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The Role of Bifurcations in Parameter Estimation: A UQ Analysis of the Non-spatial Klausmeier Model

Lisa Beer, Christian Kuehn, Chiara Piazzola

arXiv:2609.18231v1math.DSmath.NA

TL;DR

The paper asks how parameter identifiability changes near bifurcations, where small parameter uncertainties can strongly alter model outputs. It applies UQ methods to a probabilistic non-spatial Klausmeier model and finds that bistability prevents reliable joint estimation, while transient data and Fisher-information heatmaps support inference and bifurcation detection.

  • Problem

    Near bifurcations, small parameter uncertainties can dramatically affect model outputs, making reliable parameter distributions important for meaningful predictions.

  • Method

    The study partitions the model’s parameter and initial-condition space into convergence regions and applies Sobol sensitivity analysis, Bayesian inversion, and Fisher information.

  • Results

    Reliable joint estimation of a and m is possible only in region one with transient data, while practical identifiability fails in other regions, especially under bistability.

  • Takeaways & Limitations

    Fisher-information heatmaps can reconstruct the bifurcation pattern, but comprehensive identifiability assessment requires combining multiple measures and using transient information.

  • Takeaways & Limitations

    The scalar trace of the Fisher information matrix can be misleading because it may hide weak information about one parameter.

Abstract

from arXiv · show

We employ uncertainty quantification methods to investigate how parameter identifiability changes in the vicinity of a bifurcation point. We perform numerical experiments on the non-spatial Klausmeier vegetation model with random coefficients, which describes biomass-water interactions and exhibits a fold bifurcation. We partition the domain around the bifurcation into regions with distinct convergence behaviors. In each region, we follow a UQ workflow that includes sensitivity analysis, Bayesian inference, and Fisher information evaluation to assess parameter identifiability. The results show that proximity to the bifurcation point is decisive for parameter estimation. Reliable joint inference of both model parameters is not possible when the system exhibits bistability. Furthermore, we can reconstruct the model's bifurcation pattern by Fisher information heatmaps, presenting a practical tool for bifurcation detection. Lastly, we highlight the importance of transient data for successful parameter estimation.

1 Introduction

The paper examines how proximity to bifurcations affects reliable parameter estimation, using uncertainty quantification on a probabilistic non-spatial Klausmeier model. It combines sensitivity analysis, Bayesian inference, and identifiability measures to extend prior work on inferability around bifurcations.

  • 1 Introduction: Parameter reliability is especially important near bifurcations because small parameter uncertainties can produce large changes in model outputs.Bifurcations arise when parameters cross critical thresholds and the system undergoes qualitatively different dynamics.
  • 1 Introduction: The study analyzes parameter-distribution quality as a function of distance from a fold bifurcation in a probabilistic non-spatial Klausmeier vegetation model.A fold bifurcation occurs when two equilibria collide and disappear.
  • 1 Introduction: The UQ workflow combines Sobol global sensitivity analysis, Gaussian approximations of Bayesian posteriors, parameter correlations, and Fisher information.These methods are used to assess the accuracy and identifiability of estimated parameter distributions.
  • 1 Introduction: The paper extends earlier non-probabilistic work on parameter inferability around bifurcations by applying a broader UQ methodology.The approach draws on a comprehensive UQ overview and adapts its tools to the bifurcation setting.
  • 1 Introduction: The paper proceeds from model and bifurcation analysis through numerical workflow and mathematical methodology to results and conclusions.Its sections introduce the model, experiments, analytical tools, findings, and final interpretation in that order.

2 The Klausmeier Vegetation Model

The Klausmeier model describes biomass–water interactions and is reduced here to an ODE system focused on desert and uniform-vegetation states. Its equilibria form a fold bifurcation at a = 2m, beyond which bistability occurs.

