11. Extending RISE through paradigms
This chapter describes how RISE separates what a model is from how it is solved, through the notion of a paradigm. A paradigm is a self-contained computational strategy – perturbation, recursive local linearization (RLL), \(k\)-th order Taylor projection (TP), occasionally-binding-constraint (occbin) piecewise linearization, and so on – that plugs into mainland RISE through a small, fixed interface. The aim is to add advanced solution methods without modifying RISE’s core and without paradigms interfering with one another.
This chapter is primarily for developers extending RISE. It first describes
what a paradigm is and the interface a paradigm must satisfy, and only then
gives the concrete paradigms that ship with RISE as worked examples. Three
paradigms are currently provided (each under paradigms/):
occbin – piecewise-linear, OccBin-style occasionally-binding constraints (
occbin.paradigm);recursive local linearization (RLL) (
rll.paradigm);\(k\)-th order Taylor projection (TP) (
rtp.paradigm).
Each is described in Examples, after the general interface.
11.1. Goals
The paradigm architecture is designed to deliver:
a clean separation between model structure and computational method;
support for multiple parameterizations of the same model;
extensibility to advanced methods without touching RISE core;
prevention of cross-talk between parameterizations;
strictly read-only access to RISE internals by paradigm code.
A model contains exactly one paradigm at a time, but may carry multiple parameter vectors, each producing its own solution object.
11.2. What a paradigm is
A paradigm \(\mathcal{P}\) is a computational universe that
solves a parameterized model \(m(\theta)\),
defines the internal representation of the solution \(S(\theta)\), and
provides operators acting on that solution (e.g. a one-step forecast).
It is not the model, not a parameter vector, and not a container for multiple solutions. Formally,
where \(S(\theta)\) is partly transparent to RISE (through the standard
envelope below) and partly opaque (through the S.solution payload).
11.3. Responsibilities of a paradigm
A paradigm must:
operate on a single parameter vector at a time;
return a single solution object
Sconforming to the standard envelope;provide operators derived from that solution;
remain unaware of parameter multiplicity;
treat the model object
Mas read-only – it may callregular_solver(M, ...)to obtain derivatives, but must never modifyMnor return a modifiedMto RISE;avoid modifying RISE core structures or global options.
A paradigm may use RISE’s baseline solver internally, use RISE’s
constraint enforcement, and keep mutable internal state inside
S.solution (see Mutable solution objects).
A paradigm must not store global state across parameterizations, return a
modified M, or manage arrays of solutions.
11.4. The standard solution envelope
Every paradigm’s solve_engine returns a struct S with the fields
below. This standard envelope lets RISE orchestrate the workflow
(convergence checking, re-solve decisions, filter routing) without knowing
anything about the paradigm’s internals.
Field |
Type |
Meaning |
|---|---|---|
|
|
|
|
|
|
|
|
|
|
matrix or |
measurement-error covariance for the Kalman filter; |
|
handle object |
opaque, paradigm-owned payload. RISE stores it but never inspects it. All paradigm-specific state lives here. |
The envelope is deliberately minimal. Fields specific to perturbation theory
(eigenvalues, number of solutions, Tz, …) are not required, because
they are meaningless or misleading for paradigms such as RLL and TP; those
paradigms keep such quantities inside S.solution.
A paradigm should start from a failed default and populate fields as each stage succeeds, so partial failures are reported correctly:
function S = make_envelope()
S.is_solved = [false, false];
S.warrant_resolving = true;
S.retcode = 1;
S.H = [];
S.solution = [];
end
11.5. The minimum interface contract
A paradigm exposes an engines struct with these fields.
- name (required)
A short string identifier, e.g.
'perturbation','rll','rtp'.- solve_engine (required)
S = solve_engine(M, regular_solver)
Mis read-only: the paradigm may callregular_solver(M, ...)internally, but the solved model is used internally only and never returned.Smust conform to the standard envelope, and no global or shared state may be modified.- one_step_engine (required)
one_step = one_step_engine(S)
The only input is
S– the modelMis not passed here, so everything the closure needs must have been captured inS.solutionduringsolve_engine. It returns a closure[x_t, retcode, extra...] = one_step(x_tm1, eps_t, regime)
with
x_tm1the lagged endogenous vector \(x_{t-1}\),eps_tthe shock vector \(\varepsilon_t\), andregimethe integer index of the current Markov regime. It returns a nonzeroretcodeif the step fails;extra...are optional outputs such as the local linear coefficients(k, H, G)consumed by the smoother.- filter_engine (optional)
Future extension for filtering / smoothing.
- use_rise_constraint_enforcer (optional)
Logical, default
true.
11.6. Mutable solution objects
For RLL and TP the effective policy function is state-dependent: it is
updated at each simulation step as the economy evolves. This conflicts with
RISE’s assumption that the stored solution S is static. The recommended
resolution is to implement S.solution as a MATLAB handle class.
