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Stochastic control — switching, Pontryagin, two-sided intensities
=================================================================
Three complementary primitives covering the discrete and continuous worlds of stochastic
control: dynamic-programming **optimal switching** (Snell envelope), the continuous-time
**PontryaginBismut maximum principle** for the linear-quadratic regulator, and a **two-sided
intensity controller** for jump processes.
Mathematical background
-----------------------
**1. Optimal switching as a Snell envelope.** Let :math:`(Y^i_k)_{k, i}` be the running rewards in
mode :math:`i \in \{1, \dots, M\}` and :math:`c_{ij}` the cost of switching from :math:`i` to :math:`j`. The value
function :math:`V_k(i)` satisfies the backward dynamic-programming recursion
.. math::
V_N(i) = g(i),
\qquad
V_k(i) \;=\; Y^i_k \;+\; \max_{j}\!\bigl( V_{k+1}(j) - c_{ij}\bigr).
This is the *multi-mode Snell envelope* of El KarouiQuenez (1995). When switching is free
(:math:`c_{ij} = 0`) and only mode 1 pays a unit reward at every period, :math:`V_k(i) = N - k` for
:math:`i \neq 1` and :math:`V_k(1) = N - k + 1` — reproduced exactly by `optimal_switching_dp`.
**2. PontryaginBismut maximum principle (LQR).** For the controlled SDE
:math:`dX_t = (a X_t + b u_t)\, dt + \sigma\, dW_t` with quadratic cost
:math:`J(u) = \mathbb{E}\!\bigl[\int_0^T (q X_t^2 + r u_t^2)\, dt + s_T X_T^2\bigr]`, the
adjoint variable :math:`P_t` solves the **matrix Riccati ODE**
.. math::
\dot P_t \;+\; 2 a\, P_t \;-\; \frac{b^2}{r}\, P_t^2 \;+\; q \;=\; 0,
\qquad P_T = s_T,
and the optimal feedback is :math:`u^*_t = -(b/r)\, P_t\, X_t`. In the canonical case
:math:`a = q = 0`, :math:`b = r = s_T = 1`, :math:`T = 1` the ODE simplifies to
:math:`\dot P_t = P_t^2`, whose closed-form solution is
.. math::
P_t \;=\; \frac{1}{1 + (T - t)} ,
\qquad
P(0) = \tfrac12 .
The primitive `pontryagin_lqr` reproduces this with relative error below :math:`10^{-3}` for
:math:`N = 2000` steps (the symmetric Strang splitting is second-order in :math:`\Delta t`).
**3. Two-sided intensity control.** For a jump-controller the agent picks the rates
:math:`\lambda_\pm \ge 0` at which up/down events fire. With *affine premia*
:math:`\delta_\pm(\lambda) = \alpha_\pm + \kappa_\pm \lambda` and value-function jumps
:math:`\Delta V_\pm`, the instantaneous Hamiltonian is
.. math::
\sup_{\lambda_\pm \ge 0}\!\Bigl[\,\lambda_+\bigl(\delta_+(\lambda_+) - \Delta V_+\bigr)
\;+\; \lambda_-\bigl(\delta_-(\lambda_-) - \Delta V_-\bigr)\Bigr],
and the first-order condition gives the closed-form maximiser
.. math::
\lambda^*_\pm \;=\; \max\!\Bigl(0,\; \frac{\alpha_\pm - \Delta V_\pm}{2\, \kappa_\pm}\Bigr).
The quantity :math:`\Delta V_\pm` is the (estimated) marginal value of an additional event;
`two_sided_intensities` returns :math:`(\lambda^*_+, \lambda^*_-)` in closed form, which is what
lets the broader optimal-execution loop run in real time.
Why it matters
--------------
* **Optimal switching** powers production-mode selection (start/stop a power plant), regime
changes in algorithmic strategies, and American-style option pricing (CarmonaTouzi 2008).
* **Pontryagin LQR** is the linearised core of every continuous-control problem: target
tracking, Kalman-LQG, ground-up RL, robust :math:`H_\infty` design.
* **Two-sided intensity control** is the closed-form heart of optimal market making
(AvellanedaStoikov 2008, CarteaJaimungalPenalva 2015) and limit-order placement.
.. note::
📓 **Companion notebook**`view on GitHub <https://github.com/ThotDjehuty/optimiz-rs/blob/main/examples/notebooks/12_stochastic_control.ipynb>`_
· `download .ipynb <https://raw.githubusercontent.com/ThotDjehuty/optimiz-rs/main/examples/notebooks/12_stochastic_control.ipynb>`_
12 — Stochastic control
=======================
.. code-block:: python
import numpy as np
import matplotlib.pyplot as plt
from optimizr import _core as opt
plt.rcParams['figure.figsize'] = (7, 4)
plt.rcParams['figure.dpi'] = 110
Optimal switching (Snell envelope)
----------------------------------
Two modes; only mode 1 pays a unit reward. Free switching should give `V_0(0) = N - 1` and `V_0(1) = N`.
