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Quadratic-impact control — closed-form Riccati
==============================================
Closed-form Riccati feedback for the canonical *single-state, quadratic-cost* linear control
problem with running quadratic *impact* penalty.
Mathematical background
-----------------------
Let :math:`A_t` be a controlled scalar state driven by an additive control :math:`u_t` and Gaussian noise.
The controller minimises the *finite-horizon quadratic objective*
.. math::
J(u) \;=\; \mathbb{E}\!\left[\,\int_0^T \bigl(\,\tfrac{\gamma}{2}\, u_t^2
\;+\; \tfrac{\phi}{2}\, A_t^2 \,\bigr)\, dt
\;+\; \tfrac{A_T}{2}\, A_T^2 \,\right] ,
where :math:`\gamma > 0` is the **impact / control cost**, :math:`\phi \ge 0` the **running risk weight**
and :math:`A_T` the **terminal penalty** (over-loaded notation: :math:`A_T` here is the *coefficient*).
**HamiltonJacobiBellman.** With value function :math:`v(t, A) = \tfrac12 h(t)\, A^2 + c(t)`, the
HJB equation collapses to a scalar Riccati ODE on :math:`h`:
.. math::
h'(t) \;=\; \frac{h(t)^2}{\gamma} \;-\; \phi,
\qquad
h(T) \;=\; A_T .
The optimal feedback is the linear law
.. math::
u^*(t, A) \;=\; -\, \frac{h(t)}{\gamma}\, A \;\equiv\; -\, k(t)\, A,
with *feedback gain* :math:`k(t) = h(t) / \gamma`. This is the structure returned by the primitive.
**Closed-form solutions.**
* **Symmetric fixed point** :math:`\gamma = \phi = A_T = 1`: :math:`h(t) \equiv 1` is the unique solution
(RHS vanishes), so the feedback gain is constant :math:`k \equiv 1`. The notebook checks this
to machine precision.
* **Generic :math:`\phi > 0`.** Writing :math:`\bar h = \sqrt{\gamma \phi}` for the steady-state and
:math:`\rho = \sqrt{\phi / \gamma}`, the Riccati ODE has the closed-form (separation of variables /
Bernoulli substitution)
.. math::
h(t) \;=\; \bar h\, \frac{(\bar h + A_T)\, e^{2\rho(T-t)} \;-\; (\bar h - A_T)}
{(\bar h + A_T)\, e^{2\rho(T-t)} \;+\; (\bar h - A_T)} .
In the limit :math:`T - t \to \infty` the trajectory relaxes to the stationary value :math:`\bar h = \sqrt{\gamma\phi}`.
* **Free of running risk** :math:`\phi = 0`. Then :math:`h'(t) = h(t)^2/\gamma` integrates explicitly to
.. math::
h(t) \;=\; \frac{A_T}{1 + (A_T / \gamma)(T - t)} ,
recovering the Pontryagin LQR closed form :math:`P(0) = 1/2` of :doc:`stochastic_control`.
**Connection with mean-field games.** Coupling this single-agent control with an interacting
population — the running cost depending on the *average* control :math:`\bar u_t` — yields the
AlmgrenChriss MFG (LasryLions 2007); at the Nash equilibrium the optimal trajectory is the
uniform schedule :math:`\dot A^*_t = -A_0 / T` (cf. Sec. 3 of CarmonaDelarue 2018, Vol. I).
Why it matters
--------------
* **Optimal execution.** AlmgrenChriss and its mean-field variants reduce to exactly this
Riccati ODE; the closed form means *real-time* feedback re-computation.
* **Stochastic regulators.** Temperature stabilisation, attitude control, queueing-network
smoothing all map to a quadratic-impact problem with a single state.
* **Building block for higher-dimensional MPC.** Vector generalisations of :math:`h(t)` are matrix
Riccati ODEs; this scalar primitive is the verification kernel against which the matrix
solver in :doc:`matrix_riccati` is tested.
.. note::
📓 **Companion notebook**`view on GitHub <https://github.com/ThotDjehuty/optimiz-rs/blob/main/examples/notebooks/13_quadratic_impact.ipynb>`_
· `download .ipynb <https://raw.githubusercontent.com/ThotDjehuty/optimiz-rs/main/examples/notebooks/13_quadratic_impact.ipynb>`_
13 — Quadratic-impact controlled SDE
====================================
.. 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
Riccati fixed-point check
-------------------------
:math:`h'(t) = h(t)^2/γ - φ` with :math:`h(T) = A`. When :math:`γ = φ = A = 1` the right-hand side is :math:`h^2 - 1 = 0` at :math:`h = 1`, so `h ≡ 1`.
.. code-block:: python
res = opt.quadratic_impact_control_py(
gamma=1.0, phi=1.0, a_terminal=1.0,
t_horizon=0.5, n_steps=500,
)
tg = np.array(res['time_grid'])
h = np.array(res['h']); k = np.array(res['feedback_gain'])
print('h drift from 1:', float(np.max(np.abs(h - 1.0))))
.. code-block:: python
fig, ax = plt.subplots()
ax.plot(tg, h, label='h(t)')
ax.plot(tg, k, '--', label='k(t) = h(t)/γ')
ax.axhline(1.0, color='k', alpha=0.3, ls=':', label='fixed point')
ax.set_xlabel('t'); ax.legend(); ax.grid(alpha=0.3)
ax.set_title('Riccati fixed point γ=φ=A=1')
fig.tight_layout(); plt.show()
.. AUTO-PLOT-BEGIN
.. image:: ../_static/auto/algorithms__quadratic_impact_control/block_03_fig_01.png
:align: center
:width: 80%
.. AUTO-PLOT-END
.. image:: ../_static/v2/quadratic_impact_control/plot_01.png
:align: center
:width: 80%
Sensitivity to the terminal weight
----------------------------------
Vary :math:`A`, fix :math:`γ = 1`, :math:`φ = 0.25`, :math:`T = 1`.
.. code-block:: python
fig, ax = plt.subplots()
for A in [0.0, 0.25, 0.5, 1.0, 2.0, 5.0]:
r = opt.quadratic_impact_control_py(1.0, 0.25, A, 1.0, 1000)
ax.plot(r['time_grid'], r['h'], label=f'A = {A:g}')
ax.set_xlabel('t'); ax.set_ylabel('h(t)'); ax.legend(); ax.grid(alpha=0.3)
ax.set_title('Riccati sensitivity to terminal weight')
fig.tight_layout(); plt.show()
.. AUTO-PLOT-BEGIN
.. image:: ../_static/auto/algorithms__quadratic_impact_control/block_04_fig_01.png
:align: center
:width: 80%
.. AUTO-PLOT-END
.. image:: ../_static/v2/quadratic_impact_control/plot_02.png
:align: center
:width: 80%
**Verified:** `h ≡ 1` with `max|h - 1| < 1e-9` at the fixed point.
API
---
.. code-block:: rust
pub fn solve_quadratic_impact_control(cfg: &QuadraticImpactConfig) -> Result<QuadraticImpactResult>;
pub struct QuadraticImpactConfig { pub gamma: f64, pub phi: f64, pub a_terminal: f64, pub t_horizon: f64, pub n_steps: usize }
pub struct QuadraticImpactResult { pub time_grid: Array1<f64>, pub h: Array1<f64>, pub feedback_gain: Array1<f64> }