API Reference
Solve functions
tinydiffeq.solve_ode(f, solver, t_0, t_1, x_0, *, p=None, args=None, dt_0=None, save_at=None, controller=None, max_steps=4096, project=None, has_aux=None, failure_ad_reference=None, adaptive_loop='bounded', unroll=1)
Integrate dx/dt = f(x, t, args, p) from t_0 to t_1 > t_0.
The field may be declared f(x), f(x, t), f(x, t, args), or
f(x, t, args, p); x is an array or pytree with one real floating
dtype, args is inert data, and p holds differentiable parameters.
dt_0 is required. Fixed stepping and the default
adaptive_loop="bounded" use bounded lax.scan loops with exactly
max_steps attempt slots and support forward and reverse AD;
adaptive_loop="forward" runs a dynamic lax.while_loop (primal,
JVP, and nested forward mode only). project (an idempotent clamp) is
applied at every field evaluation and accepted state. The field may
return (dx, aux); saved aux follows SaveAt and participates in
AD. unroll (a static int, fixed stepping only) unrolls that many
steps per iteration of the integration scan — identical values,
fewer/larger GPU dispatches, more compile time. Returns a
:class:Solution; sol.ok reports whether t_1 was reached with
every requested output valid — outputs are never poisoned.
Source code in src/tinydiffeq/ode.py
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tinydiffeq.solve_bvp(fun, bc, t, y_0, z_0=None, *, p=None, args=None, S=None, fun_jac_ad='auto', bc_jac_ad='auto', tol=0.001, bc_tol=None, max_nodes=128, has_aux=None)
Solve dy/dt = fun(t, y, z, args, p) + S y / (t - t[0]) with
two-point boundary conditions bc(y(t_a), y(t_b), z, args, p) = 0.
A faithful JAX port of :func:scipy.integrate.solve_bvp (4th-order Lobatto
IIIA collocation with residual-controlled mesh refinement and a damped
Newton method), with scipy's algorithm, constants, and default tolerances.
fun and bc are pointwise — a scalar t and one node's state
pytree — and may be declared with 2 to 5 positional arguments in the
orders above. z_0 is the guess for scipy's unknown parameters (any
pytree), solved jointly with y and returned as sol.z; bc must
then return n + size(z) residuals as a 1-D array. p holds known
differentiable parameters — the only AD input: JVP/VJP rules (composing
to higher order) differentiate sol.y, sol.yp, sol.z, and
sol.aux with respect to p implicitly at the solution, never
through the iterations, and the guesses t, y_0, z_0 (and
args, S) are differentiation-inert.
args is inert pass-through data. Local Jacobians come from AD instead
of scipy's finite differences; fun_jac_ad/bc_jac_ad choose
"jvp", "vjp", or "auto" (forward when square or tall, reverse
when strictly fat). max_nodes (static, default 128) fixes the padded
output length: the mesh t starts from the given guess and grows under
refinement, the returned tail repeats t[-1] and the last active rows,
and sol.num_nodes counts active nodes, so
hermite_interpolate(ts, sol.t, sol.y, sol.yp) evaluates exactly
scipy's returned C1 cubic spline (hermite_derivative its derivative).
fun may return (value, aux); aux is evaluated once at the solution
over all padded nodes and participates in AD. tol is floored at
100 * eps of the working dtype (taken from y_0), silently.
Failures never raise inside the solve: sol.status carries scipy's
codes and a singular collocation Jacobian is reported as status 2 with the
last iterate returned. The collocation system is factored once per Newton
refresh by a structured orthogonal factorization of its bordered
almost-block-diagonal form (O(max_nodes) instead of the dense cubic,
where scipy uses sparse LU). The whole solve is compiled with
lax.while_loop loops, keyed on the identity of fun and bc
(reuse module-level functions rather than rebuilding closures per call);
for repeated solves call it inside an outer jax.jit so the wrapper's
per-call validation and dispatch trace away.
