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Part of the book series: Communications and Control Engineering ((CCE))

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Abstract

In this chapter, we show that the degenerate points may separate the state space into different regions for multiple classes, and we discuss the optimization of multi-class degenerate diffusion processes. We also show that under some conditions, the performance function of finite-horizon optimization problems, or the potential function of the long-run average optimization problems, is semi-smooth at degenerate points and smooth at non-degenerate points. Thus, degenerate points coincide with semi-smooth points. Furthermore, there are some special features at the degenerate points: the local time at these points are zero, and the process can only move toward one direction. Therefore, the effect of semi-smoothness of a function can be ignored at these degenerate points in the Ito-Tanaka formula. With these special features in consideration, various optimization problems such as long-run average, finite-horizon, optimal stopping, and singular control, become simpler.

The formulation of a problem is often more essential than its solution, which may be merely a matter of mathematical or experimental skills [1].

Albert Einstein

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Notes

  1. 1.

    These follow naturally from the Lipschitz condition.

  2. 2.

    The lemma may follow directly from Theorem 2.2 by the confluencity of the process in \(( - \infty , 0]\).

  3. 3.

    More w-ergodic classes may be reached for multidimensional processes.

  4. 4.

    Since our derivation holds if [0, 1] is changed to [0, c] for any \(c>0\), this condition is equivalent to f(x) bounded in a neighborhood of 0, [0, c], for a \(c>0\).

  5. 5.

    Under these conditions, the Lipschitz condition (3.9) holds in [a, b].

  6. 6.

    Also called an antiderivative, \(h(x) := \int f(x)dx \) is defined as any function with \( \dot{h}(x) = f(x)\).

  7. 7.

    Note the difference between \(\dot{\varPsi } (0_- )\) and \(\dot{\varPsi }_- (0)\).

  8. 8.

    One needs to verify that both the denominator and numerator in H(x) at \(x=0\) are zero or infinite. This is true depending on \(\mu (0_\pm ) >0\) or \(<0\), as shown in the term \(\frac{2 \mu (x)}{\sigma ^2(x)}\) in the exponential. We will not go into the details.

  9. 9.

    This proof applies to both cases with \(f(x) \not \equiv 0\) and \(f(x)\equiv 0\).

  10. 10.

    These conditions are weaker than those in Lemma 4.5.

  11. 11.

    In finite-horizon problems with (4.13), the potential function is the same as the performance measure \(\eta (x)\); however, in the infinite-horizon long-run average problem, they are different, i.e., \(\eta (x) \ne g(x)\). A potential function is the solution to a Poisson equation.

  12. 12.

    Note for long-run average, the potential function g(x) in Theorem 4.3 is different from the performance function \(\eta (x)\).

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Cao, XR. (2020). Degenerate Diffusion Processes. In: Relative Optimization of Continuous-Time and Continuous-State Stochastic Systems. Communications and Control Engineering. Springer, Cham. https://doi.org/10.1007/978-3-030-41846-5_4

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