Abstract
The paper presents exact formulae related to the distribution of the first passage time τx of the jump-telegraph process. In particular, the Laplace transform of τx is analysed, when a jump component is in the opposite direction to the crossing level x > 0. The case of double exponential jumps is also studied in detail.
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Appendix: Conditions determining appearance of conjugate complex roots
Appendix: Conditions determining appearance of conjugate complex roots
Consider the compound Poisson process with constant drift, \(X(t)=ct+{\sum }_{n = 1}^{N(t)}Y_{n},\) where N(t) is a homogeneous Poisson process with parameter λ,λ > 0; {Yn}n≥ 1 are independent identically distributed random jumps. For simplicity, we assume that Yn has the symmetric Laplace distribution with the density function \(h(y)=\dfrac 12 b\exp (-b|y|), b>0\).
In this particular case, Eq. 3.9 is equivalent to the pair of equations:
Let c > 0 (the case c < 0 can be analysed similarly). Since for q > 0
and c > 0, all three roots of the first equation of (A.1) are always real: one negative and two positive, see Fig. 10.
The second equation of (A.1) is equivalent to
This equation always has one negative root. The other two roots are real positive if and only if function f(α) has a negative local minimum, minα> 0f(α) < 0, which is taken at the stationary point
After the tedious algebra, one can see that the inequality minα> 0f(α) < 0 is equivalent to
where α∗ is defined by (A.3).
Note that condition (A.4) fails when b = (λ + q)/c, see Fig. 11.
If b≠(λ + q)/c, then (A.4) is valid only when the trend c is far from (λ + q)/b. More precisely, if c↓ 0, then α∗↑ +∞, in such a way that \(c\alpha _{*}\downarrow \dfrac 23(\lambda +q),\) which ensures (A.4) for a small c > 0. In contrast, if c → +∞, then \(\alpha _{*}\to b/\sqrt {3}\), which again gives (A.4) for a sufficiently large trend c.
See Fig. 11: in case (1) (0 < c ≪ (λ + q)/b) and in case (3) (c ≫ (λ + q)/b) we have two positive real roots; case (2) with moderate c corresponds to two conjugate complex roots with a positive real part.
Consider another example. Let c1 = −c2 = c > 0 and the jump part is the same. In this case, Eq. 3.29 becomes
Note that
Hence, Eq. A.5 always has at least one positive real root, see Fig. 12.
Equation A.5 has two additional positive real roots if and only if there exists α > b such that
see Fig. 12 (dashed parabola (λ + q)2 − c2α2 with small c which corresponds to three real positive roots). Otherwise, Eq. A.5 has one real positive root and a pair of conjugate complex roots with positive real part.
Since, the point of local maximum of f(α),α > b, corresponds to
Equation A.5 has three real positive roots if the following relation holds:
which is equivalent to sufficiently small c,c < (λ + q)/b, such that
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Ratanov, N. First Crossing Times of Telegraph Processes with Jumps. Methodol Comput Appl Probab 22, 349–370 (2020). https://doi.org/10.1007/s11009-019-09709-5
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DOI: https://doi.org/10.1007/s11009-019-09709-5