  • 2 The Klausmeier Vegetation Model: The Klausmeier model represents patterned vegetation and tracks biomass n together with downhill surface water w.The full model describes vegetation patterns in semiarid regions, including stripes that move uphill on slopes.
  • 2 The Klausmeier Vegetation Model: The model’s water input is a and plant mortality is m; vegetation uptake is represented by wn2, while −w denotes baseline water loss.These terms connect the model parameters and state variables to precipitation, mortality, uptake, and evaporation-like loss.
  • 2 The Klausmeier Vegetation Model: The study reduces the PDE model to an ODE system, excluding patterned states while retaining bifurcation structure in desert and uniform-vegetation regimes.This reduction focuses on convergence to plant-free or uniform vegetation states.
  • 2.1 Bifurcation Analysis: The system has a plant-free equilibrium and two additional equilibria that exist as distinct real solutions only when a > 2m.The equilibria are obtained by setting w′ = n′ = 0 and solving the resulting steady-state equations.
  • 2.1 Bifurcation Analysis: At a = 2m, two equilibria collide and disappear, defining a fold bifurcation; for a > 2m, one attracting and one repelling branch produce bistability.The bifurcation diagram uses m = 0.45 and varies a as the free bifurcation parameter, with stable and unstable branches shown separately.
  • 2.1 Bifurcation Analysis: The bifurcation diagram guides a partition of parameter and initial-condition space into regions with distinct convergence behaviors.This interpretation uses basins of attraction to determine which steady state simulations approach.

3 Applied Workflow

The workflow partitions parameter and initial-condition space around the bifurcation into regions with different attraction and convergence behaviors. It then combines sensitivity analysis, Bayesian inference, transient-data comparisons, and Fisher-information heatmaps to assess identifiability.

  • 3 Applied Workflow: The workflow divides the parameter and initial-condition space into four regions corresponding to distinct attraction and convergence behaviors.Regions one and four converge to the plant-free equilibrium, region three to the nontrivial equilibrium, and region two exhibits alternating convergence behavior.
  • 3 Applied Workflow: Sobol sensitivity analysis evaluates how parameter and initial-condition variations affect time-dependent output variance within each region.The analysis is intended to reveal which inputs are most influential and therefore more inferable from data.
  • 3 Applied Workflow: For each region, noisy trajectory data are generated and Bayesian inversion estimates the joint distribution of a and m using a Gaussian posterior centered at the MLE.The workflow evaluates local parameter inferability at representative parameter and initial-condition combinations.
  • 3 Applied Workflow: Two experiments compare parameter estimation with transient and steady-state observations against estimation without transient-phase data.This comparison directly assesses the contribution of transient information to parameter estimation.
  • 3 Applied Workflow: Fisher information is mapped over a grid of a and n0 values to create heatmaps describing parameter identifiability around the bifurcation.For each grid point, the workflow simulates noisy data, computes the MLE, and evaluates Fisher information.

4 Mathematical Tools

The paper combines global sensitivity analysis, Bayesian inversion, Gaussian posterior approximation, and Fisher information to assess parameter influence and identifiability from noisy dynamical-system data. These tools expose how parameter correlations, local likelihood geometry, and data limitations affect estimation quality.

  • Sensitivity analysis: Sobol indices quantify how parameter uncertainty contributes to model-output variability globally and over time, including each parameter’s interactions with the others.First-order indices measure the variance contribution from a parameter alone, whereas total indices include its interactions with all other parameters.
  • Inverse UQ: Bayesian inversion updates a prior parameter distribution with noisy observations to obtain a posterior describing which parameter values are most plausible.The likelihood measures agreement between model predictions and observations, while the maximum likelihood estimate gives the best parameter choice under the stated Gaussian-noise and uniform-prior setup.
  • Gaussian approximation: The posterior can be approximated locally by a Gaussian around the maximum likelihood estimate when the negative log-likelihood Hessian is invertible and sufficiently smooth.This approximation depends critically on the MLE and covariance matrix and may be inappropriate when the likelihood mode is ill-shaped.
  • Fisher information: Fisher information is the negative Hessian of the log-likelihood, and its inverse gives the covariance matrix of the Gaussian approximation.Its trace summarizes local likelihood curvature: high values indicate a peaked likelihood and more reliable estimates, whereas low values imply higher variance and possible loss of identifiability.
  • Identifiability: Strong parameter correlations stretch likelihood contours, make covariance matrices ill-conditioned, and prevent independent estimation of the parameters.Correlation analysis and Fisher information therefore provide complementary diagnostics of posterior quality.
  • Identifiability: Structural identifiability is necessary but not sufficient for successful estimation because noisy and limited data can undermine practical identifiability.The structural condition requires that identical outputs for all times imply identical parameters.

