Appendix A.1. Preliminary Elements
Consider a bidirectional stochastic process with stationary, independent increments and initial value . The bidirectional property requires that have positive probability of taking both negative and positive values. We also require process to have a cumulant generating function (c.g.f.) defined on an open interval which includes zero. We denote this c.g.f. by so, by definition, for . These assumptions for process imply that we are considering a subfamily of Lévy processes.
We let S denote the first hitting time of threshold by process . Thus, is the process level reached at the hitting time S. The excess is referred to as the overshoot of the process at the first hitting time. For notational convenience, we let D denote for some fixed time and V denote for . Furthermore, we denote the probability density function (p.d.f.) of D by . This p.d.f. notation reminds us of the conditioning on time t. We denote the conditional p.d.f. of D given by , the p.d.f. of the first hitting time S given by , and the p.d.f. of V by . If the process has no overshoot then and we take as a limiting density function concentrated on 0 (a Dirac delta function).
We will refer to as our primal process and its dual process by , where an asterisk subscript is used to designate properties of the dual process. The dual process has the same probability law as , that is, . So has c.g.f. defined for all . We are interested in the situation where the primal process has a positive mean parameter so that its dual process has a negative mean parameter . Sample paths of the primal process must eventually hit threshold so for its first hitting time S when . Sample paths of the dual process are not guaranteed to reach the threshold so for its first hitting time S.
A sample path of the primal process
either reaches level D at time
t without hitting threshold
during interval
or it does hit
at some time
and subsequently travels from
to
D in the interval
. This line of reasoning gives us the following probability identity connecting the mathematical constituents of this setting:
The corresponding probability identity for the dual process is:
Here the functions with asterisks are the corresponding entities for the dual process that are found in (
A1) for the primal process.
Appendix A.3. Evaluating Bundles of Sample Paths
The Esscher property provides Lévy processes with a remarkable feature. This feature is apparent if we consider discrete versions of the sample paths of our processes. Let be a sequence of levels of a sample path corresponding to ordered time points of the process . Here with and . Thus, the path experiences probabilistically independent increments of during time increments , for . We note that the partition of the path from the origin to at time can be as fine as desired for the analysis at hand.
With the Esscher property, the probability densities of the primal and dual processes for any path increment
i are related as follows:
where
and
denote the respective probability densities. It follows then that the probability densities of any given sample path
from 0 at time 0 to
at time
for the primal and dual processes are related by:
where
and
denote the respective probability densities for path
. The relationship in (
A9) shows that the probability densities of the primal and dual processes for any path
under the Esscher property are proportional, with the multiplier
being determined only by the cumulative vertical distance
travelled by the sample path
.
The result in (
A9) provides a mechanism for evaluating probabilities of different bundles or sets of sample paths for a stochastic process observed over a given time interval
. The mechanism visualizes discrete simulations of many sample paths for the process using a fixed partition of the time interval
. In particular, we consider the simulation of a set
of independent sample paths from the primal process where
denotes the probability density of a path
. If we are interested in estimating the probability of experiencing a simulated sample path that meets a specified condition
C then we sort through set
and keep only sample paths that meet the condition, resulting in a subset that we can denote by
. The probability density for this subset is therefore
.
We can exploit the correspondence of path densities in (
A9) to evaluate the relationships between corresponding terms in the probability identities (
A1) and (
A2). P.d.f.
, for example, is the probability density for the primal process of the set of sample paths that connect the origin to
at time
t, which we now denote by
. Using (
A9), we then have the following link between
and
for the primal and dual processes.
Next we consider the subset of
that contains sample paths that do not cross the threshold
in the interval
. We denote this subset by
. Using (
A9), we have the following link between the conditional p.d.f.s
and
for the primal and dual processes.
Note that probabilities and must be included to adjust for the condition that the first hitting time lies beyond t.
