The Role of Hellinger Processes in Mathematical

This paper illustrates the natural role that Hellinger processes can play in solving problems from finance. We propose an extension of the concept of Hellinger process applicable to entropy distance and f -divergence distances, where f is a convex logarithmic function or a convex power function with general order q, 0 6= q < 1. These concepts lead to a new approach to Merton’s optimal portfolio problem and its dual in general Lévy markets.


Introduction
Merton's problem of finding the optimal investment strategy in a continuous-time securities market was proposed by Merton in 1969 ([18]).Using the technology of dynamic programming, he derived in [18] and [19] a non-linear PDE (Hamilton-Jacobi-Bellman equation) and produced explicit solutions for the cases of power, logarithmic and exponential utility function.Later on, the rich theory of martingales found its way into the problem, via the works of Harrison and Pliska [9], Karatzas et al [15] and Cox and Huang [2].In these works, the duality methodology of convex analysis combined with martingale technology to provide a powerful method to deal with this problem, e.g.[10], [15], [3], [16], [20].The main feature of the application of martingale technology to portfolio optimization is the derivation of the equivalent "dual problem", a minimization problem over the set of martingale measures.This latter is similar to the problem of choosing the appropriate martingale measure that one faces in the problem of pricing derivative securities in incomplete markets.In fact, the intimate relation between these two problems was established by Davis [4] by giving the investor an extremal objective in the form of a utility maximization problem.Indeed, Davis was the first to plug the derivative pricing problem for incomplete markets into a utility maximization framework to get a unique risk neutral measure (the "pricing measure").
In recent years, there has been increased activity in extending this framework to include more general models of securities.Papers which address processes of independent increments [8] and general semimartingales [16], [20] have all added to the framework.
In information theory (that part of probability theory which addresses the notion of distance between probability measures) there has been an upsurge of interest in the last decade in the concept of Hellinger processes and integrals.These processes arise from a dynamical approach to the Kakutani-Hellinger distance between two probability measures, see [12] and [17].The application of Hellinger processes in mathematical finance started with the work of [14].Very recently, [8] proposed the Hellinger martingale measure as an alternative to the minimal and optimal variance martingale measures for the case of processes with independent increments.In that paper, the pricing measure derived from a specific power-law utility (with exponent p = −1) is shown to be identical to the equivalent martingale measure which is nearest to the physical measure ("real-world measure") in the sense of the (q = 1/2) Hellinger distance.Thus, the paper shows a link between information theory and portfolio theory for a single example of utility function.
In the present paper, we strengthen the link between information theory and portfolio theory by demonstrating that Grandits' example can be extended to more general utility functions.Working in an exponential Lévy process market model, we show that for the most general power law utility, for the logarithmic utility, and for exponential utility, one can in each case define a process which possesses a number of properties similar to the Hellinger processes.Then the pricing measure in each case is shown to be identical to the equivalent martingale measure which minimizes the corresponding generalized Hellinger process.In the case of exponential utility, the corresponding pricing measure is the minimal entropy martingale measure which was introduced by Frittelli in [5], [6] (see also [1] for related works).
The organization of the paper is as follows.Section 2 introduces the exponential Lévy market model and provides some preliminary analysis.In section 3, we review Merton's problem and its dual formulation and give an economic interpretation for the solution to this problem.Section 4 reviews the definition of Hellinger processes and presents their defining properties.Our main contribution is in section 5, where we define examples of generalized Hellinger processes corresponding to the three types of utility functions mentioned above, and demonstrate their relation to Merton's problem and their desirable information theoretic properties.

