Merge pull request SciML#268 from ArnoStrouwen/canon

canonify docs

Author: ChrisRackauckas

README.md

@@ -1,9 +1,7 @@
 # JumpProcesses.jl
 
 [![Join the chat at https://julialang.zulipchat.com #sciml-bridged](https://img.shields.io/static/v1?label=Zulip&message=chat&color=9558b2&labelColor=389826)](https://julialang.zulipchat.com/#narrow/stream/279055-sciml-bridged)
-[![Stable](https://img.shields.io/badge/docs-stable-blue.svg)](http://jump.sciml.ai/stable/)
-[![Dev](https://img.shields.io/badge/docs-dev-blue.svg)](http://jump.sciml.ai/dev/)
-[![Global Docs](https://img.shields.io/badge/docs-SciML-blue.svg)](https://docs.sciml.ai/dev/modules/JumpProcesses/)
+[![Global Docs](https://img.shields.io/badge/docs-SciML-blue.svg)](https://docs.sciml.ai/JumpProcesses/stable/)
 
 [![Coverage Status](https://coveralls.io/repos/github/SciML/JumpProcesses.jl/badge.svg?branch=master)](https://coveralls.io/github/SciML/JumpProcesses.jl?branch=master)
 [![codecov](https://codecov.io/gh/SciML/JumpProcesses.jl/branch/master/graph/badge.svg)](https://codecov.io/gh/SciML/JumpProcesses.jl)
@@ -25,18 +23,18 @@ and one of the core solver libraries included in
 [DifferentialEquations.jl](https://github.com/JuliaDiffEq/DifferentialEquations.jl).
 
 For information on using the package,
-[see the stable documentation](http://jump.sciml.ai/stable/). Use the
-[in-development documentation](http://jump.sciml.ai/dev/) for the version of
+[see the stable documentation](https://docs.sciml.ai/JumpProcesses/stable/). Use the
+[in-development documentation](https://docs.sciml.ai/JumpProcesses/dev/) for the version of
 the documentation, which contains the unreleased features. 
 
 The documentation includes
-- [a tutorial on simulating basic Poisson processes](https://jump.sciml.ai/stable/tutorials/simple_poisson_process/)
-- [a tutorial and details on using JumpProcesses to simulate jump processes via SSAs (i.e. Gillespie methods)](https://jump.sciml.ai/stable/tutorials/discrete_stochastic_example/),
-- [a tutorial on simulating jump-diffusion processes](https://jump.sciml.ai/stable/tutorials/jump_diffusion/),
-- [a reference on the types of jumps and available simulation methods](https://jump.sciml.ai/stable/jump_types/),
-- [a reference on jump time stepping methods](https://jump.sciml.ai/stable/jump_solve/),
-- [a FAQ](https://jump.sciml.ai/stable/faq) with information on changing parameters between simulations and using callbacks,
-- [the JumpProcesses.jl API documentation](https://jump.sciml.ai/stable/api/).
+- [a tutorial on simulating basic Poisson processes](https://docs.sciml.ai/JumpProcesses/stable/tutorials/simple_poisson_process/)
+- [a tutorial and details on using JumpProcesses to simulate jump processes via SSAs (i.e. Gillespie methods)](https://docs.sciml.ai/JumpProcesses/stable/tutorials/discrete_stochastic_example/),
+- [a tutorial on simulating jump-diffusion processes](https://docs.sciml.ai/JumpProcesses/stable/tutorials/jump_diffusion/),
+- [a reference on the types of jumps and available simulation methods](https://docs.sciml.ai/JumpProcesses/stable/jump_types/),
+- [a reference on jump time stepping methods](https://docs.sciml.ai/JumpProcesses/stable/jump_solve/),
+- [a FAQ](https://docs.sciml.ai/JumpProcesses/stable/faq) with information on changing parameters between simulations and using callbacks,
+- [the JumpProcesses.jl API documentation](https://docs.sciml.ai/JumpProcesses/stable/api/).
 