Source code in src/tinydiffeq/bvp.py
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tinydiffeq.solve_semi_explicit_dae(f, g, solver, t_0, t_1, y_0, z_0, *, p=None, args=None, dt_0=None, save_at=None, controller=None, root_solver=None, has_aux=None, has_algebraic_aux=None, failure_ad_reference=None, max_steps=4096, adaptive_loop='bounded')
Integrate a semi-explicit index-1 DAE.
The system is dy/dt = f(y, z, t, args, p) with
0 = g(y, z, t, args, p) and a square nonsingular dg/dz. z_0
is a root guess: initial consistency is solved automatically and its
derivative comes from the constraint. RK4 and Tsit5 restore g = 0 at
every stage through :class:LMRootSolver; Rodas5P advances the block
mass-matrix system with one reused LU factorization per attempted step,
so its later z values satisfy the constraint to integration accuracy.
Roots and their implicit derivatives are delegated to nlls-gram. f
may return (dy, saved_aux); g may return
(residual, algebraic_aux), in which case f takes
(y, z, t, args, p, algebraic_aux).
failure_ad_reference=(y, z, t, p) provides a domain-safe point for
inactive vmap lanes. adaptive_loop follows
:func:tinydiffeq.solve_ode. Returns a :class:DAESolution with
root-solve diagnostics.
Source code in src/tinydiffeq/dae.py
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tinydiffeq.solve_semi_explicit_sdae(drift, diffusion, g, solver, t_0, t_1, y_0, z_0, *, key, n_steps, p=None, args=None, save_at=None, root_solver=None, has_aux=None, has_algebraic_aux=None, failure_ad_reference=None)
Integrate a semi-explicit index-1 Ito SDAE with diagonal noise.
The system is dy = drift(y, z, t) dt + diffusion(y, z, t) dW with
0 = g(y, z, t). solver is EulerMaruyama or SRA1, applied
to the reduced SDE obtained from the locally unique root z = Z(y, t):
the differential state advances on a fixed uniform grid of n_steps
steps, and a root solve restores consistency at every node and at SRA1's
drift stage. SRA1's strong order 1.5 requires a diffusion that depends
only on time. A fixed key defines one common-random-numbers path;
JVP/VJP with respect to y_0 and p are pathwise, and z_0 is a
root guess with zero tangent. Aux contracts, failure_ad_reference,
and failure behavior follow solve_semi_explicit_dae.
Source code in src/tinydiffeq/sdae.py
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tinydiffeq.solve_sde(drift, diffusion, solver, t_0, t_1, x_0, *, key=None, n_steps, noise=None, p=None, args=None, save_at=None, project=None, has_aux=None, failure_ad_reference=None, unroll=1)
Integrate the Ito SDE dx = drift dt + diffusion d_w with diagonal
noise on a fixed grid of n_steps uniform steps from t_0 to
t_1 > t_0.
drift and diffusion follow the same signature convention as
solve_ode. solver is EulerMaruyama, Milstein, or SRA1,
each declaring its per-step noise through
solver.sample_noise(x_0, key, n_steps, dt, dtype). Exactly one of
key and noise must be provided: a fixed key presamples a
fixed, reproducible noise process, differentiable with respect to x_0
and p; an explicit noise pytree (validated against the solver's
spec) is additionally differentiable as data. SaveAt(ts=...) raises —
interpolation is wrong for rough paths. drift may return
(value, aux); diffusion is value-only. unroll (a static int)
unrolls that many steps per iteration of the underlying lax.scan —
identical values, fewer/larger GPU dispatches, more compile time.
Source code in src/tinydiffeq/sde.py
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tinydiffeq.solve_linear_ode(operator, method, t_0, t_1, x_0, *, save_at=None)
Solve dx/dt = A(x) for a fixed homogeneous linear operator.
operator is either a square matrix using the column convention
A @ x or a callable mapping the state pytree to an identically
structured pytree. DenseExponential materializes a callable operator
before a dense matrix exponential; the Krylov methods evaluate only
operator actions. Endpoint output is the default, and SaveAt(ts=...)
evaluates independent exponential actions at the requested times. JVPs
and VJPs flow through the initial state and differentiable operator
arrays. The operator must be autonomous, homogeneous, and linear.
