A theoretical foundation for state-transition cohort models in health decision analysis

Abstract

Following its introduction over three decades ago, the cohort model has been used extensively to model population trajectories over time in decision-analytic modeling studies. However, the stochastic process underlying cohort models has not been properly described. In this study, we explicate the stochastic process underlying a cohort model, by carefully formulating the dynamics of populations across health states and assigning probability rules on these dynamics. From this formulation, we explicate a mathematical representation of the system, which is given by the master equation. We solve the master equation by using the probability generation function method to obtain the explicit form of the probability of observing a particular realization of the system at an arbitrary time. The resulting generating function is used to derive the analytical expressions for calculating the mean and the variance of the process. Secondly, we represent the cohort model by a difference equation for the number of individuals across all states. From the difference equation, a continuous-time cohort model is recovered and takes the form of an ordinary differential equation. To show the equivalence between the derived stochastic process and the cohort model, we conduct a numerical exercise. We demonstrate that the population trajectories generated from the formulas match those from the cohort model simulation. In summary, the commonly-used cohort model represent the average of a continuous-time stochastic process on a multidimensional integer lattice governed by a master equation. Knowledge of the stochastic process underlying a cohort model provides a theoretical foundation for the modeling method.

Introduction

Decision models have been used in various applications from clinical decision making to screening guideline development. The objective of decision modeling is to integrate and present evidence within a coherent and explicit mathematical structure that can be used to link evidence to decision-relevant outcomes. In decision modeling, a state-transition Markov model is often used to simulate the prognosis of a patient or a group of patients following an intervention. Beck and Pauker [1] introduced the modeling method over 30 years ago with the aim to provide a simple tool for prognostic modeling and for practical use in medical decision making. They applied standard methods from Markov chain theory [2, 3] to simulate a life history of an individual which is structured as transitions across various heath states over time, i.e. a stochastic process on a finite state space ($\mathbb{S}$). However, the current literature in decision modeling lacks clarity in the following two concepts. First, a cohort model, an extension of the state-transition model from one individual to a group of individuals, is often used to introduce and describe a stochastic process on $\mathbb{S}$. According to [1] and the subsequent published tutorials and textbook [4–7], given a matrix of transition probabilities and an initial distribution of counts of individuals across health states, a cohort model generates the life trajectory of a cohort of identical individuals by repeated multiplications of the vector of population counts by the transition probability matrix. This matrix operation alludes to a stochastic process on a much larger state space, i.e. ${\mathbb{N}}^{\left|\mathbb{S}\right|}$ (compared to $\mathbb{S}$), where $\mathbb{N}$ and $\left|\mathbb{S}\right|$ denote the set of natural numbers and the number of states, respectively. For example, $\mathbb{S}$ may be a partitioning on an individual’s health state into healthy, sick, or dead. In contrast, ${\mathbb{N}}^{\left|\mathbb{S}\right|}$ may refer to a partitioning of a cohort of individuals into the numbers of healthy, sick and, dead individuals. The convolution of these two different processes in decision modeling literature lead to the second issue: practitioners are taught that cohort models capture the average behavior of the individuals. [7, 8] However, this claim is often stated without any clear reference to which stochastic process. Frederix et. al. [9] proposes an ordinary differential equation (ODE)-based method to approximate Markov models whilst acknowledging that the ODEs can describe only “the typical (mean) change,” albeit, without providing any rational or reference. One of the standard textbooks [7] describes cohort model as a representation of the average experience of patients in the cohort without providing a rationale to support this description. Furthermore, wide acceptance of methodologies does not automatically imply veracity. [10] In the context of cohort models, the wide acceptance is ingrained by the ISPOR-SMDM Modeling Good Research Practices Task Force-3. [11] The published best practices cites the work of Beck et al. [1, 4] as the main and only references for cohort models, thereby standardizing cohort models as the recommended method for simulating population trajectories despite of the lack of a proper description of the theoretical support in the decision modeling area.