Because handle objects are passed by reference, the one_step closure and
RISE’s stored copy of S.solution point to the same object: when
one_step updates it in place, RISE’s copy reflects the change
automatically, without RISE needing to know an update occurred.
classdef SolutionHandle < handle
properties
% paradigm-specific fields populated by solve_engine, e.g.
T % TP: current polynomial coefficients
k, H, G % RLL: current local linear policy
% ...
end
end
The workflow is:
solve_engineconstructs a freshSolutionHandle, populates it, and stores it asS.solution;one_step_engine(S)extractspayload = S.solutionand builds a closure capturingpayloadby reference;at each step the closure updates
payloadin place; RISE’s storedS.solutionreflects the updates automatically;RISE reads only the envelope fields and never the payload.
Note
Because RISE never reads S.solution directly, this pattern is safe. The
only contract is that one_step(x_tm1, eps_t, regime) always returns a
valid x_t and retcode, whatever the payload’s internal state.
11.7. Responsibilities of RISE
RISE manages model structure and parameter multiplicity; calls
solve_engine(M, regular_solver) for each \(\theta_i\) (passing M
read-only); stores each \(S_i\) in model.solution(i); and routes
simulation, forecasting and filtering through the closures returned by
one_step_engine (and filter_engine). The workflow is
RISE must not inspect or modify S.solution, assume any format inside
it, or reuse a one_step closure across different parameter vectors.
11.8. Isolation, safety and persistence
To prevent cross-talk between parameterizations, each call to
solve_engine must construct a fresh SolutionHandle (copying a
handle copies only the reference, not the data), no paradigm may keep
persistent state outside S.solution, and RISE must not reuse engines
across parameter vectors unless the paradigm is stateless.
For saving models to disk, paradigms should provide serialization hooks
blob = serialize_solution(S)
S = deserialize_solution(blob)
which RISE stores without inspecting.
11.9. Examples
11.9.1. The OccBin paradigm
The piecewise-linear (Guerrieri–Iacoviello, “OccBin”) method for an
arbitrary number of occasionally-binding constraints is shipped as a
ready-to-use paradigm, occbin.paradigm. The whole method lives in the
paradigm package: RISE exchanges only the standard solution envelope and
never needs a dedicated occbin option or any in-core occbin state.
Write the model as a Markov-switching model with one reference regime in
which no constraint binds, plus, for each constraint, a chain whose second
state is the binding branch (e.g. the policy-rate equation becomes
R = bind*r_zlb + (1-bind)*R_TAYLOR). Then activate the paradigm at solve
time:
m = dsge_model('mymodel');
C = { struct('var','R','dir',-1,'bound',1,'chain','ocb') }; % R >= 1
m = set(m,'solve_paradigm',{@occbin.paradigm,'ref',1,'constraints',C});
m = solve(m);
sims = simulate(m,'simul_periods',1000);
RISE stays agnostic about what the paradigm needs: the paradigm itself
imposes a single common (unique, imposed) steady state and pins the
constraint chains’ transition probabilities to zero – the binding regime is
chosen by the constraints, not by chance – so you do not pass
sstate_imposed / sstate_unique and do not set those transition
probabilities in the calibration.
constraints is a cell of structs, one per constraint:
field |
meaning |
|---|---|
|
endogenous variable carrying the bound (char) |
|
|
|
the numeric bound |
|
name of the Markov chain that switches this constraint (char) |
ref is the reference regime index (where every chain is in its
non-binding state). Further options: maxspell (default 200, the
longest binding spell tried before giving up) and use_pinv (default
true). The paradigm enforces the constraint itself, so
use_rise_constraint_enforcer is false.
At solve time the paradigm imposes the (common) steady state, evaluates the structural system under each regime, and solves only the reference regime. At simulation time it takes a reference-regime step each period; if a constraint is violated it grows a binding spell (backward recursion with the reference rule as the terminal condition) until the period after the spell is slack again. For several constraints the active set at each date is the set of violated constraints, and the matching regime is read from the model’s regime table, so the method scales to any number of chains.
There is no filter_engine: OccBin has no associated filtering
procedure, so estimation/filtering under this paradigm is not provided.
The model-side construction (the binding chain and the convex-combination equation) is described in Occasionally-binding constraints.
11.9.2. Recursive local linearization (RLL)
solve_enginecallsregular_solverread-only, extracts the baseline local policy \((k_0, H_0, G_0)\), stores everything in anrll.SolutionHandle, and returns the standard envelope withS.solution = payload.one_step_engine(S)returns a closure that builds a zero-shock stance, re-evaluates the structural derivatives at that stance, solves the local linear system for updated \((k_t, H_t, G_t)\), updates the payload in place, and returns \(x_t\) together with \((k_t, H_t, G_t)\) for the smoother.