The density functions in the rightmost terms of (
A1) and (
A2) arise from sample paths that cross the threshold
in the interval
. The correspondence of these primal and dual densities is established as follows. Let subset
consist of paths that first cross the threshold
at a specified time
s in the interval
, experience an overshoot of
v, and then proceed to level
at time
t. So, again using (
A9), we have the following equation:
The distribution of process increment
does not depend on
for either the primal or dual processes. Therefore, when we integrate both sides of (
A12) with respect to
, the following integrals evaluate to 1:
Using this result, Equation (
A12) reduces to:
Of particular interest is the limit of (
A14) if we now let
t go to infinity. As a first hitting is inevitable for the primal process, we have
. For the dual process, a first hitting may not occur in finite time so the limiting probability
will be less than 1. Equation (
A14) therefore reduces to:
To proceed further, we will now separate processes according to whether they overshoot threshold or not when their sample paths first exit the threshold.
Appendix A.5. First Hitting Times with Overshoot
We next consider bidirectional Lévy processes with jump components that do overshoot thresholds. To deal with these processes, we reformulate the first hitting time of the process. Instead of having primal process
start at the origin with
, we let the process operate until it encounters its first positive level and shift the time origin to that position. We denote this initial positive level by
so
. To proceed, we return to a discrete version of the sample path for the re-scaled process
and consider a partition of time interval
, with equally spaced time points
where
and
. Let the successive levels
correspond to
, so
and
. We then consider the successive maxima
of the process, which starts with
. We define the successive increments in the maxima by
. Now we keep only positive increments
, discarding all
that are zero. These positive increments are necessarily independent and identically distributed. The increments mark out the vertical advance of the partitioned primal process from starting level
toward the failure threshold at
. We re-index the successive positive increments and denote them by
,
where
is the
nth positive increment in the sequence. It is evident that the set
is a sequence of
m renewal intervals for a delayed renewal process [
17]. The delay
in the process is, in effect, the overshoot of the zero-axis by the process in its first passage to that level.
Building on this formulation as a delayed renewal process, we denote the s.f. of the successive renewal intervals
by
. Next, we assume that the delayed renewal process is, in fact, in equilibrium so
is a random draw from the equilibrium c.d.f.:
where
denotes the mean of s.f.
. Parameter
is the mean vertical advance of the process whenever a positive advance occurs. With the assumption that the renewal process is in equilibrium, it follows therefore that
is also the c.d.f. of the overshoot that will be experienced when the primal process crosses threshold
. Moreover, the equilibrium condition implies that the overshoot c.d.f.
will be independent of the first hitting time
S of threshold
.
Finally, we consider the corresponding dual process which, of course, is also bidirectional with a jump component. The preceding line of development for constructing an equilibrium renewal process for advances toward the failure threshold at can be applied to the dual process. For the dual process, we denote the s.f. of the renewal interval by and the equilibrium c.d.f. for overshoot by .
We return now to Equation (
A14) and rearrange it into a product of ratios for matched terms as follows:
It can be seen that only the rightmost ratio on the left side of Equation (
A18) contains terms that are functions of overshoot
v. It follows therefore that this ratio cannot depend on
v although it may depend on survival time
s. Denoting this rightmost ratio by
, we have:
Now, however, we can add that if the primal process and dual processes are in equilibrium then the densities in (
A19) do not depend on
s and, hence,
equals some constant
Q for all
s. In this case, the two density functions in the ratio are those corresponding to c.d.f.s
and
, which we denote by
and
, respectively. Moreover, in this same equilibrium condition, it follows that the density functions
and
for the survival time
S of the primal and dual processes must be identical. Thus, the identity
is assured for all bidirectional Lévy processes with overshoot, provided survival time is measured from a time point where the process is in equilibrium. As a final consequence, we see that constant
so the probability that
S is finite is given by
. When the primal process has no overshoot, we have from (
A19) that
for all
s and, hence, the probability that
S is finite is given by
, a result we saw earlier.
An implication of adopting the equilibrium formulation for the overshoot case is that the first hitting time of will be immediate if . In other words, if the initial process maximum falls above threshold then and failure occurs at the outset. The survival function therefore has a probability mass at zero equal to .