This paper aims to address the aforementioned problems by placing cohort models in a larger framework based on existing literature on stochastic process. Therefore, in this paper, we explicate the stochastic process underlying a cohort model and derive its corresponding probability function from which the prevailing notion of an average is based on. For this paper, we adopt a continuous-time perspective, i.e. for a discrete-time process, a corresponding continuous-time process exists (embeddability assumption). In addition, we assume that transition rates are time-invariant and the process of interest is Markovian, i.e. knowledge of the current state conveys all information that is relevant to forecasting future states. This paper is organized into four main parts. Firstly, we review the prevailing descriptions of cohort model in decision modeling literature and formulate their mathematical representations to substantiate our claim of lack of clarity in the current description of a cohort model. Secondly, we postulate a precise description of the cohort dynamics and the probability rules on these dynamics to derive the underlying stochastic process. Thirdly, we solve for the probability function associated with the stochastic process by method of evolution equation. To show that the derived stochastic process corresponds to a cohort model, we also derive the mathematical formulas for the average and the variance of the process. Fourthly, the correspondence is then demonstrated by showing the equivalence between the first two moments of the process and the cohort model via a numerical example. Throughout this exposition, we try to strike a balance between mathematical rigor and accessibility to practitioners.

Methods

Prevailing views of the cohort model

Beck and Pauker [1] introduced a discrete-time Markov model as a method for representing a patient’s prognosis which can be viewed as a sequence of states of health in discrete time steps. We distinguish between three prevalent descriptions of a Markov model [4, 5, 7, 8] in current literature and practice: (1) a model for an individual or a Markov chain on $\mathbb{S}$, (2) a cohort simulation or a process on ${\mathbb{R}}^{\left|\mathbb{S}\right|}$, and (3) the continuous-time analogue of a cohort model from which the ODE-based method [9] arises.

Markov chain on $\mathbb{S}$

A discrete-time Markov chain on a finite set of mutually exclusive and completely exhaustive states: $\mathbb{S}=\{S_1,S_2,\dots ,S_s\}$, is a stochastic process, {S(n)} = {S(t_n)} where $\left|\mathbb{S}\right|=s$, $S\left(n\right)\in \mathbb{S}$, t_n = t₀ + nτ, t₀ is the initial time, τ is the Markov cycle and n ∈ {0, 1, …, N}, given an s × s stochastic matrix of transition probabilities governing the transitions among states, P_τ(t) = (p_ij(t))_1≤i,j≤s, and a 1 × s vector of initial probability distribution p(t₀) = [1 0 … 0 0] if, without loss of generality, we assume an individual start in S₁. Each p_ij(t, τ) has the usual interpretation of the probability of an individual transitioning from S_i to S_j in τ at time t. In principle, to calculate the distribution of states in the next cycle, p(t + τ), we post-multiply the distribution in the current cycle, p(t), with P_τ(t):

$$\begin{array}{c}\hfill \mathbf{p}(t+\tau )=\mathbf{p}\left(t\right){\mathbf{P}}_{\tau }\left(t\right)\end{array}$$ (1)

Cohort simulation

An s-state cohort simulation [1, 7] is a recursive algebraic calculation that generates a trajectory of population counts (state-configuration):

$$\begin{array}{c}\hfill \mathbf{N}\left(t\right)=[N_1\left(t\right)N_2\left(t\right)\dots N_s\left(t\right)],\end{array}$$ (2)

where $\mathbf{N}\left(t\right)\in {\mathbb{R}}^s$ denotes the number of individuals in state S_i at time t ≥ t₀, given P_τ(t) as defined above, and an initial distribution N(t₀) = [n₀ 0 … 0 0]. In principle, to calculate the distribution of individuals across all states at time t + τ, N(t + τ), the state-configuration at time t, N(t), is projected forward in time using the linear operator P_τ(t):

$$\begin{array}{c}\hfill \mathbf{N}(t+\tau )=\mathbf{N}\left(t\right){\mathbf{P}}_{\tau }\left(t\right)\end{array}$$ (3)

Eq 3 indicates that: first, a cohort simulation is not a stochastic process; secondly, the relevant state space is different compared to a Markov chain model for an individual, $\mathbb{S}$ vs. ${\mathbb{R}}^s$; and, the integrality constaint is relaxed from ${\mathbb{N}}^s$ to ${\mathbb{R}}^s$.