 ## Installation
 There are two ways to install `JumpProcesses.jl`. First, users may install the meta
@@ -48,7 +46,7 @@ the facilities for developing and solving Jump problems.
 
 To install the `DifferentialEquations.jl` package, refer to the following link
 for complete [installation
-details](https://docs.sciml.ai/dev/modules/DiffEqDocs/).
+details](https://docs.sciml.ai/DiffEqDocs/stable/).
 
 If the user wishes to separately install the `JumpProcesses.jl` library, which is a
 lighter dependency than `DifferentialEquations.jl`, then the following code will

docs/make.jl

@@ -19,7 +19,7 @@ makedocs(sitename = "JumpProcesses.jl",
          doctest = false,
          format = Documenter.HTML(; analytics = "UA-90474609-3",
                                   assets = ["assets/favicon.ico"],
-                                  canonical = "https://jump.sciml.ai/stable/",
+                                  canonical = "https://docs.sciml.ai/JumpProcesses/",
                                   prettyurls = (get(ENV, "CI", nothing) == "true"),
                                   mathengine),
          pages = pages)

docs/src/faq.md

@@ -143,7 +143,7 @@ of `u[1]`, giving
 
 ## How can I access earlier solution values in callbacks?
 When using an ODE or SDE time-stepper that conforms to the [integrator
-interface](https://docs.sciml.ai/dev/modules/DiffEqDocs/basics/integrator/) one
+interface](https://docs.sciml.ai/DiffEqDocs/stable/basics/integrator/) one
 can simply use `integrator.uprev`. For efficiency reasons, the pure jump
 [`SSAStepper`](@ref) integrator does not have such a field. If one needs
 solution components at earlier times one can save them within the callback

docs/src/index.md

@@ -7,7 +7,7 @@ jump-ODE and jump-SDE models, including jump diffusions.
 
 JumpProcesses is a component package in the [SciML](https://sciml.ai/) ecosystem,
 and one of the core solver libraries included in
-[DifferentialEquations.jl](https://github.com/JuliaDiffEq/DifferentialEquations.jl).
+[DifferentialEquations.jl](https://docs.sciml.ai/DiffEqDocs/stable/).
 
 The documentation includes
 - [a tutorial on simulating basic Poisson processes](@ref poisson_proc_tutorial)
@@ -28,7 +28,7 @@ the facilities for developing and solving Jump problems.
 
 To install the `DifferentialEquations.jl` package, refer to the following link
 for complete [installation
-details](https://docs.sciml.ai/dev/modules/DiffEqDocs/).
+details](https://docs.sciml.ai/DiffEqDocs/stable).
 
 If the user wishes to separately install the `JumpProcesses.jl` library, which is a
 lighter dependency than `DifferentialEquations.jl`, then the following code will

docs/src/jump_types.md

@@ -139,7 +139,7 @@ MassActionJump(reactant_stoich, net_stoich; scale_rates = true, param_idxs=nothi
   ```
   is preferred over
   ```julia
-  reactant_stoich = [[3 => 1, 1 => 2, 4 = > 2], [3 => 2, 2 => 2]]
+  reactant_stoich = [[3 => 1, 1 => 2, 4 => 2], [3 => 2, 2 => 2]]
   ```
 
 
@@ -236,7 +236,7 @@ jump-jump dependency graph, passed through the named parameter `dep_graph`. i.e.
 JumpProblem(prob,DirectCR(),jump1,jump2; dep_graph=your_dependency_graph)
 ```
 For systems with only `MassActionJump`s, or those generated from a
-[Catalyst](https://github.com/SciML/Catalyst.jl) `reaction_network`, this graph
+[Catalyst](https://docs.sciml.ai/Catalyst/stable/) `reaction_network`, this graph
 will be auto-generated. Otherwise you must construct the dependency graph
 manually. Dependency graphs are represented as a `Vector{Vector{Int}}`, with the
 `i`th vector containing the indices of the jumps for which rates must be
@@ -253,7 +253,7 @@ through the following `JumpProblem` kwargs:
    of variable indices. The corresponding variables are those that have their
    value, `u[i]`, altered when the jump occurs.
 