Appendix A.6. Case Demonstrations
We now present case demonstrations of stochastic process families in which the primal and dual processes have the same survival distributions. We begin by looking at two families whose sample paths do not exhibit overshoot. We then consider an additional two families that do exhibit overshoot.
Cases with No Overshoot
As the primal process, consider a Wiener process
with mean parameter
and variance parameter
. Let
so
. The p.d.f. of
D is:
The c.g.f. for the process is:
which is defined for all real numbers
. As Wiener sample paths are continuous, we have no overshoot.
For dual process
,
and
. Also,
so:
It also can be verified that so the Esscher property holds.
The first hitting time
S of the primal and dual processes has the following inverse Gaussian c.g.f.:
As the primal process, consider a Poisson-Bernoulli random walk
defined by the following doubly stochastic process. Bernoulli events occur according to a Poisson process with rate parameter
and each Bernoulli event is either an up-step of
with probability
p or a down-step of
with probability
. Assume the event outcomes occur in a mutually independent fashion. We take the threshold
to be a natural number so there is no overshoot. The process therefore takes the following form:
Here denotes the Poisson process and denotes the binomial process for the number of up-step outcomes among the Bernoulli trials occurring during time interval .
The probability function of
for this process is evaluated by expanding the probability product
and then summing over all pairs
for which
, taking account of the condition that
for
. The result is the following form, which involves a tractable infinite series:
where
denotes an indicator function. A little mathematics gives the following c.g.f. for the process
:
which is defined for all real numbers
. The mean parameter is easily evaluated from this c.g.f. as
. To ensure a positive mean parameter, we set
.
The dual process
is obtained by simply interchanging
p and
, that is, by letting
. Again, for
,
, the process mean is
, and
so:
It also can be verified with a little algebra that the stochastic process has the Esscher property.
The first hitting time
S of the primal and dual processes has the following c.g.f.:
Cases with Overshoot
For both cases with overshoot, we consider bilateral processes that are created by taking the difference of independent monotonically non-decreasing jump processes with stationary independent increments.
As the primal process, consider a bilateral gamma process
, defined as the difference between two independent gamma processes
and
, as follows:
In the most general case, the processes may have different positive shape parameters
and different positive scale parameters
. This process has attracted some interest in financial mathematics [
18]. The general bilateral gamma process has c.g.f.:
The process mean is .
Equal shape parameters. The special case in which the component processes
and
share the same shape parameter, say,
provides a family of processes
for which
if
. The c.g.f. in (
A30) simplifies to:
It can be verified that the Esscher property
holds in this case with
. For this equal-shape case, a little algebra shows that the p.d.f. of
takes the following form:
It is noteworthy that the integral in (
A32) depends parametrically only on
and
.
Equal scale parameters. The counterpart of the equal-shape case is the equal-scale case in which the component processes
and
share the same scale parameter, say,
. In this case, the family of processes
have mean
if
. The c.g.f. in (
A30) simplifies to:
Quantity
U is the positive root (
) of the following equation:
For this equal-scale case, however, the Esscher property does not hold. We therefore do not pursue it further.
As the primal process, consider a bilateral inverse Gaussian process
, defined as the difference between two independent inverse Gaussian processes
and
, as follows:
In the most general case, the processes may have different positive scale parameters
and different positive shape parameters
. The general bilateral inverse Gaussian process has c.g.f.:
Equal shape parameters. The special case in which the component processes
and
share the same shape parameter, say,
provides a family of processes
for which
if
. The c.g.f. in (
A36) simplifies to:
It can be verified that the Esscher property holds in this case with .
Equal scale parameters. The counterpart of the equal-shape case is the equal-scale case in which the component processes and share the same scale parameter, say, . In this case, the family of processes have mean and, hence, do not fall into the class of processes that interest us here. Equation has only a single root at 0 in the interval so the Esscher property does not hold.