Continuous-time ODE-equivalence

The recursive formula (Eq 3) can be written as a difference equation and if we take the limit of this difference equation with respect to the Markov cycle, we obtain the differential form of a cohort model:

$$\begin{array}{cc}\hfill \underset{\tau \to 0^{+}}{lim}\frac{\mathbf{N}(t+\tau )-\mathbf{N}\left(t\right)}{\tau }& =\underset{\tau \to 0^{+}}{lim}\mathbf{N}\left(t\right)\frac{{\mathbf{P}}_{\tau }\left(t\right)-\mathbf{I}}{\tau }\hfill \\ \hfill \frac{d}{dt}\mathbf{N}\left(\mathbf{t}\right)& =\mathbf{N}\left(\mathbf{t}\right)\mathbf{Q},\hfill \end{array}$$ (4)

where Q is the infinitesimal generator matrix of size s × s, $\mathbf{Q}={\left({\widehat{c}}_{kl}\right)}_{1\le i,j\le s}$, for the continuous-time stochastic process underlying a cohort model. The off-diagonal elements of Q are non-negative while the diagonal elements are non-positive, ${\widehat{c}}_{ii}=-{\displaystyle \sum _{j=1,j\ne i}^s}{\widehat{c}}_{ij}$. If ${lim}_{\tau \to 0}\frac{{\mathbf{P}}_{\tau }\left(t\right)-\mathbf{I}}{\tau }=\mathbf{Q}$ [12, 13], then the continuous-time version of a cohort model is a deterministic process (cf. Eq 3) governed by an ordinary differential equation (ODE) or, alternatively, a rate equation for the state-configuration. As in a cohort simulation, the ODE (Eq 4) operates on a different state space, i.e. ${\mathbb{R}}^s$, and does not represent an individual process.

Reformulation of cohort model

Formulation strategy

In the context of decision modeling, the typical system of interest is exemplified by the health state of an individual following the implementation of an intervention and the changes in the health state during a time period, often a lifetime. The representation is dynamic in the sense that the states and parameters of the system are functions of time. The formulation of a dynamic process underlying the changes in an individual’s health state starts by observing the state of the world at, at least two different time points, e.g., at t and t + τ. The difference between the two observations are then identified and the events, that contributed to these differences in health state and are most consistent with the prevailing evidence and theories, are postulated. After identifying all possible events, an individual’s health state is then represented by enumerating the possible health states, i.e. a partitioning on the world via $\mathbb{S}$. The dynamics of the system is consequently determined by the identified events and operationalized by assigning the allowable transitions to all pairs of states in $\mathbb{S}$ that are consistent with theories and data. The aforementioned formulation of a process for an individual, which follows Beck and Pauker [1], is then extended to a cohort of individuals, i.e. a process on ${\mathbb{N}}^s$. In this expanded state space, the dynamic system of interest is the changes in state-configuration, which is represented by Eq 2. The transition from one state-configuration to another represents not only a change in health state of one individual, which follows the rules on $\mathbb{S}$ but also a change in the number of individuals of the two corresponding states.

Given the state space and the transition rules, we then specify the nature of the transitions, i.e. stochastic or deterministic changes. The choice of a stochastic (vs. deterministic) representation of the transition is natural because the applications of decision modeling often involves a disease progression component which is an inherently random system, i.e. can be described up to a certain degree of confidence. In contrast to a deterministic model, in which given an initial condition, the sequence of the states of the world can be determined with a probability of one, the solution to a stochastic model can be represented by a multidimensional probability function at any t following the initial time t₀. Therefore, the state of the system at any given time can only be described with a probabilistic statement, i.e., the probability of observing a particular state-configuration, $\mathbf{N}\left(t\right)=\mathbf{n}\in {\mathbb{Z}}^s$ at time t or P(N(t) = n) = P(n, t).

