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