5 Numerical Experiments

The experiments show that parameter identifiability depends strongly on convergence region, transient information, and proximity to bistability or bifurcation structure. Joint estimation of a and m succeeds only in region one with transient data, whereas Fisher-information heatmaps reveal the bifurcation pattern but require complementary identifiability measures.

  • Sobol sensitivity analysis: Sensitivity analysis finds that a dominates steady-state sensitivity in region three, while interactions involving w0 and n0 remain important despite negligible first-order indices.In region one, transient interactions are prominent before sensitivities settle toward zero; initial conditions are therefore fixed in later experiments.
  • Sobol sensitivity analysis: Time-dependent Sobol indices converge after the system reaches steady state, making transient duration important for interpreting parameter sensitivity.The model converges to the plant-free equilibrium in regions one and four and to the non-trivial equilibrium in region three.
  • Parameter estimation: Steady-state-only observations preserve estimation quality for a but make simultaneous inference of m impossible, even in region one.Sobol analysis explains this result because sensitivity to m occurs primarily during the transient phase.
  • Fisher information: Fisher-information heatmaps reconstruct the bifurcation structure because parameters separating attraction regions produce highly sensitive likelihoods.However, reducing the Fisher information matrix to its trace can falsely suggest joint identifiability when one parameter contributes little information.
  • Parameter estimation: Joint estimation of a and m is reliable only in region one when transient data are available; strong correlations prevent practical identifiability elsewhere.The unsuccessful regions show nearly flat likelihood contours, highly correlated maximum-likelihood estimates, and inadequate Gaussian posterior approximations.
  • Discussion: Identifiability decreases in the bistable regime, even when regions share similar attraction behavior and Sobol sensitivity results.This indicates that parameter correlations can help identify multistability regions, but Fisher information alone is not sufficient.

6 Conclusion

The paper finds that parameter identifiability in the Klausmeier ODE depends strongly on location relative to the fold bifurcation and on transient data. It also reconstructs the bifurcation pattern with Fisher-information heatmaps, while noting that the model's simplicity limits direct generalization.

  • Parameter estimation depends heavily on parameter location and the availability of transient data.
  • Fisher-information heatmaps can reconstruct the model's bifurcation pattern.
  • Joint estimation of both parameters is not possible in the bistable regime after the bifurcation.The authors state that calibration would require historical data from a non-vegetated state.
  • The importance of transient and historical data underscores the need for long-term data collection in real-world applications.
  • The study uses a very simple Klausmeier model with only two compartments and two parameters, limiting its scope.The authors hope the insights transfer to more complex models with similar, though more complex, bifurcation behavior.

A.1 Klausmeier Model Stability Analysis

The appendix analyzes equilibrium stability through Jacobian eigenvalues. One equilibrium is unstable, while the stability of another depends on the sign of α and, for the stated application range, on the conditions m < 2 and a > 2m.

  • The stability analysis uses Jacobian eigenvalues: all negative real parts imply stability, whereas any positive real part implies instability.
  • The Jacobian analysis transforms the equilibrium conditions using m = w±n± before applying the eigenvalue sign criterion.
  • The equilibrium (w−, n−) is unstable regardless of α because β > 0 there.
  • The stability of (w+, n+) depends on the sign of α through the real parts of its eigenvalues.
  • For m < 2, the equilibrium is asymptotically stable when a > 2m.The case m ≥ 2 is omitted because real-world applications usually have mortality values below two.
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