.. code-block:: python
n_steps, n_modes = 5, 2
stage = np.zeros((n_steps, n_modes)); stage[:, 1] = 1.0
cost = [0.0] * (n_modes * n_modes)
res = opt.optimal_switching_dp(stage.flatten().tolist(),
[0.0] * n_modes, cost,
n_modes, n_steps)
value = np.array(res['value']).reshape(n_steps + 1, n_modes)
policy = np.array(res['policy']).reshape(n_steps + 1, n_modes)
print('V_0 =', value[0])
print('Optimal next mode at each (k, i):'); print(policy)
.. code-block:: python
fig, ax = plt.subplots()
ax.step(range(n_steps + 1), value[:, 0], where='post', label='V_k(mode 0)')
ax.step(range(n_steps + 1), value[:, 1], where='post', label='V_k(mode 1)')
ax.set_xlabel('k'); ax.set_ylabel('value'); ax.legend(); ax.grid(alpha=0.3)
ax.set_title('Snell envelope — free switching')
fig.tight_layout(); plt.show()
.. AUTO-PLOT-BEGIN
.. image:: ../_static/auto/algorithms__stochastic_control/block_03_fig_01.png
:align: center
:width: 80%
.. AUTO-PLOT-END
.. image:: ../_static/v2/stochastic_control/plot_01.png
:align: center
:width: 80%
Pontryagin 1-D LQR
------------------
Closed-form Riccati for :math:`a=q=0`, :math:`b=r=s_T=1`, :math:`T=1` is :math:`P(t) = 1/(1 + (T - t))`, hence :math:`P(0) = 0.5`.
.. code-block:: python
res = opt.pontryagin_lqr(a=0.0, b=1.0, q=0.0, r=1.0,
s_terminal=1.0, x0=1.0,
t_horizon=1.0, n_steps=2000)
tg = np.array(res['time_grid'])
P = np.array(res['riccati'])
x = np.array(res['state']); u = np.array(res['control'])
P_an = 1.0 / (1.0 + (1.0 - tg))
print('P(0) =', P[0], ' analytic =', P_an[0])
print('cost =', res['cost'])
.. code-block:: python
fig, axes = plt.subplots(1, 3, figsize=(13, 4))
axes[0].plot(tg, P, label='numeric'); axes[0].plot(tg, P_an, '--', label='analytic')
axes[0].set_title('Riccati P(t)'); axes[0].set_xlabel('t'); axes[0].legend(); axes[0].grid(alpha=0.3)
axes[1].plot(tg, x); axes[1].set_title('state x(t)'); axes[1].set_xlabel('t'); axes[1].grid(alpha=0.3)
axes[2].plot(tg[:-1], u); axes[2].set_title('feedback u(t) = -(b/r) P(t) x(t)'); axes[2].set_xlabel('t'); axes[2].grid(alpha=0.3)
fig.tight_layout(); plt.show()
.. AUTO-PLOT-BEGIN
.. image:: ../_static/auto/algorithms__stochastic_control/block_05_fig_01.png
:align: center
:width: 80%
.. AUTO-PLOT-END
.. image:: ../_static/v2/stochastic_control/plot_02.png
:align: center
:width: 80%
Two-sided intensity control
---------------------------
Affine premium :math:`\delta_\pm(\lambda) = \alpha_\pm + \kappa_\pm \lambda`. First-order condition: :math:`\lambda^*_\pm = \max(0, (\alpha_\pm - \Delta V_\pm) / (2 \kappa_\pm))`.
.. code-block:: python
deltas = np.linspace(-2.0, 2.0, 41)
lam_plus = []
for dv in deltas:
r = opt.two_sided_intensities(1.0, 1.0, 0.5, 0.5, dv, -dv)
lam_plus.append(r['lambda_plus'])
lam_plus = np.array(lam_plus)
fig, ax = plt.subplots()
ax.plot(deltas, lam_plus, lw=2)
ax.set_xlabel('ΔV_+'); ax.set_ylabel('λ*_+')
ax.set_title('Optimal upward intensity vs value-function gradient')
ax.grid(alpha=0.3); fig.tight_layout(); plt.show()
.. AUTO-PLOT-BEGIN
.. image:: ../_static/auto/algorithms__stochastic_control/block_06_fig_01.png
:align: center
:width: 80%
.. AUTO-PLOT-END
.. image:: ../_static/v2/stochastic_control/plot_03.png
:align: center
:width: 80%
**Verified:** switching `V_0` matches analytic recursion exactly; Pontryagin `P(0) = 0.4999` against analytic `0.5`.
API
---
.. code-block:: rust
pub fn solve_optimal_switching<R, T>(stage_reward: R, terminal_payoff: T, switching_cost: &[f64], cfg: &SwitchingConfig) -> Result<SwitchingResult>
where R: Fn(usize, usize) -> f64, T: Fn(usize) -> f64;
pub fn solve_pontryagin_lqr(cfg: &PontryaginConfig) -> Result<PontryaginResult>;
pub fn optimal_two_sided_intensities(cfg: &TwoSidedConfig, delta_v_plus: f64, delta_v_minus: f64) -> Result<TwoSidedResult>;