Source code in src/tinydiffeq/exponential.py
tinydiffeq.jvp_linear_ode(operator, method, t_0, t_1, x_0, x_0_tangent, *, batched=False)
Return a terminal linear solve and hand-coded initial-state JVP.
With batched=True, every tangent leaf has a leading direction axis.
Dense mode forms one exponential and applies it to every direction.
Matrix-free Krylov mode vectorizes independent exponential actions. The
operator is fixed: use ordinary jax.jvp when differentiating operator
entries or arrays captured by a callable.
Source code in src/tinydiffeq/exponential.py
tinydiffeq.vjp_linear_ode(operator, method, t_0, t_1, x_0, cotangent, *, batched=False)
Return a terminal linear solve and hand-coded initial-state VJP.
The pullback is another exponential action with the transposed operator.
batched=True accepts multiple terminal cotangents on a leading axis.
Dense mode reuses the primal exponential for every cotangent. Callable
transpose actions are generated with jax.linear_transpose and therefore
require the declared operator to be linear in its state argument.
Source code in src/tinydiffeq/exponential.py
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tinydiffeq.simulate_markov_chain(chain, state_0, *, key, num_steps, method=None, save_at=None)
Simulate a primal finite-state homogeneous discrete-time Markov chain.
state_0 is one scalar integer index and key one JAX key. Use
jax.vmap over initial states and independently split keys for ensembles.
num_steps is static. SequentialMarkov is the CPU-oriented default;
AssociativeMarkov composes sampled state maps in parallel and returns the
identical path for the same key. SaveAt selects the endpoint, all steps,
or a one-dimensional array of integer step indices.
Source code in src/tinydiffeq/markov.py
tinydiffeq.simulate_continuous_time_markov_chain(chain, t_0, t_1, state_0, *, key, max_jumps, method=None, save_at=None)
Simulate a primal finite-state CTMC with Gillespie's direct recurrence.
max_jumps is a static bound. Endpoint output is the default;
SaveAt(steps=True) returns the padded event path and SaveAt(ts=...)
evaluates its right-continuous piecewise-constant state. sol.ok is false
if the jump budget does not cover t_1. Associative execution composes
state and holding-time maps; states agree with sequential execution for the
same key, while event times can differ by floating-point reassociation.
Source code in src/tinydiffeq/markov.py
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tinydiffeq.forecast_markov_chain(chain, distribution_0, *, num_steps, method=None, save_at=None)
Forecast a fixed DTMC probability mass function.
Endpoint output defaults to binary matrix powering. Multi-row output defaults
to chronological matrix-vector scan; AssociativeMarkov instead composes
prefix transition matrices and can expose useful GPU parallelism for small
state spaces. The deterministic forecast supports JVP/VJP with respect to
distribution_0; the prepared chain is treated as fixed.
Source code in src/tinydiffeq/markov.py
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tinydiffeq.forecast_continuous_time_markov_chain(chain, t_0, t_1, distribution_0, *, method=None, save_at=None)
Forecast a fixed CTMC probability mass with exponential actions.
For one endpoint this evaluates distribution_0 @ exp((t_1-t_0) Q).
DenseExponential forms the dense exponential.
KrylovExponential applies a static Arnoldi approximation;
AdaptiveKrylovExponential adapts its internal time slices. Both support
MatrixFreeContinuousTimeMarkovChain probability pytrees.
Requested times are independent exponential actions vectorized over the query
axis. JVP/VJP with respect to distribution_0 are supported.
Source code in src/tinydiffeq/markov.py
Solvers
tinydiffeq.Euler
dataclass
Explicit Euler. Fixed-step only: no embedded error estimate.
Source code in src/tinydiffeq/solvers.py
tinydiffeq.RK4
dataclass
Classic fourth-order Runge-Kutta. Fixed-step only: no error estimate.
Source code in src/tinydiffeq/solvers.py
tinydiffeq.Tsit5
dataclass
Tsitouras 5(4) explicit Runge-Kutta with embedded error estimate.
