t@@ -65,7 +65,28 @@
(δ18Othreshold) is specified
with uniform probability across the linear
parameter interval. The user specifies the bounds
- of the model parameters, which define the model space.
+ of the model parameters.
+
+
+ Given a single value of model parameters
+ (εint, εgla,
+ tdegla,
+ δ18Othreshold), the TCN
+ concentration after the duration of e.g. the entire
+ Quaternary period in a sample can be computed. This
+ forward model describes a history of exhumation and
+ TCN production in a sample volume as it experiences the
+ variable physical environment of the Pleistocene.
+
+
+ When model parameters
+ (εint, εgla,
+ tdegla,
+ δ18Othreshold) are allowed to
+ vary within specified limits, they can be thought of as
+ orthogonal axes creating a coordinate system in higher-order
+ space. Every position in this model space is associated with
+ a certain set of model parameter values.
t@@ -73,13 +94,29 @@
- forward responses are computed based on an initial set of
- model parameters that is proposed using the
- Metropolis-Hastings technique. A burn-in phase of 1000
- iterations is first used to make a crude initial search of
- the model space. This step is followed by a more detailed
- and local search of the model space based on the best-fit
- model parameters from the burn-in phase.
+ A MCMC walker is a numerical entity which sequentially
+ explores the model parameter space in order to obtain the
+ best result between a forward-model and an observational
+ dataset. During each iteration
+ the walker takes its current position in model space, plugs
+ the parameter value into the forward-model, and
+ evaluates if the output result matches the observational
+ record better or worse than the output at its previous
+ position in model space. If the new results better matches
+ the observed dataset, it continues walking along the same
+ path in model space with a small random perturbation.
+
+
+
+ Starting at a random place inside the model space, a burn-in
+ phase of 1000 iterations is first used to make a crude
+ search of the entire model space.
+ The burn-in phase is followed by a similar but more detailed
+ and local search of the model space, based on the best-fit
+ model parameters from the burn-in phase. The weighted
+ least-squared misfit to observed TCN concentrations is used
+ to evaluate the likelyhood for the combinations of
+ model parameter values.
|