 Methodology article
 Open Access
 Published:
Bayesian inference of biochemical kinetic parameters using the linear noise approximation
BMC Bioinformatics volume 10, Article number: 343 (2009)
Abstract
Background
Fluorescent and luminescent gene reporters allow us to dynamically quantify changes in molecular species concentration over time on the single cell level. The mathematical modeling of their interaction through multivariate dynamical models requires the deveopment of effective statistical methods to calibrate such models against available data. Given the prevalence of stochasticity and noise in biochemical systems inference for stochastic models is of special interest. In this paper we present a simple and computationally efficient algorithm for the estimation of biochemical kinetic parameters from gene reporter data.
Results
We use the linear noise approximation to model biochemical reactions through a stochastic dynamic model which essentially approximates a diffusion model by an ordinary differential equation model with an appropriately defined noise process. An explicit formula for the likelihood function can be derived allowing for computationally efficient parameter estimation. The proposed algorithm is embedded in a Bayesian framework and inference is performed using Markov chain Monte Carlo.
Conclusion
The major advantage of the method is that in contrast to the more established diffusion approximation based methods the computationally costly methods of data augmentation are not necessary. Our approach also allows for unobserved variables and measurement error. The application of the method to both simulated and experimental data shows that the proposed methodology provides a useful alternative to diffusion approximation based methods.
Background
The estimation of parameters in biokinetic models from experimental data is an important problem in Systems Biology. In general the aim is to calibrate the model so as to reproduce experimental results in the best possible way. The solution of this task plays a key role in interpreting experimental data in the context of dynamic mathematical models and hence in understanding the dynamics and control of complex intracellular chemical networks and the construction of synthetic regulatory circuits [1]. Among biochemical kinetic systems, the dynamics of gene expression and of gene regulatory networks are of particular interest. Recent developments of fluorescent microscopy allow us to quantify changes in protein concentration over time in single cells (e.g. [2, 3]) even with single molecule precision (see [4] for review). Therefore an abundance of data is becoming available to estimate parameters of mathematical models in many important cellular systems.
Single cell imaging techniques have revealed the stochastic nature of biochemical reactions (see [5] for review) that most often occur far from thermodynamic equilibrium [6] and may involve small copy numbers of reacting macromolecules [7]. This inherent stochasticity implies that the dynamic behaviour of one cell is not exactly reproducible and that there exists stochastic heterogeneity between cells. The disparate biological systems, experimental designs and data types impose conditions on the statistical methods that should be used for inference [8–10]. From the modeling point of view the current common consensus is that the most exact stochastic description of the biochemical kinetic system is provided by the chemical master equation (CME) [11]. Unfortunately, for many tasks such as inference the CME is not a convenient mathematical tool and hence various types of approximations have been developed. The three most commonly used approximations are [12]:

1.
The macroscopic rate equation (MRE) approach which describes the thermodynamic limit of the system with ordinary differential equations and does not take into account random fluctuations due to the stochasticity of the reactions.

2.
The diffusion approximation (DA) which provides stochastic differential equation (SDE) models where the stochastic perturbation is introduced by a state dependant Gaussian noise.

3.
The linear noise approximation (LNA) which can be seen as a combination because it incorporates the deterministic MRE as a model of the macroscopic system and the SDEs to approximatively describe the fluctuations around the deterministic state.
Statistical methods based on the MRE have been most widely studied [8, 13–15]. They require data based on large populations. The main advantages of this method are its conceptual simplicity and the existence of extensive theory for differential equations. However, single cells experiments and studies of noise in small regulatory networks created the need for statistical tools that are capable to extract information from fluctuations in molecular species. Few methods used CME to address this. Algorithm, proposed by [16], approximated the likelihood function, the other, suggested by [17] simulated it using Monte Carlo methods. Recently, also a method based on the exact likelihood [18] has been developed. Although, substantial progress has been made in numerical methods for solving CME, inference algorithms based on the CME are computationally intensive and difficult to apply to problems of realistic size and complexity [19]. Another group of methods is based on the DA [9, 20]. This uses likelihood approximation methods (e.g. [21]) that are computationally intensive and require sampling from high dimensional posterior distributions. Inference about the volatility process becomes difficult for low frequency data that are not directly measured at the molecular level [10, 20]. The aim of this study is to investigate the use of the LNA as a method for inference about kinetic parameters of stochastic biochemical systems. We find that the LNA approximation provides an explicit Gaussian likelihood for models with hidden variables and measurement error and is therefore simpler to use and computationally efficient. To account for prior information on parameters our methodology is embedded in the Bayesian paradigm. The paper is structured as follows: We first provide a description of the LNA based modeling approach and then formulate the relevant statistical framework. We then study its applicability in four examples, based on both simulated and experimental data, that clarify principles of the method. Additional file 1 contains details of mathematical and statistical modeling, particularly comparison of the proposed method with an algorithm based on the DA.