FSAL: the last stage k_7 = g(x_1, t + dt) is the next step's first stage,
so an accepted adaptive step costs six fresh evaluations. Note k_7 is
evaluated at the projected accepted state, so the FSAL cache stays
consistent with the state actually carried forward when project binds.
Source code in src/tinydiffeq/solvers.py
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step_fixed(g, t, x, dt, f_0, project)
Take a fixed step without constructing the unused embedded error.
tinydiffeq.Rodas5P
dataclass
Fifth-order Rodas5P Rosenbrock--Wanner method.
An eight-stage, linearly implicit method with an embedded error estimate
and a stiff-aware fourth-order continuous extension, supported by
:func:tinydiffeq.solve_ode and
:func:tinydiffeq.solve_semi_explicit_dae with one dense LU
factorization reused across the stages of each attempted step. The
implementation follows Steinebach (2023) and SciML's
OrdinaryDiffEqRosenbrock.Rodas5P:
- https://doi.org/10.1007/s10543-023-00967-x
- https://github.com/SciML/OrdinaryDiffEq.jl/tree/master/lib/OrdinaryDiffEqRosenbrock
Source code in src/tinydiffeq/solvers.py
tinydiffeq.EulerMaruyama
dataclass
Euler-Maruyama for Ito SDEs with diagonal noise. Fixed-step only.
Strong order 0.5 for multiplicative noise. sample_noise returns the
Brownian increments with the same pytree structure as the state and a
leading n_steps axis.
Source code in src/tinydiffeq/solvers.py
tinydiffeq.Milstein
dataclass
Milstein for Ito SDEs with diagonal noise. Fixed-step only.
Strong order 1.0 under the diagonal commutativity condition: each
diffusion component may depend only on its own state component. The
correction (1/2) g g' (d_w^2 - dt) evaluates g g' as the
forward-mode derivative of the diffusion field in the direction of its
own value, which equals the diagonal term exactly in that case.
sample_noise matches EulerMaruyama.
Source code in src/tinydiffeq/solvers.py
tinydiffeq.SRA1
dataclass
Rossler SRA1 stochastic Runge-Kutta for Ito SDEs with additive diagonal noise. Fixed-step only.
Strong order 1.5 when the diffusion is independent of the state (it may
depend on time). sample_noise returns (d_w, d_z): two independent
sqrt(dt) * N(0, 1) draws per step. The time-Wiener integral
I_10 / dt is realized internally as (d_w + d_z / sqrt(3)) / 2,
reproducing its variance dt^3 / 3 and covariance dt^2 / 2 with
the increment.
Source code in src/tinydiffeq/solvers.py
tinydiffeq.DenseExponential
dataclass
tinydiffeq.KrylovExponential
dataclass
Static Arnoldi exponential action for an array or callable operator.
krylov_dim, num_substeps, and reorthogonalization_passes are
static compilation controls. Two-pass classical Gram--Schmidt is the
stable default; one pass reduces the dominant basis memory traffic when
the operator has been validated for it. The precision-dependent default
error tolerances are 1e-5/1e-7 for float32 and
1e-10/1e-12 for float64.
Source code in src/tinydiffeq/exponential.py
tinydiffeq.AdaptiveKrylovExponential
dataclass
Adaptive matrix-free Arnoldi exponential action.
The Krylov dimension remains static while accepted internal time slices
adapt to the leading-term Arnoldi residual. max_steps bounds all
accepted and rejected attempts, keeping compiled shapes static. The
precision-dependent tolerance defaults match KrylovExponential.
Source code in src/tinydiffeq/exponential.py
Step-size controllers
tinydiffeq.ConstantStepSize
dataclass
Accept every step and keep the carried step size unchanged.
Source code in src/tinydiffeq/controllers.py
tinydiffeq.IController
dataclass
Integral step-size controller with max-norm error.
Accept iff E = max(|err| / (atol + rtol * max(|x_0|, |x_1|))) <= 1
(forced accept once the step reaches dt_min), and propose
dt_next = dt_used * clip(safety * E**(-1/order), factor_min, factor_max)
clipped to [dt_min, dt_max]. Omitted rtol/atol default to
1e-4/1e-6 for float32 states and 1e-7/1e-9 for float64;
dt_min defaults to ten machine epsilons in the time dtype, scaled by
max(1, |t_1|).
