at each point. The effective inter-arrival distribution when an Erlang point process is thinned is given in the following lemma. As mentioned above, the chiasma model is obtained by a (1/2)-thinning of a crossover model with rate *μ*=2*λ* *m*, which yields (9).

### **Lemma 2**

*p*-thinning of an Erlang(

*m*,

*μ*) point process is a point process with inter-arrival density

### *Proof*

*q*=1−

*p*and

*Δ*=

*μ*

*q*

^{1/m }, then the density is

where the last equality uses (13). □

The derivation of multilocus probabilities in the tetrad case requires a more involved argument.

### **Lemma 3**

The matrices \(M_{0}^{tetrad}\), \(M_{1}^{tetrad}\) and \(M_{2}^{tetrad}\) are given by (10).

### *Proof*

*M*

_{0},

*M*

_{1}and

*M*

_{2}:

*M*

_{0}=

*D*

_{0}+

*M*

_{2}and since \(p_{0}^{(k)} + p_{1}^{(k)} + p_{2}^{(k)}=1\), \(M_{0}+M_{1}+M_{2} = D_{0} + D_{1} + \sum _{k=2}^{\infty } \left [ p_{0}^{(k)} + p_{1}^{(k)} + p_{2}^{(k)} \right ] D_{k} = D_{\infty }.\) Therefore

*M*

_{0}+

*M*

_{1}+

*M*

_{2}=(

*M*

_{2}+

*D*

_{0})+

*M*

_{1}+

*M*

_{2}=

*D*

_{ ∞ }, so \(M_{2}= {1 \over 2} [ D_{\infty } - D_{0} -M_{1}]\) and \(M_{0}= {1 \over 2} \left [ D_{\infty } + D_{0} -M_{1}\right ]\).

*M*

_{1}has form (10). Noting that \(p_{1}^{(1)}=1\) is consistent with the definition of \(p_{1}^{(k)}\), we have \(M_{1} = \sum _{k=1}^{\infty } p_{1}^{(k)} D_{k}\) has the claimed form, where \(h_{r,m}(u) = \sum _{k=1}^{\infty } p_{1}^{(k)} u^{mk+r}/(mk+r)!\),

*r*=0,…,2

*m*−1. Differentiating

*h*

_{ r,m }2

*m*times gives

*h*

_{ r,m }satisfies the (2

*m*)

^{ th }order differential equation

*j*=

*m*+

*r*and =0 otherwise. The general solution to these equations is

*ω*=

*ω*(2

*m*)= exp(

*i*

*π*/

*m*): the summation gives the solution of the homogeneous equation and the remaining terms give a particular solution. Laborious calculations with the initial conditions show that

*γ*

_{ j,r,m }=

*c*

_{ j,r,m }

*ω*

^{−jr }. More algebra shows that the above simplifies to (10). □

Next we derive formulas for the coincidence function *S* _{4}. For the crossover process, \(S_{4}^{cross}(d)=(1/m) {\mathbf {v}} (M_{0}^{cross}(\lambda d) +M_{1}^{cross}(\lambda d)) {\mathbf {v}}^{T}\), where \({\mathbf {v}} = {\mathbf {1}} ({\lim }_{d \downarrow 0} M_{1}(\lambda d)/ r^{cross}(d))\). Now *r*(*d*)=*λ* *d*+*o*(*d*) and *f* _{ r,q }(*λ* *d*)=(*λ* *d*)^{ r }+*o*(*d* ^{ r }) as *r* *↓*0, so the limiting matrix of *M* _{1}(*λ* *d*)/*r*(*d*) is all zero, except for the lower left element which is the constant *m*. Hence **v**=(0,…,0,*m*), with only one non-zero entry. Now \((M_{0}^{cross}(\lambda d) +M_{1}^{cross}(\lambda d))\) has (*m,m*)^{ th } entry *f* _{ m−1,2m }(*λ* *d*)+*f* _{2m+1,2m }(*λ* *d*)=*f* _{ m−1,m }(*λ* *d*), where the last identity is obtained by adding two series of form (13). Hence \(S_{4}^{cross}(d)=(1/m) m^{2} \exp (- \lambda d) f_{m-1,m}(\lambda d)\).

The argument is similar for the NCI chiasma model: \(S_{4}^{NCI}(d)=(1/m) {\mathbf {v}} \linebreak (M_{0}^{NCI}(2 \lambda d) +M_{1}^{NCI}(2\lambda d)) {\mathbf {v}}^{T} = (1/m) {\mathbf {v}} D_{\infty }(2 \lambda d) {\mathbf {v}}^{T}\), where **v** is the same as above. The (*m,m*)^{ th } entry of *D* _{ ∞ } is exp(−2*λ* *d*) *f* _{ m−1,m }(2*λ* *d*), giving the formula for \(S_{4}^{NCI}\).

*D*

_{ ∞ }(

*u*) is called the 1-hyperbolic matrix in Muldoon and Ungar (1996). It is a circulant matrix, is related the fast Fourier transform, always has determinant 1, and

*D*

_{ ∞ }(

*u*)

*D*

_{ ∞ }(

*v*)=

*D*

_{ ∞ }(

*u*+

*v*). The matrices \(M_{0}^{cross}(u)\) and \(M_{1}^{cross}(u)\) are blocks of

*D*

_{ ∞ }(

*u*;2

*m*), i.e.

This structure may be useful in compressing formulas or speeding up computations of multilocus probabilities.

The computational effort needed to evaluate Erlang multilocus probabilities need not be an obstacle to using them in a genetic linkage study. One can precompute many of the terms needed in the formulas and the remaining computations are small compared to the total computation time used in linkage programs.

In mathematical terms, the crossover process is an alternating renewal process, with state alternating between 0 and 1 and the multilocus probabilities are essentially the finite dimensional distributions of the process. While we focused on the genetic application of these results, the results may be of interest in other fields, e.g. telecommunication networks and queues, where they can be used to model the busy/non-busy state of a system with buffers. They may describe busy or non-busy status in a queueing system that buffers exponential arrivals. Examples include a shuttle bus that waits for *m* passengers before leaving, a computer system that buffers *m* bytes before initiating an input or output operation, and communication networks that relay packets through *m* nodes.

When *m*=1, i.e. the inter-event distances are exponential, the alternating renewal process is called a random telegraph process and is used in the study of defects in semiconductors, see Simoen and Claeys (2016). Using *m*>1 gives a generalized random telegraph process; such processes may be useful in semiconductor models.

R programs for computations of map distances, multilocus probabilities and coincidence functions for Erlang renewal models are available from the author.

## Notes

### Acknowledgements

The author would like to thank Soumitra Ghosh for discussions on the genetics in this paper, Richard Holzsager for discussions on the mathematics in this paper, and the anonymous referees whose suggestions improved the paper.

### Competing interests

The author declares that he has no competing interests.

### Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

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