-For systems generated from a [Catalyst](https://github.com/SciML/Catalyst.jl)
+For systems generated from a [Catalyst](https://docs.sciml.ai/Catalyst/stable/)
 `reaction_network` these will be auto-generated. Otherwise you must explicitly
 construct and pass in these mappings.
 
@@ -274,7 +274,7 @@ For representing and aggregating constant rate jumps
 In general, for systems with sparse dependency graphs if `Direct` is slow, one
 of `SortingDirect`, `RSSA` or `RSSACR` will usually offer substantially better
 performance. See
-[DiffEqBenchmarks.jl](https://github.com/JuliaDiffEq/DiffEqBenchmarks.jl) for
+[DiffEqBenchmarks.jl](https://docs.sciml.ai/SciMLBenchmarksOutput/stable/) for
 benchmarks on several example networks.
 
 ## Remaking `JumpProblem`s

docs/src/tutorials/discrete_stochastic_example.md

@@ -19,16 +19,16 @@ tutorial](@ref poisson_proc_tutorial). We will illustrate
 
 !!! note
 
-    This tutorial assumes you have read the [Ordinary Differential Equations tutorial](https://docs.sciml.ai/dev/modules/DiffEqDocs/tutorials/ode_example/) in [`DifferentialEquations.jl`](https://docs.sciml.ai/dev/modules/DiffEqDocs/).
+    This tutorial assumes you have read the [Ordinary Differential Equations tutorial](https://docs.sciml.ai/DiffEqDocs/stable/tutorials/ode_example/) in [`DifferentialEquations.jl`](https://docs.sciml.ai/DiffEqDocs/stable).
 
 We begin by demonstrating how to build jump processes using
-[JumpProcesses.jl](https://github.com/SciML/JumpProcesses.jl)'s different jump types,
+[JumpProcesses.jl](https://docs.sciml.ai/JumpProcesses/stable/)'s different jump types,
 which encode the rate functions (i.e. transition rates, intensities, or
 propensities) and state changes when a given jump occurs.
 
 Note, the SIR model considered here is a type of stochastic chemical kinetics
 jump process model, and as such the biological modeling functionality of
-[Catalyst.jl](https://github.com/SciML/Catalyst.jl) can be used to easily
+[Catalyst.jl](https://docs.sciml.ai/Catalyst/stable/) can be used to easily
 specify the model and automatically calculate inputs needed for JumpProcesses's
 optimized simulation algorithms. We summarize this alternative approach at the
 beginning for users who may be interested in modeling chemical systems, but note
@@ -40,7 +40,7 @@ reaction, and necessary data structures for the simulation algorithms, such as
 dependency graphs, are automatically calculated.
 
 We'll make use of the
-[DifferentialEquations.jl](https://github.com/SciML/DifferentialEquations.jl)
+[DifferentialEquations.jl](https://docs.sciml.ai/DiffEqDocs/stable/)
 meta package, which includes JumpProcesses and ODE/SDE solvers, Plots.jl, and
 (optionally) Catalyst.jl in this tutorial. If not already installed they can be
 added as follows
@@ -97,9 +97,9 @@ created, and the probability per time some infected individual recovers.
 For those less-familiar with the time-change representation, we next give a more
 intuitive explanation of the model as a collection of chemical reactions, and
 then demonstrate how these reactions can be written in
-[Catalyst.jl](https://github.com/SciML/Catalyst.jl) and seamlessly converted
+[Catalyst.jl](https://docs.sciml.ai/Catalyst/stable/) and seamlessly converted
 into a form that can be used with the
-[JumpProcesses.jl](https://github.com/SciML/JumpProcesses.jl) solvers. Users
+[JumpProcesses.jl](https://docs.sciml.ai/JumpProcesses/stable/) solvers. Users
 interested in how to directly define jumps using the lower-level JumpProcesses
 interface can skip to [Building and Simulating the Jump Process Using the
 JumpProcesses Low-Level Interface](@ref).
@@ -164,7 +164,7 @@ frequently jumps should occur, and an `affect!` function for how the state
 should change when that jump type occurs.
 