Methods
The chemical master equation (CME) is the primary tool to model the stochastic behaviour of a reacting chemical system. It describes the evolution of the joint probability distribution of the number of different molecular species in a spatially homogeneous, well stirred and thermally equilibrated chemical system [11].
Even though these assumptions are not necessarily satisfied in living organisms the CME is commonly regarded as the most realistic model of biochemical reactions inside living cells. Consider a general system of N chemical species inside a volume Ω and let X = (X_{1},..., X_{ N })^{T}denote the number and x = X/Ω the concentrations of molecules. The stoichiometry matrix S = {S_{ ij }}_{i = 1,2...N; j = 1,2...R}describes changes in the population sizes due to R different chemical events, where each S_{ ij }describes the change in the number of molecules of type i from X_{ i }to X_{ i }+ S_{ ij }caused by an event of type j. The probability that an event of type j occurs in the time interval [t, t + dt) equals (x, Ω, t)Ωdt. The functions (x, Ω, t) are called mesoscopic transition rates. This specification leads to a Poisson birth and death process where the probability h(X, t) that the system is in the state X at time t is described by the CME [12] which is given in Additional file 1. It is straightforward to verify that the first order terms of a Taylor expansian of the CME in powers of are given by the following MRE
where ϕ_{ i }= lim_{Ω→∞, X→∞}X_{ i }/Ω, φ = (ϕ_{1},..., ϕ_{ N })^{T}and .
Including also the second order terms of this expansion produces the LNA
which decomposes the state of the system into a deterministic part φ as solution of the MRE in (1) and a stochastic process ξ described by an Itô diffusion equation
where W(t) denotes R dimensional Wiener process, and f_{ i }= f_{ i }(φ) (see Additional file 1 for derivation).
The rationale behind the expansion in terms of is that for constant average concentrations relative fluctuations will decrease with the inverse of the square root of volume [22]. Therefore the LNA is accurate when fluctuations are sufficiently small in relation to the mean (large Ω). Hence, the natural measure of adequacy of the LNA is the coefficient of variation i.e. ratio of the standard deviation to the mean (see Additional file 1). Validity of this approximation is also discussed in details in [22, 23]. In addition it can be shown that the process describing the deviation from the deterministic state converges weakly to the diffusion (3) as Ω → ∞ [24]. In order to use the LNA in a likelihood based inference method we need to derive transition densities of the process x.
Transition densities
The LNA provides solutions that are numerically or analytically tractable because the MRE in (1) can be solved numerically and the linear SDE in (3) for an initial condition ξ(t_{ i }) = has a solution of the form [25]
where the integral is in the Itô sense and (s) is the fundamental matrix of the nonautonomous system of ODEs
The Itô integral of a deterministic function is a Gaussian random variable [26], therefore equations (4), (5) imply that the transition densities of the process ξ are Gaussian [26] (throughout the paper we use 'Gaussian' or 'normal' shortly to denote either a univariate or a multivariate normal distribution depending on the context)
where Θ denotes a vector of all model parameters, ψ(·μ_{i1}, Ξ_{i1}) is the normal density with mean μ_{i1}and covariance matrix Ξ_{i1}specified by
It follows from (2) and (6) that the transition densities of x are normal
The properties of the normal distribution allow us to construct a convenient inference framework that is reminiscent of the Kalman filtering methodology (see e.g. [27]).
Inference
It is rarely possible to observe the time evolution of all molecular components participating in the system of interest [28]. Therefore, we partition the process x_{ t }into those components y_{ t }that are observed and those z_{ t }that are unobserved.
Let , and denote the timeseries that comprise the values of processes x, y and z, respectively, at times t_{0},..., t_{ n }. Here and throughout the paper we use the same letter to denote the stochastic process and its realization.
