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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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:
-
(a)
\(g(x)\le f(x)\);
-
(b)
\(\lim _{x\rightarrow \infty }g(x) = \infty \);
-
(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:
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:
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:
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:
\(\square \)
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
It is easy to check that for such \(\delta \) the condition \(|x-1|\ge \varepsilon \) implies the inequality
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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DOI: https://doi.org/10.1007/s10959-020-01047-4