 ## Building and Simulating the Jump Processes from Catalyst Models
-Using [Catalyst.jl](https://github.com/SciML/Catalyst.jl) we can input our full
+Using [Catalyst.jl](https://docs.sciml.ai/Catalyst/stable/) we can input our full
 reaction network in a form that can be easily used with JumpProcesses's solvers
 ```@example tut2
 using Catalyst
@@ -175,7 +175,7 @@ end β ν
 ```
 To build a pure jump process model of the reaction system, where the state is
  constant between jumps, we will use a
-[`DiscreteProblem`](https://docs.sciml.ai/dev/modules/DiffEqDocs/types/discrete_types/).
+[`DiscreteProblem`](https://docs.sciml.ai/DiffEqDocs/stable/types/discrete_types/).
 This encodes that the state only changes at the jump times. We do this by giving
 the constructor `u₀`, the initial condition, and `tspan`, the timespan. Here, we
 will start with `999` susceptible people, `1` infected person, and `0` recovered
@@ -270,7 +270,7 @@ jump = ConstantRateJump(rate, affect!)
 where `rate` is a function `rate(u,p,t)` and `affect!` is a function of the
 integrator `affect!(integrator)` (for details on the integrator, see the
 [integrator interface
-docs](https://docs.sciml.ai/dev/modules/DiffEqDocs/basics/integrator/)). Here
+docs](https://docs.sciml.ai/DiffEqDocs/stable/basics/integrator/)). Here
 `u` corresponds to the current state vector of the system; for our SIR model
 `u[1] = S(t)`, `u[2] = I(t)` and `u[3] = R(t)`. `p` corresponds to the parameters of
 the model, just as used for passing parameters to derivative functions in ODE
@@ -309,7 +309,7 @@ people in the different states.*
 
 Since we want the system state to change only at the discrete jump times, we
 will build a
-[`DiscreteProblem`](https://docs.sciml.ai/dev/modules/DiffEqDocs/types/discrete_types/)
+[`DiscreteProblem`](https://docs.sciml.ai/DiffEqDocs/stable/types/discrete_types/)
 ```@example tut2
 prob = DiscreteProblem(u₀, tspan, p)
 ```
@@ -390,22 +390,22 @@ problems involving only `ConstantRateJump`s and `MassActionJump`s.
 ## [Reducing Memory Use: Controlling Saving Behavior](@id save_positions_docs)
 