Our aim is to estimate the vector of unknown parameters Θ from a sequence of measurements . The initial condition φ(t_{0}) is parameterized as an element of Θ. Given the Markov property of the process x the augmented likelihood P(, Θ) is given by
where are Gaussian densities specified in (8), and is an initial density assumed to be normal for mathematical convenience. It can then be shown that (see Additional file 1) is Gaussian. Therefore
where φ(·φ(t_{0}),..., φ(t_{ n }), ) is Gaussian density with mean vector (φ(t_{0}),..., φ(t_{ n })) and covariance matrix whose elements can be calculated numerically in a straightforward way (see Additional file 1). Since the marginal distributions are also Gaussian it follows that the likelihood function P(Θ) can be obtained from the augmented likelihood (10)
where the covariance matrix Σ = {Σ^{(i, j)}}_{i, j = 0,..., n}is a submatrix of such that and φ_{ y }is the vector consisting of the observed components of φ.
Fluorescent reporter data are usually assumed to be proportional to the number of fluorescent molecules [29] and measurements are subject to measurement error, i.e. errors that do not influence the stochastic dynamics of the system. We therefore assume that instead of the matrix our data have the form . The parameter λ is a proportionality constant (it is straightforward to generalize for the case with different proportionality constants for different molecular components) and denotes a random vector for additive measurement error. For mathematical convenience we assume that the joint distribution of the measurement error is normal with mean 0 and known covariance matrix Σ_{ϵ}, i.e. . If measurement errors are independent with a constant variance then . Equation (11) implies that the likelihood function can be written as
Since for given data the likelihood function (12) can be numerically evaluated, any likelihood based inference is straightforward to implement. Using Bayes' theorem, the posterior distribution P(Θ) satisfies the relation [30]
We use the standard MetropolisHastings (MH) algorithm [30] to sample from the posterior distribution in (13).
Results and Discussion
In order to study the use of the LNA method for inference we have selected four examples which are related to commonly used quantitative experimental techniques such as measurements based on reporter gene constructs and reporter assays based on Polymerase Chain Reaction (e.g. RTPCR, QPCR). For expository reasons, all case studies consider a model of single gene expression.
Model of single gene expression
Although gene expression involves various biochemical reactions it is essentially modeled in terms of only three biochemical species (DNA, mRNA, protein) and four reaction channels (transcription, mRNA degradation, translation, protein degradation) [31–33]. The stoichiometry matrix has the form
where rows correspond to molecular species and columns to reaction channels. Let x = (r, p) denote concentrations of mRNA and protein, respectively. For the reaction rates
we can derive the following macroscopic rate equations
For the general case it is assumed that the transcription rate k_{ R }(t) is timedependent, reflecting changes in the regulatory environment of the gene such as the availability of transcription factors or chromatin structure.
Using (14), (15) and (16) in (3) we obtain the following SDEs describing the deviation from the macroscopic state (see section 3.1.4 of Additional file 1 for derivation)
We will refer to the model in (16) and (17) as the simple model of single gene expression.
In order to test our method on a nonlinear system we will also consider the case of an autoregulated network where the transcription rate of the gene is a function of the concentration of the protein that the gene codes for and where the protein is a transcription factor that inhibits the production of its own mRNA. This is parameterized by a Hill function [31] where k_{ R }(t) now describes the maximum rate of transcription, H is a dissociation constant and n_{ H }is a Hill coefficient.
Thus, the nonlinear autoregulatory model the system is described by the MRE
and the SDEs
where . We refer to this model as the autoregulatory model of single gene expression. The two models constitute the basis of our inference studies below.
Inference from fluorescent reporter gene data for the simple model of single gene expression
To test the algorithm we first use the simple model of single gene expression. We generate data according to the stoichiometry matrix (14) and rates (15) using Stochastic Simulation Algorithm (SSA) [34] and sample it at discrete time points. We then generate artificial data that are proportional to the simulated protein data with added normally distributed measurement error with known variance . Furthermore we assume that mRNA levels are unobserved. The volume of the system Ω is unknown and we put Ω = 1 so that concentration equals the number of molecules. Thus the data are of the form
where is the simulated protein concentration, λ is an unknown proportionality constant and is measurement error. For the purpose of our example we model the transcription function by
This form of transcription corresponds to an experiment, where transcription increases for t ≤ b_{3} as a result of being induced by an environmental stimulus and for t > b_{3} decreases towards a baseline level b_{4}.