Master equation

Given the formulation strategy, we formalize the description of the process in this section. An event of transitioning from S_k to S_l is denoted by the transition R_kl where k, l ∈ {1…, s}. Since the occurrence of each transition alters the state-configuration, each R_kl is associated with a vector representing this change, s_kl, and is defined as s_kl = e_l − e_k where e_i is the i-th column of an identity matrix of size s. We associate each transition with a propensity function: ν_kl(n, t) = c_kl(t)h(n_k, n_l), where c_kl(t) is the transition rate for transition R_kl, and N_k(t) = n_k and N_l(t) = n_l. The function h(n_k, n_l) determines the number of ways R_kl can occur which is equal to the number of individuals in S_k, h_kl(n_k, n_l) = n_k. The propensity function denotes the probability of a (any) transition occurring in continuous time as a function of the state-configuration and rate constant. The probability of observing one particular transition R_kl in a small time interval τ is assumed to be linear in time: c_kl(t)τ + o(τ), where o(τ) represents other terms that decay to zero faster than τ. Therefore, the probability of a transition from S_k to S_l in time step τ is given by n_kc_kl(t)τ + o(τ) (see S1 Appendix). A transition R_k,l occurring with a probability ν_kl(n, t)τ in a time step τ alters the current state N(t) = n to:

$$\begin{array}{c}\hfill \mathbf{N}(t+\tau )=\mathbf{n}+s_{kl}\end{array}$$

Following the mathematical descriptions of the possible changes in the state-configuration and the probabilities of these changes, we derive the evolution equation for P(n, t), i.e., master equation (also known as the forward Kolmogorov equation), which describes how P(n, t) changes in continuous time. The master equation is obtained by enumerating all possible events contributing to a change in the probability of observing a particular state-configuration in an infinitesimal time step and is given by (see S1 Appendix):

$$\begin{array}{c}\hfill \frac{dP(\mathbf{n},t)}{dt}=\sum _{k=1}^s\sum _{l=1,l\ne k}^s({\nu }_{kl}(\mathbf{n}-s_{kl},t)P(\mathbf{n}-s_{kl},t)-{\nu }_{kl}(\mathbf{n},t)P(\mathbf{n},t))\end{array}$$ (5)

The terms, ν_kl(n, t)P(n, t), represent the probability transferred from one to another state-configuration resulting from the transition R_kl. (probability flux). In principle, a master equation expresses the change per unit of time of the probability of observing a state-configuration n as the sum of two opposite effects: the probability flux into and out of n. Therefore, a master equation is essentially a rate equation for the probability of observing a state-configuration (c.f. Eq 4). The solution to the master equation, P(n, t), contains all information about the modeled system and can be, under some conditions on c_kl(t) obtained by applying the generating function technique (see S1 Appendix). A probability generating function (PGF) of P(n, t) is defined by:

$$\begin{array}{c}\hfill G(\mathbf{x},t)=\sum _{\mathbf{n}}{x}_1^{n_1}{x}_2^{n_2}\dots x_s^{n_s}P(\mathbf{n},t)\end{array}$$ (6)

The explicit solution to the Eq 6 is obtained by solving a first-order linear partial differential equation (PDE) for G(x, t). [14] We solve for the PGF under two initial conditions: (1) an arbitrary initial distribution and (2) all individuals start in S₁. From the solution to the PDE, we recover P(n, t) by using the definition of PGF and obtain the first two moments of the process, i.e., the mean and the variance from the first derivative of G(x, t) (see S1 Appendix).