 Note that jumps act via DifferentialEquations.jl's [callback
-interface](https://docs.sciml.ai/dev/modules/DiffEqDocs/features/callback_functions/),
+interface](https://docs.sciml.ai/DiffEqDocs/stable/features/callback_functions/),
 which defaults to saving at each event. This is required in order to accurately
 resolve every discontinuity exactly (and this is what allows for perfectly
 vertical lines in plots!). However, in many cases when using jump problems you
 may wish to decrease the saving pressure given by large numbers of jumps. To do
 this, you set the `save_positions` keyword argument to `JumpProblem`. Just like
 for other
-[callbacks](https://docs.sciml.ai/dev/modules/DiffEqDocs/features/callback_functions/),
+[callbacks](https://docs.sciml.ai/DiffEqDocs/stable/features/callback_functions/),
 this is a tuple `(bool1, bool2)` which sets whether to save before or after a
 jump. If we do not want to save at every jump, we would thus pass:
 ```@example tut2
 jump_prob = JumpProblem(prob, Direct(), jump, jump2; save_positions = (false, false))
 ```
 Now the saving controls associated with the integrator should specified, see the
 main [SciML
-Docs](https://docs.sciml.ai/dev/modules/DiffEqDocs/basics/common_solver_opts/)
+Docs](https://docs.sciml.ai/DiffEqDocs/stable/basics/common_solver_opts/)
 for saving options. For example, we can use `saveat = 10.0` to save at an evenly
 spaced grid:
 ```@example tut2

docs/src/tutorials/jump_diffusion.md

@@ -2,7 +2,7 @@
 
 !!! note
 
-    This tutorial assumes you have read the [Ordinary Differential Equations tutorial](https://docs.sciml.ai/dev/modules/DiffEqDocs/tutorials/ode_example/) in [`DifferentialEquations.jl`](https://docs.sciml.ai/dev/modules/DiffEqDocs/).
+    This tutorial assumes you have read the [Ordinary Differential Equations tutorial](https://docs.sciml.ai/DiffEqDocs/stable/tutorials/ode_example/) in [`DifferentialEquations.jl`](https://docs.sciml.ai/DiffEqDocs/stable).
 
 Jump Diffusion equations are stochastic differential equations with discontinuous
 jumps. These can be written as:
@@ -67,9 +67,9 @@ value 2, we do:
 rate(u, p, t) = 2
 ```
 Now we define the `affect!` of the jump. This is the same as an `affect!` from a
-[`DiscreteCallback`](https://docs.sciml.ai/dev/modules/DiffEqDocs/features/callback_functions/),
+[`DiscreteCallback`](https://docs.sciml.ai/DiffEqDocs/stable/features/callback_functions/),
 and thus acts directly on the
-[integrator](https://docs.sciml.ai/dev/modules/DiffEqDocs/basics/integrator/).
+[integrator](https://docs.sciml.ai/DiffEqDocs/stable/basics/integrator/).
 Therefore, to make it halve the current value of `u`, we do:
 ```@example tut3
 function affect!(integrator)

docs/src/tutorials/simple_poisson_process.md

@@ -12,7 +12,7 @@ parameters, and current time. Throughout this tutorial these are denoted by `u`,
 `p` and `t`. Likewise, when a jump occurs any
 DifferentialEquations.jl-compatible change to the current system state, as
 encoded by a [DifferentialEquations.jl
-integrator](https://docs.sciml.ai/dev/modules/DiffEqDocs/basics/integrator/), is
+integrator](https://docs.sciml.ai/DiffEqDocs/stable/basics/integrator/), is
 allowed. This includes changes to the current state or to parameter values.
 
 This tutorial requires several packages, which can be added if not already
@@ -80,7 +80,7 @@ occurred (at time `integrator.t`)
 affect!(integrator) = (integrator.u[1] += 1)
 ```
 Here the convention is to take a [DifferentialEquations.jl
-integrator](https://docs.sciml.ai/dev/modules/DiffEqDocs/basics/integrator/),
+integrator](https://docs.sciml.ai/DiffEqDocs/stable/basics/integrator/),
 and directly modify the current solution value it stores. i.e. `integrator.u` is
 the current solution vector, with `integrator.u[1]` the first component of this
 vector. In our case we will only have one unknown, so this will be the current

src/SSA_stepper.jl

@@ -35,7 +35,7 @@ jump_prob = JumpProblem(prob, Direct(), jump, jump2)
 sol = solve(jump_prob, SSAStepper())
 ```
 see the
-[tutorial](https://jump.sciml.ai/stable/tutorials/discrete_stochastic_example/)
+[tutorial](https://docs.sciml.ai/JumpProcesses/stable/tutorials/discrete_stochastic_example/)
 for details.
 """
 struct SSAStepper <: DiffEqBase.DEAlgorithm end

src/extended_jump_array.jl

@@ -4,7 +4,7 @@ $(TYPEDEF)
 Extended state definition used within integrators when there are
 `VariableRateJump`s in a system. For detailed examples and usage information see
 the
-- [Tutorial](https://jump.sciml.ai/stable/tutorials/discrete_stochastic_example/)
+- [Tutorial](https://docs.sciml.ai/JumpProcesses/stable/tutorials/discrete_stochastic_example/)
 
 ### Fields