11.9.3. \(k\)-th order Taylor projection (TP)
solve_enginecallsregular_solverread-only, uses the perturbation solution as a warm start, runsrtp.solveorder by order to obtain \(T^* = \{T_1^*,\dots,T_h^*\}\), and stores \(T^*\), the topology andget_Fin anrtp.SolutionHandle. The solved coefficients are converted to divided differences (Taylor coefficients) before they are stored, so that\[x_t = \sum_{q=0}^{K} T^*_{\text{regime}}\{q{+}1\}\, \bigl(z_t - z_{\text{anchor}}\bigr)^{\otimes q}.\]one_step_engine(S)returns a closure with two schemes, selected by thereanchoroption:re-anchored (
reanchor=true, the default — Levintal’s scheme): at each step it rebuildsget_Fwith the anchor at the current state \(x_{t-1}\) (rtp.from_rise(m, x_{t-1}, opts), which evaluates the model derivatives along the trajectory, with \(x_{t+1}=g(\text{forward state})\)), re-solvesrtp.solvethere, and evaluates the polynomial. This re-centers the approximation on the current state and is what makes TP more accurate than perturbation away from the steady state, at the cost of a projection re-solve per step.fixed polynomial (
reanchor=false): evaluates the stored steady-state anchored \(T^*\) directly. Fast, but at the steady-state anchor this coincides with perturbation (single-anchor TP and perturbation impose the same conditions there).
In both cases \(z_t = (p_{t-1}, b_{t-1}, \sigma{=}1, \varepsilon_t)\) and \(z_{\text{anchor}} = (p_{t-1}, b_{t-1}, \sigma{=}0, \varepsilon{=}0)\).
Solution accuracy can be quantified with the model’s accuracy method; on the RBC model re-anchored TP attains an Euler error 8–13 times smaller than perturbation at \(\pm 30\%\) capital.
11.9.4. Risk-adjusted linear (RAL)
The risk-adjusted linear paradigm, ral.paradigm, turns a higher-order
perturbation solution into a linear one that still carries the effect of
uncertainty. solve_engine calls regular_solver read-only at an arbitrary
internal order \(k\) (the user’s choice), then takes the linearization
of that policy function: it keeps every term that fits a linear representation
in the states and shocks – the constant (the precautionary \(\sigma^a\)
level shifts) and the linear and risk-adjusted slope terms – and discards the
genuine curvature (\(\text{state}\times\text{state}\),
\(\text{state}\times\text{shock}\), …) and every higher-order block. The
result is the affine policy
where \(c\) is the precautionary level correction and \(A, B\) are the risk-adjusted slopes. Under regime switching the linearization is taken per regime, so each regime gets its own precautionary level and slopes.
Unlike the other paradigms, RAL dissolves after solving. Because its output
is a genuine first-order solution, solve_engine hands the native
state_space back to RISE (signalling S.dissolve = true in the envelope)
and steps aside: the dispatcher adopts the native solution and clears the
paradigm, so from then on the model is an ordinary first-order model. Every
downstream path – simulate, irf, and in particular the analytic linear
Kalman filter that RISE auto-selects when no filter is named – runs natively,
with no bespoke RAL one_step or filter. The precautionary level is carried
in the sigma (perturbation) column of the first-order solution, so it enters
simulation and the filter constant and correctly cancels out of impulse
responses (which are deviations).
Activate it at solve time:
m = dsge_model('mymodel','max_deriv_order',2);
m = set(m,'solve_paradigm',{@ral.paradigm,'order',2});
m = solve(m); % m is now a native first-order model
sims = simulate(m,'simul_periods',1000);
The order option (default 2) is the internal perturbation order from which
the risk correction is read: order 2 captures the leading precautionary
level and the risk-adjusted slopes; higher orders additionally fold in the
\(\sigma^a\) (\(a>2\)) corrections. The output is first order
regardless. Evaluation is first-order cheap and needs no pruning – the only
nonlinear content, the curvature, has been removed – and the residual gap to
the full order-\(k\) solution is exactly that discarded curvature.
11.10. Design principles
A model has exactly one paradigm.
A model may have multiple parameterizations; each has one solution
S.Mis always read-only inside a paradigm.S.solutionis always opaque to RISE.The envelope gives RISE just enough to orchestrate workflows.
Mutable simulation-time state lives inside
S.solutionvia handle semantics.Paradigm-specific solution concepts (eigenvalues, number of solutions, Taylor coefficients) live inside
S.solution, not in the envelope.A dissolving paradigm (e.g.
ral.paradigm) is the one exception to the first and fourth points: when its result is itself a standard solution it setsS.dissolve = trueand hands back a nativestate_space; the dispatcher adopts it and clears the paradigm, leaving a paradigm-free model that RISE filters and simulates with its ordinary machinery.