Source code in src/tinydiffeq/controllers.py
tinydiffeq.PIController
dataclass
Proportional-integral step-size controller with max-norm error.
In addition to the current scaled error E, this controller carries the
previous accepted step's error E_prev (starting at one) and proposes
dt_next = dt_used * clip(safety * E**(-(p_coeff+i_coeff)/order)
* E_prev**(p_coeff/order), factor_min, factor_max). The defaults
p_coeff=0.4 and i_coeff=0.3 damp step-size oscillations;
p_coeff=0, i_coeff=1 reproduces :class:IController, and the
tolerance and dt_min defaults match it.
Source code in src/tinydiffeq/controllers.py
Markov-chain models and methods
tinydiffeq.DiscreteMarkovChain
Prepared dense homogeneous finite-state transition matrix.
Construction validates and normalizes the rows and builds Vose alias tables.
Construct once outside transformed code, then pass the object through jit
or as a shared vmap argument.
Source code in src/tinydiffeq/markov.py
tinydiffeq.ContinuousTimeMarkovChain
Prepared dense homogeneous finite-state generator matrix.
Off-diagonal entries must be nonnegative and each row must sum to zero. Zero rows are absorbing states. Construction extracts exit rates and builds alias tables for the embedded jump chain; construct outside transformed code.
Source code in src/tinydiffeq/markov.py
tinydiffeq.MatrixFreeContinuousTimeMarkovChain
Fixed CTMC forward generator represented by a pytree linear action.
forward_generator(probabilities) must return the same probability-pytree
structure and dtype and represent the forward equation dπ/dt = L(π).
The callable is static JAX structure; close only over fixed model data or put
changing arrays inside a callable pytree.
Source code in src/tinydiffeq/markov.py
tinydiffeq.SequentialMarkov
dataclass
Chronological scan method; unroll=1 is the CPU-oriented default.
Source code in src/tinydiffeq/markov.py
tinydiffeq.AssociativeMarkov
dataclass
tinydiffeq.MatrixPowerMarkov
dataclass
Output selection and results
tinydiffeq.SaveAt
dataclass
What the solve functions return. Exactly one mode must be set.
t_1=True (the solver default) returns the endpoint only. ts=grid
interpolates the internal steps onto a fixed query grid — output shape is
(len(ts), ...) however many steps the controller takes, and ts is
a data leaf; with exact=True an explicit constant-step ODE instead
gathers states at queries that must coincide with realized knots.
steps=True returns the initial state and accepted steps as the valid
prefix of a max_steps + 1 buffer, padded with the last valid row
(fill="last") or inf (fill="inf") and masked by
Solution.accepted.
Source code in src/tinydiffeq/save_at.py
tinydiffeq.LMRootSolver
dataclass
Configuration for algebraic root solves in semi-explicit DAEs/SDAEs.
The implementation is :class:nlls_gram.LevenbergMarquardt at its
defaults. max_steps bounds one algebraic root's nonlinear iterations,
independently of the integration's time-step budget. Roots use residual
stopping only: gtol and xtol must remain zero, and every accepted
root must report CONVERGED with Euclidean residual norm strictly below
atol (None selects 1e-6 in float32, 1e-10 in float64).
solver_options is a mapping (or pairs) forwarded verbatim to the
LevenbergMarquardt constructor, e.g.
solver_options={"linear_solver": QR()}; cache_jacobian and
geodesic_acceleration are fixed to False. predictor selects
the explicit-stage warm start: "previous" reuses the most recent
successful root, "secant" extrapolates it to a strictly later stage
time and assumes the continued root is locally unique.