We assume that at time t_{0} (t_{0} <<b_{3}) the system is in a stationary state. Therefore, the initial condition of the MRE is a function of unknown parameters (ϕ_{ R }(t_{0}), ϕ_{ P }(t_{0})) = (b_{4}/γ_{ R }, b_{4}k_{ P }/γ_{ R }γ_{ P }).
To ensure identifiability of all model parameters we assume that informative prior distributions for both degradation rates are available. Priors for all other parameters were specified to be noninformative. To infer the vector of unknown parameters
we sample from the posterior distribution
using the standard MH algorithm. The distribution P(Θ) is given by (12).
The protein level of the simulated trajectory is sampled every 15 minutes and a sample size of 101 points obtained. We perform inference for two simulated data sets: estimate 1 is based on a single trajectory while estimate 2 represents a larger data set using 20 sampled trajectories (see Figure 1A). All prior specifications, parameters used for the simulations and inference results are presented in Table 1A. Estimate 1 demonstrates that it is possible to infer all parameters from a single, short length time series with a realistically achievable time resolution. Estimate 2 shows that usage of the LNA does not seem to result in any significant bias. A bias has not been detected despite the very small number of mRNA molecules (5 to 35  Figure 2A in Additional file 1) and protein molecules (100 to 500  Figure 1A). The coefficient of variation varied between approximately 0.15 and 0.4 for both molecular species (Figure 1 in the Additional file 1).
Inference for this model required sampling from the 9 dimensional posterior distribution (number of unknown parameters). If instead one used a diffusion approximation based method it would be necessary to sample from a posterior distribution of much higher dimension (see Additional file 1). In addition, incorporation of the measurement error is straightforward here, whereas for other methods it involves a substantial computational cost [20].
Inference from fluorescent reporter gene data for the model of single gene expression with autoregulation
The following example considers the autoregulatory system with only a small number of reacting molecules. Using SSA we generated artificial data from the single gene expression model with autoregulation. The protein time courses were then sampled every 15 minutes at 101 discrete points per trajectory (see Figure 1B). As before we assume that the mRNA time courses are not observed and that the protein data are of the form given in (20), i.e. proportional to the actual amount of protein with additive Gaussian measurement error. As in the previous case study we estimate parameters from two simulated data sets, a single trajectory and an ensemble of 20 independent trajectories. The inference results summarized in Table 1B show that despite the low number of mRNA (015 molecules, see Figure 2 in Additional file 1) and protein (10250 molecules, see Figure B) all parameters can be estimated well with appropriate precision.
Inference for PCR based reporter data
In the case of reporter assays based on Polymerase Chain Reaction (e.g. RTPCR, QPCR) measurements are obtained from the extraction of the molecular contents from the inside of cells. Since the sample is sacrificed, the sequence of measurements are not strictly associated with a stochastic process describing the same evolving unit. Assume that at each time point t_{ i }(i = 0,..n) we observe l measurements that are proportional to the number of RNA molecules either from a single cell or from a population of s cells. This gives a (n + 1) × l matrix of data points
where is the actual RNA level, λ is the proportionality constant, is a Gaussian independent measurement error indexed by time t_{ i }. j = 1,..., l indexes the l measurements that are taken at time t_{ i }. Note that and are independent random variables as they refer to different cells. We assume that the dynamics of RNA is described by the simple model of single gene expression with LNA equations (16) and (17). Let ϒ_{ t }denote the distribution of measured RNA at time t (u_{ t }~ ϒ_{ t }). In order to accommodate for the different form of data we modify the estimation procedure as follows. For analytical convenience we assumed that the initial distribution is normal . This together with eq. (8) and normality of measurement error implies that . Simple explicit formulae for μ_{ t }and are derived in Additional file 1. Since all observations are independent we can write the posterior distribution as
where ψ(·, ) is the normal density with parameters , . In order to infer the vector of the unknown parameters Θ = (γ_{ R }, λ, b_{0}, b_{1}, b_{2}, b_{3}, b_{4}, , ) we sample from the posterior using a standard MH algorithm. To test the algorithm we have simulated a small (l = 10, n = 50, plotted in Figure 2) and a large (l = 100, n = 50) data set using SSA algorithm with parameter values given in Table 2. The data were sampled discretely every 30 minutes and a standard normal error was added. Initial conditions were sampled from the Poisson distribution with mean b_{4}/γ_{ R }. The estimation results in Table 2 show that parameters can be inferred well in both cases even though the number of RNA molecules in the generated data is very small (about 535 molecules). Since subsequent measurements do not belong to the same stochastic trajectory, estimation for the model presented here is not straightforward with the diffusion approximation based methods.
