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Necessary and Sufficient Conditions for the Uniform Integrability of the Stochastic Exponential

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Abstract

We establish necessary and sufficient conditions for uniform integrability of the stochastic exponential \({{{\mathcal {E}}}}(M)\), where M is a continuous local martingale.

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References

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Acknowledgements

I am very grateful to unknown referees for very helpful and important comments.

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Appendix

Appendix

Here we introduce four important lemmas with proofs. These lemmas are essential in the proof of Theorems 1 and 2.

Lemma 1

Let \(f:[0;+\infty ) \rightarrow (0; +\infty )\) be a non-decreasing function with \(\lim _{x\rightarrow \infty }f(x) = \infty \). Then, a non-decreasing, absolutely continuous function \(g:[0;+\infty ) \rightarrow [0; +\infty )\) exists which satisfies the following conditions:

  1. (a)

    \(g(x)\le f(x)\);

  2. (b)

    \(\lim _{x\rightarrow \infty }g(x) = \infty \);

  3. (c)

    \(g(x+y)\le g(x)+y+2\).

Proof

Define the function F: \(F(x) = \sum ^{\infty }_{k=1}f(k-1)1_{[k-1; k[}(x)\). It is obvious that \(F(x)\le f(x)\). Let us denote by \(\bigtriangleup F(k)=F(k)-F(k-1)\) the jumps of F. Because f is non-decreasing, the jumps of F will be nonnegative. Now define a non-decreasing sequence \((g_k)_{k\ge 1}\) through the recurrence relationship:

$$\begin{aligned} g_0=0; \, g_1=1\wedge f(0); \, g_2=g_1+(1\wedge \bigtriangleup F(1)); \, g_k = g_{k-1}+(1\wedge \bigtriangleup F(k-1)) \,\, k\ge 2. \end{aligned}$$

As a result, we have points \((k; g_k), \,\,\, k\ge 0\). Define function g by connecting points \((k; g_k)\) with straight lines. It follows from the definition that g is absolutely continuous, non-decreasing, \(g(x)\le F(x) \le f(x)\) and \(\lim _{x\rightarrow \infty }g(x) = \infty \). It remains to show that \(g(x+y)\le g(x)+y+2\). Let us take \(x\in [k-1;k[\) and \(y\in [n-1;n[\). It is clear that \(x+y \le k+n\). Using the definition of the function g, we obtain:

$$\begin{aligned} g(x+y)-g(x)\le g(k+n)-g(k-1)&= \sum _{i=1}^{k+n}1\wedge \bigtriangleup F(i-1) - \sum _{i=1}^{k-1}1\wedge \bigtriangleup F(i-1) = \\&\quad = \sum _{i=k}^{k+n}1\wedge \bigtriangleup F(i-1) \le n+1 \le y+2. \end{aligned}$$

So, by arbitrariness of k and n, \(g(x+y)\le g(x)+y+2\). \(\square \)

Lemma 2

For any random variable \(\xi \) such that \(P(0\le \xi < \infty )=1\) there exists a positive, non-decreasing and continuous function g with \(\lim _{x\rightarrow \infty }g(x) = \infty \), such that \(Eg(\xi ) < \infty \).

Proof

If \(\xi \) is a bounded random variable, then the proof of Lemma 2 is trivial, so we can consider only the case when \(\xi \) is unbounded. In this case, \(F_{\xi }(x)<1\) for any \(x\in [0;+\infty )\) where \(F_{\xi }(x) = P(\xi \le x)\) is the probability distribution function of \(\xi \). Let us take \(f(x)=\frac{1}{\sqrt{1 - F_{\xi }(x-)}}\). Then we will have:

$$\begin{aligned} Ef(\xi )&= \int ^{\infty }_0 \frac{1}{\sqrt{1 - F_{\xi }(x-)}} {\text {d}}F_{\xi }(x) = \bigg [ -2\sqrt{1-F_{\xi }(x)} \bigg ]^{\infty }_0 \\&\quad - \sum _{0<x<\infty }\Big [ -2\sqrt{1-F_{\xi }(x)} + 2\sqrt{1-F_{\xi }(x-)}-\frac{\Delta F_{\xi }(x)}{\sqrt{1-F_{\xi }(x-)}} \Big ] \\&\quad \le \bigg [ -2\sqrt{1-F_{\xi }(x)} \bigg ]^{\infty }_0 = 2\sqrt{1-F_{\xi }(0)} < \infty . \end{aligned}$$

Here we have used the inequality \(-2\sqrt{1-F_{\xi }(x)} + 2\sqrt{1-F_{\xi }(x-)}-\frac{\Delta F_{\xi }(x)}{\sqrt{1-F_{\xi }(x-)}} \ge 0\), which follows from the convexity of the function \(y \rightarrow -2\sqrt{1-y}\). Now if we use Lemma 1, we can find an absolutely continuous, positive and non-decreasing function g with \(\lim _{x\rightarrow \infty }g(x) = \infty \), such that \(g(x)\le f(x)\). The inequalities \(g(x)\le f(x)\) and \(Ef(\xi ) < \infty \) imply that \(Eg(\xi ) < \infty \). \(\square \)

Lemma 3

Let \(\varphi \) be a lower function. Then, the function \(\psi (x)=\varepsilon \varphi (\frac{x}{\varepsilon ^2})\) will be a lower function, too.

Proof

It is well known that if \(B_t\) is a Brownian motion, then \(W_t = \varepsilon B_{t/\varepsilon ^2}\) will be Brownian motion, too. With this if we take \(s=t/\varepsilon ^2\), then we will have:

$$\begin{aligned}&P \Big \{ \omega \,\, : \,\, \exists \, t(\omega ), \, W_t< \psi (t) \,\,\, \forall \, t>t(\omega ) \Big \} \\&\quad = P \Big \{ \omega \,\, : \,\, \exists \, s(\omega ), \, B_s < \varphi (s) \,\,\, \forall \, s>s(\omega ) \Big \} = 0. \end{aligned}$$

\(\square \)

Lemma 4

For any \(\varepsilon >0\), there exists \(\delta > 0\) sufficiently close to 0 such that the inequality \(\delta x^2 + \delta \varepsilon \le \frac{1}{2}(x-1)^2\) holds true for any \(x \notin (1-\varepsilon ; 1+\varepsilon )\).

Proof

It is clear that we can take \(\delta >0\) sufficiently close to 0 such that

$$\begin{aligned} 1-\varepsilon< \frac{1-\sqrt{2\delta (1+\varepsilon -2\delta \varepsilon )}}{1-2\delta }< \frac{1+\sqrt{2\delta (1+\varepsilon -2\delta \varepsilon )}}{1-2\delta } < 1+\varepsilon . \end{aligned}$$

It is easy to check that for such \(\delta \) the condition \(|x-1|\ge \varepsilon \) implies the inequality

$$\begin{aligned} (1-2\delta )x^2 - 2x + 1-2\delta \varepsilon \ge 0 \end{aligned}$$

which is equivalent to \(\delta x^2 + \delta \varepsilon \le \frac{1}{2}(x-1)^2\). \(\square \)

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Chikvinidze, B. Necessary and Sufficient Conditions for the Uniform Integrability of the Stochastic Exponential. J Theor Probab 35, 282–294 (2022). https://doi.org/10.1007/s10959-020-01047-4

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