Source code in src/tinydiffeq/dae.py
tinydiffeq.DAESolution
dataclass
Result of the deterministic or stochastic semi-explicit DAE solvers.
ts/ys/zs follow the :class:Solution shape contract, with
zs the algebraic states. Explicit-method saved values sit at
converged roots; Rodas5P satisfies the constraint to integration accuracy
after its initial consistency root, and requested-grid interpolants need
not satisfy it exactly. num_root_solves counts logical active root
calls (including failures and the initial consistency solve) and
num_root_steps sums their LM update steps; like num_steps, both
are path diagnostics with exact-zero tangents.
Source code in src/tinydiffeq/solution.py
tinydiffeq.BVPSolution
dataclass
Result of solve_bvp.
Arrays are padded to the static max_nodes: the t tail repeats the
right endpoint and the y/yp tails repeat the last active row, so
sol(ts) evaluates exactly the C1 cubic spline scipy's solve_bvp
returns and sol.derivative(ts) its derivative. z holds the solved
unknown parameters (None when the
problem has none), rms_residuals is zero on inactive intervals,
num_nodes counts active mesh nodes, and num_iterations is scipy's
niter. status uses scipy's codes (0 converged, 1 max_nodes
exceeded, 2 singular Jacobian, 3 boundary-condition tolerance unsatisfied)
and ok is status == 0; a failed status returns the last iterate,
which may be non-finite. Under AD only y, yp, z, and aux
carry tangents with respect to p; every other field is
differentiation-inert with exact-zero tangents.
Source code in src/tinydiffeq/solution.py
tinydiffeq.Solution
dataclass
Result of solve_ode/solve_sde/solve_linear_ode.
ts/xs hold times and states in the shape dictated by SaveAt.
ok is a scalar bool: the integration reached t_1 and every
required saved output was valid. Outputs are never poisoned; callers that
want diverging values map jnp.where(sol.ok, x, jnp.inf) over leaves.
num_accepted counts accepted steps, num_steps counts logical
attempts including rejections, accepted masks the valid prefix in
steps mode (row 0 is always True), and aux holds the field's
saved auxiliary pytree with the same leading saved-time axis as xs.
Source code in src/tinydiffeq/solution.py
tinydiffeq.MarkovDistribution
dataclass
Forecast probability mass, evaluation steps/times, and validity flag.
Source code in src/tinydiffeq/markov.py
Utilities
tinydiffeq.diagonal_brownian_increments(x_0, key, n_steps, dt, dtype)
Draw n_steps diagonal Brownian increments sqrt(dt) * N(0, 1).
Arrays retain the exact (n_steps,) + x_0.shape draw. Pytree states use
one shared flat draw, partitioned into leaves in JAX's deterministic
pytree leaf order.
Source code in src/tinydiffeq/solvers.py
tinydiffeq.hermite_interpolate(ts_query, knot_ts, knot_xs, knot_fs)
Cubic Hermite interpolation of (knot_ts, knot_xs, knot_fs) at
ts_query, where knot_fs holds the time derivatives at the knots.
knot_ts must be nondecreasing; duplicate knots are allowed and
queries falling on a zero-width bracket return the left knot value.
Queries outside the knot span clamp to the boundary knot values (flat
extrapolation) rather than evaluating the cubic outside its bracket.
Source code in src/tinydiffeq/interpolation.py
tinydiffeq.hermite_derivative(ts_query, knot_ts, knot_xs, knot_fs)
Derivative of the C1 cubic Hermite interpolant at ts_query.
Uses searchsorted(side="left") so a query at a repeated right-endpoint
knot lands on the last positive-width bracket and returns the knot
derivative instead of the degenerate bracket's zero. Queries outside the
knot span return zero, the derivative of the clamped value extension.
Source code in src/tinydiffeq/interpolation.py
tinydiffeq.cumulative_trapezoid(g, ts, *, substeps=1)
Cumulative composite-trapezoid integral of a time-only g(t) on the
(possibly nonuniform) sorted grid ts.
Each grid interval is subdivided into substeps uniform panels, so the
quadrature error shrinks with substeps without changing the output
grid. Returns (integral, values) where integral[k] approximates
the integral of g from ts[0] to ts[k] (integral[0] = 0)
and values = g(ts); g may return any array shape, which is
appended to the leading grid axis.