Estimation of gfp protein degradation rate from cycloheximide experiment
In this section the method is applied to experimental data. After a period of transcriptional induction, translation of gfp was blocked by the addition of cycloheximide (CHX). Details of the experiment are presented in Additional file 1. Fluorescence was imaged every 6 minutes for 12.5 h (see Figure 2). Since inhibition may not be fully efficient we assume that translation may be occurring at a (possibly small) positive rate k_{ P }. The model with the LNA is
The observed fluorescence is assumed to be proportional to the signal with proportionality constant λ. For comparison we also consider the diffusion approximation for which an exact transition density can be derived analytically (see Additional file 1 for derivation)
Since incorporation of measurement error for the diffusion approximation based model is not straightforward, we assume that measurements were taken without any error to ensure fair comparison between the two approaches. Table 3 shows that estimates obtained with both methods are not very different.
Conclusion
The aim of this paper is to suggest the LNA as a useful and novel approach to the inference of biochemical kinetics parameters. Its major advantage is that an explicit formula for the likelihood can be derived even for systems with unobserved variables and data with additional measurement error. In contrast to the more established diffusion approximation based methods [9, 20] the computationally costly methods of data augmentation to approximate transition densities and to integrate out unobserved model variables are not necessary. Furthermore, this method can also accommodate measurement error in a straightforward way.
The suggested procedure here is implemented in a Bayesian framework using MCMC simulation to generate posterior distributions. The LNA has previously been studied in the context of approximating Poisson birth and death processes [22–24, 35] and it was shown that for a large class of models the LNA provides an excellent approximation. Furthermore, in [35] it is shown that for the systems with linear reaction rates the first two moments of the transition densities resulting from the CME and the LNA are equal. Here we propose using the LNA directly for inference and provide evidence that the resulting method can give very good results even if the number of reacting molecules is very small. In our previous study [10] we have presented differences between fitting deterministic and stochastic models, where we used diffusion approximation based method. Our experience from that work and from study [20] is that implementation of diffusion approximation based methods is challenging especially for data that are sparsely sampled in time because the need for imputation of unobserved time points leads to a very high dimensionality of the posterior distribution. This usually results in highly autocorrelated traces affecting the speed of convergence of the Markov chain. Our method considerably reduces the dimension of the posterior distribution to the number of unknown parameters of a model only and is independent of the number of unobserved components (see Additional file 1). Nevertheless it can only be applied to the systems with sufficiently large volume, where fluctuations around a deterministic state are relatively close to the mean.
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Acknowledgements
This research was funded by BBSRC SABR grant BB/F005814/1 and EU BIOSIM Network Contract 005137. DAR is funded by EPSRC Senior Research Fellowship EP/C544587/1 and MK by studentship, Dept of Statistics, University of Warwick. CVH was funded by Wellcome Trust Programme Grant (067252, to JRED and MRHW) and now is recipient of The Prof. John Glover Memorial Postdoctoral Fellowship.
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MK proposed and implemented the algorithm. CVH performed the cycloheximide experiment. MK wrote the paper with assistance from BF and DAR, who supervised the study.
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Additional file 1: . Supplementary information contains derivation of the theoretical results, details about algorithm implementation and comparison with the inference method based on the diffusion approximation. (PDF 515 KB)
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Komorowski, M., Finkenstädt, B., Harper, C.V. et al. Bayesian inference of biochemical kinetic parameters using the linear noise approximation. BMC Bioinformatics 10, 343 (2009). https://doi.org/10.1186/1471210510343
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DOI: https://doi.org/10.1186/1471210510343
Keywords
 Posterior Distribution
 Transition Density
 Diffusion Approximation
 Stochastic Simulation Algorithm
 Ordinary Differential Equation Model