Results

Solution to master equation

The solution to the master equation, the probability function of a state-configuration n at time t, for an arbitrary initial state-configuration P(n, 0) is given by: where z_i = [z_i1 z_i2 … z_is] where i ∈ {1, 2, …, s}, B(t) = exp At, i.e. the matrix exponential and A is an s × s matrix, (c_kl)_{k,l∈{1,2,…,s}}, with elements of the form: a_kl = c_kl − γ_kδ_kl with ${\gamma }_k={\sum }_{l=1}^s{c}_{kl}$ and δ_kl is the Kronecker delta (δ_kl = 1 if k = l and is 0 otherwise). Matrix A is identical to matrix Q in Eq 4, the generator matrix for the continuous-time ODE-equivalence of a cohort model. For the case where all n₀ individuals start in S₁ (N₁(0) = n₀), the probability function of a state-configuration n at time t is represented by:

$$\begin{array}{c}\hfill P(\mathbf{n},t)=n_0!\prod _{m=1}^s\frac{B_{1m}{\left(t\right)}^{n_m}}{n_m!}\end{array}$$ (7)

The mean of the number of individuals in the i-th state at time t is given by:

$$\begin{array}{c}\hfill E\left[N_i\left(t\right)\right]={\varphi }_i\left(t\right)=n_0{B}_{1i}\left(t\right)\end{array}$$ (8)

The variance of the number of individuals is the i-th state at time t is given by:

$$\begin{array}{c}\hfill V_i\left(t\right)=n_0{B}_{1i}\left(t\right)(1-B_{1i}\left(t\right))\end{array}$$ (9)

For an arbitrary initial distribution, the mean of the number of individuals in state S_i is given by:

$$\begin{array}{c}\hfill {\varphi }_i^a\left(t\right)=\sum _{\mathbf{n}}\sum _{k=1}^s{n}_k{B}_{ki}\left(t\right)P(\mathbf{n},t),\end{array}$$ (10)

and the variance is given by:

$$\begin{array}{c}\hfill V_i^a\left(t\right)=\sum _{\mathbf{n}}\left[\sum _{k=1}^s{n}_k{B}_{ki}\left(t\right)\right((n_k-1)B_{ki}\left(t\right)+\sum _{l=1,l\ne k}^s{n}_l{B}_{li}\left(t\right)+1\left)\right]P(\mathbf{n},t)+{\varphi }_i^a{\left(t\right)}^2\end{array}$$ (11)

Numerical verification

We conduct a numerical exercise to verify the validity of the derived stochastic process. In particular, we aim to verify the formulas for the mean (Eq 8) and the variance (Eq 9). For this verification exercise, we consider a stochastic process with s = 4, i.e. $\mathbb{S}=\{S_1,S_2,S_3,S_4\}$ (Fig 1), rate constants (elements of Q): c₁₂ = 0.05, c₁₃ = 0.01, c₁₄ = 0.001, c₂₃ = 0.1, c₂₄ = 0.05, and c₃₄ = 2, and an initial condition in which all individuals start in S₁, i.e. N₁(0) = 10000. As a set of benchmarks for the mean, we simulate the population trajectories, i.e. the counts of individuals in all states, (1) using a cohort model with τ = 1-year (Eq 3) and (2) a continuous-time cohort model (Eq 4). The benchmark for variance is based on 1000 Monte Carlo samples of microsimulation population with τ = 1-year. Each microsimulation population is conceived as a realization of 10000 Markov chains with the generator matrix Q (as in Eq 4). The calculation of the 1-year transition probability matrix from the Q matrix is based on the formulas from Welton and Ades. [15] The results of the population trajectories are given in Fig 2. We observe no difference between the empirical estimates from the microsimulation and the analytic formulas for both the mean and the variance of the process associated with the cohort model. The code for the numerical exercise is available under a GNU GPL license and can be found at https://github.com/rowaniskandar/CM_ME_plosone.

Fig 1. A 4-states continuous-time stochastic process used in numerical verification exercise.

Fig 2. Population trajectories across 4 states.

[CM: Cohort model, MSM: Microsimulation, ODE: Continuous-time cohort model, PGF: Master equation, sd: Standard deviation]. Note: plots are on top of each other.

Discussion

In this study, we explicate the stochastic process underlying the commonly used cohort model, defined as a continuous-time discrete-state stochastic process, in the context where population counts are of interest. First, We start the derivation by specifying a stochastic state-transition model for an individual following Beck and Pauker: a stochastic process on state space $\mathbb{S}$. [1] We then extend the model to a cohort of individuals by formulating a set of postulates for the cohort dynamics: a stochastic process on ${\mathbb{N}}^{\left|\mathbb{S}\right|}$. The evolution equation representing the stochastic process for the cohort dynamics in the form of master equation is then obtained. We then solve the master equation to get the probability function of individuals across all states, which completely characterizes stochastic nature of the dynamics, by using the generating function method. Based on the explicit form of the generating function, the analytical formulas for the average and variance are obtained. This measure of variance quantifies the inherent variability of the population trajectories (aleatory uncertainty [16] or first-order uncertainty [17]) and may be useful for quantifying the extent of variability in the mean prediction. In our simulation example, we show that to estimate the variance of the population counts across states, we need to replicate the microsimulation population a number of times in addition to the individual Monte Carlo runs within each population, which is a potentially computationally intensive task and is similar to applying uncertainty analysis to a microsimulation model. [18] In particular, if some of the events in the model are rare and/or the expected differences in the effect sizes among strategies are small, we expect the required number of Monte Carlo runs to be high. Our theoretical result provides a more direct and non-computationally demanding approach through the explicit formula for the variance. The derived probability function, when all individuals start in one state (a typical scenario in most applications) takes the form of a multinomial distribution and is a known result from the stochastic compartmental model literature [19]. In applications where the relevant population comprises of an actual cohort (e.g. birth cohorts), the individuals are often, prior to an implementation of an intervention, distributed across health states. For this purpose, we also derive the probability function and formulas for the moments, for an arbitrary initial condition. Lastly, we show the equivalence between the average of the derived stochastic process and the cohort model; thereby substantiating the prevailing notion of cohorts models as average process.

In the introduction to cohort models [1] for use in decision modeling, the authors emphasized the clinical utility of a Markov process (as opposed to a decision tree model) for modeling patient’s prognosis with ongoing risks: a model for an inherently stochastic system. A stochastic representation of a system amounts to making probabilistic statements about its state given a set of probabilistic rules for the system dynamics. Therefore, the solution to any stochastic processes or models takes the form of a probability function on a set of random variables [2], i.e., in our context, P(n, t), which is the solution to the master equation. However, in their expositions, population counts were used as a representation of the stochastic system via a cohort simulation. The multiplication of the transition probabilities (used in individual process) with the cohort size (Eq 3) produces a deterministic quantity, i.e. the average of the process, not a probabilistic statement about the process. The commonly used representation of a cohort model via cohort simulation in decision modeling literature convolutes two distinct processes: a process on $\mathbb{S}$ and a Markov chain on ${\mathbb{N}}^s$. The notion of the average as represented by cohort simulation is based on the latter. To date, our work is the only study that delineates the convolution of these two different processes which has been perpetuated by tutorials and textbooks in decision modeling [7, 20].

Having an explicit form of the evolution equation for P(n, t) is advantageous for, in some cases (e.g. time-invariant rates), finding the analytical form of P(n, t) and, in most cases (e.g. time-varying rates), deriving the mean and the variance of the process by using their evolution equations and without knowing the explicit form of P(n, t). In addition, given this knowledge of evolution equation associated with a cohort model, we can identify the relationship between cohort models and other known methodologies in stochastic process. In the classification tree of Markov processes [21], a cohort model as represented by the master equation is derived from the differential Chapman-Kolmogorov equation without the drift and diffusion coefficients. If the cohort size is sufficiently large, a cohort model can be approximated by the van Kampen’s expansion method [22], which is analytically more tractable compared to master equation. In addition, if we relaxed the integrality constraint on the state space to allow for nonnegative real numbers, a cohort model may be represented by a Fokker-Planck or a stochastic differential equation. [21, 23] Therefore, our study results provide practitioners and researchers the proper platform for the porting of methods from stochastic process literature for applications in decision modeling.

Knowledge of the underlying process will provide a proper context for efforts to resolve or clarify methodological challenges or issues, for example, in estimating the appropriate time step for cohort models. [24, 25] Practitioners of cohort models are taught to add an additional half-year of lives at the end of the cohort simulation to account for the fact that individuals transition at the end of each time step. This half-cycle correction is a consequence of discretizing a continuous-time scale. However, the refinement of half-cycle correction method was based on the average process [26], i.e. not taking into account the variance of the process or other higher-order moments. Naimark et al. [26] proposed several methods, including numerical integration techniques to determine the appropriate time step to bypass the need of half-cycle correction. Elbasha and Chhatwal [27] quantified the approximation errors from using these numerical integration methods in the context of a 3-states cohort model. However, these numerical approximation methods were applied to the “state membership function,” which is essentially the average number of individuals: an approximation of an approximation. This study result can facilitate a more accurate approximation, which would be based on directly using the master equation, i.e. based on how a change in the time step affects the probability function.

One limitation of the study concerns the focus on cohort models with time-invariant rates. In most applications, the transition probabilities are often time-dependent (e.g. age-specific probability of death due to other causes). A direct consequence of assuming non-constant rates is that the solution to a master equation becomes mathematically intractable and henceforth inaccessible to most practitioners. However, various numerical and approximation methods for solving master equations are available as a corollary of knowing the proper placement of cohort models in the classification tree of stochastic processes, as described above. For example, Gillespie’s stochastic simulation [28] and tau-leap methods [29] numerically solve a master equation by simulating all possible events one-at-a-time or in batches, respectively. Despite of this limitation, our analytical results remain applicable in many situations since no restriction is placed on the number of states and the allowable transition patterns on the set of states. In addition, the analytical results for an arbitrary initial condition can be utilized to approximate a process with time-varying rates by using a piecewise process. Each piece or time interval corresponds to a time-invariant process. The initial condition of the next time interval would be the distribution of individuals at the end of the previous interval. We plan to introduce this piecewise method in a future study.

This paper also assumes that the discrete-time transition probability matrix is embeddable to a continuous-time model, i.e. the limit of P exists and its equal to the generator matrix of the process (Eq 4). Although discrete-time Markov models have been the method of choice in many applications in decision modeling, the processes under consideration, e.g. biological process or disease progression, evolve continuously; henceforth the appropriate modeling framework would be a continuous-time model [30]. In addition, the reason for the greater popularity of the discrete-time structure stems from its simpler mathematical nature, not from considerations of veracity. [31] However, in some instances, one can argue that an individual-level model tend to follow a discrete-time process, e.g. the transitions among living arrangements for an elderly patient occur in discrete time steps. However, if we consider a cohort of individuals, the probability of a patient transitioning in a small time interval would very likely to be nonzero. Nevertheless, we believe that future studies investigating whether the typical Markov models in decision modeling are embeddable are warranted.

Conclusion

Many decisions in health are often made with incomplete understanding of the underlying phenomena. In such cases, stochastic models can serve as powerful tools for aiding decision-makers in synthesizing evidence from different sources, estimating decision-relevant outcomes, and quantifying the impact of uncertainty on decision-making. In particular, the cohort model provides an easy-to-implement method for modeling recurrent events over time and has been used extensively in many applications ranging from clinical decision making to policy evaluations. A cohort model represents the average of a stochastic process which is presented by a master equation. The derived stochastic process rectifies and unifies the prevailing descriptions of cohort models in the literature and practice. Knowledge of the underlying theoretical framework would reaffirm the prevailing beliefs in the veracity and validity of the method and thereby increase confidence in conclusions derived from studies using cohort models. Future studies should focus on increasing the flexibility of cohort models and decreasing computational time by leveraging the relationship between the derived process and other stochastic processes.

Supporting information

S1 Appendix. Mathematical derivations.

(PDF)

Data Availability

All relevant data are within the paper and its Supporting Information files.

Funding Statement

The author received no specific funding for this work.