The market model
We start with a filtered probability space (Ω, F, (F t ) 0≤t≤T , P ), a one-dimensional Brownian motion W and a one-dimensional Poisson random measure N (dt, dy) with Lévy measure ν(dy).The filtration is supposed to satisfy the usual conditions by which we mean right continuity and completeness i.e.F t = s>t F s and N ⊂ F 0 where N is the set of F-measurable and P -negligible events.We consider a financial market consisting of a risk-free asset (bank account) B given by where r > 0 is a constant interest rate and a stock S (risky asset).An ideal market is assumed in which transaction costs and liquidity effects are neglected and there are no limits on short-selling or borrowing.The stock process S is assumed to be governed by the following stochastic differential equation Here σ > 0, b are constants and N is the compensated Poisson random measure given by N (dt, dy) = N (dt, dy) − dt ν(dy).We have denoted the indicator functions I {y≤1} , I {y>1} by I ≤ , I > .We make two assumptions on the Lévy measure: Note the first condition is a strengthening of the general condition that 1 ∧ |y| 2 be integrable; the second condition is natural for a non-negative financial asset.
The discounted stock price B −1 t S t can be written as the Doléans-Dade exponential B −1 S = S 0 E(L) of the following Lévy process (stationary process with independent increments) (2.5) Here E(L) is the unique solution to the SDE dK = K − dL, K 0 = 1.As shown in [13], B −1 S can equivalently be expressed as the ordinary exponential S 0 exp(X) of a Lévy process with Lévy measure ν with supp(ν ) = (−∞, ∞).
We denote by M a , M e,loc and M e the spaces of all absolutely continuous local martingale measures, locally equivalent martingale measures and equivalent martingale measures respectively.The following proposition gives a representation of the density for the most general Q ∈ M a as the exponential of some (local) martingale with respect to the Brownian motion and the Poisson random measure.
Proposition 2.1 Let Q be a probability measure absolutely continuous with respect to P with conditional density Z t = E(dQ/dP |F t ).Then 1. Z can be written E(M ) for a (local) martingale of the form for a predictable W -integrable process β and non-negative P × B(IR)-measurable function Y (ω, t, y) (we will omit ω in the notation of β, Y and simply denote them by β t , Y t (y); recall P ⊂ F × B(IR + ) is the predictable σ-algebra) which satisfies almost surely for any T < ∞.
1.For details about this representation, we refer the reader to chapter III, section 4 of [12].
] is a P -local martingale and the result follows by direct calculation.
In this paper we will focus on two restricted families M a,det ⊂ M a,mark ⊂ M a of exponential martingales Z where "deterministic" martingales are defined by (2.6) with β = β(t), Y = Y (t, y) deterministic functions and "markovian" martingales are defined by (2.6) The set M a is not reduced to a singleton unless ν is zero.Indeed, (2.9) admits an infinite number of solutions: one martingale measure can be described by a second is given by ) is also a solution.By the fundamental theorem of arbitrage pricing [9] this implies that the market is incomplete and there exist payoffs (contingent claims) which cannot be perfectly replicated.One of the most important problems one faces in incomplete markets is which martingale measure to choose as pricing measure.Schweizer and Föllmer propose the minimal martingale measure [7], others propose the variance-optimal martingale measure [21].In general, however, the correct approach is via utility theory, a typical problem of which is the Merton problem.

The Merton problem
Consider an investor who wants to invest in their wealth in this market in an optimal way over the period [0, T ].Letting π t , 1 − π t be the fraction of wealth invested at time t in the stock and bank respectively and making the usual self-financing requirement (meaning no money is withdrawn from or added to the portfolio), then the wealth process X π,x t which follows from an initial endowment x = X 0 is given by The investor's tolerance of risk is quantified by a utility function U (x) which measures their pleasure experienced when the wealth is x.
Definition 3.1 A utility function U is a strictly increasing, strictly concave and twice continuously differentiable real valued function defined on IR + such that Remark.With the domain taken to be IR + = [0, ∞) we have placed an extra restriction that the portfolio value may never become negative.In one example discussed in §5 we will consider a utility function supported on IR.
The Merton problem for a given utility function U and initial wealth x is now to determine the strategy π * to be implemented over the investment horizon [0, T ] which maximizes the expected utility of the terminal wealth X π * T .Thus the Merton problem is to produce (if possible) the maximizer π * amongst admissible strategies A(0, x) for the problem We have used the definition Definition 3.2 A predictable process π is an "admissible trading strategy" over the period [t, T ] if X π,x is positive P-as.We denote the set of such processes by A(t, x).
To study (3.11) it is useful to consider a dynamical version of the problem defined by Then in the markovian setting as we have here, we are lead to study the HJB equation for u(t, x): As is now well known, the so-called "primal" problem (3.11) can also be addressed by focusing on the Legendre transform V of U defined by which is a strictly decreasing, strictly convex and twice differentiable function.Now one studies the "dual problem" When a minimal Z can be found for the dual problem, we can interpret it as the equivalent martingale measure (pricing measure) which captures the risk preferences coded into the utility function U .Furthermore, as shown in [16], the functions u(x) and v(y) can themselves be obtained from each other by using Legendre transform: In this paper, we will treat the cases of exponential, power and logarithmic utility.The extension to general semimartingales for these utility functions will require a careful treatment using stochastic calculus.The extension to general utility function is also possible and will be the focus of our future work.the q-Hellinger integral.The particular case q = 1/2 is related to the Kakutani-Hellinger distance ρ t between P and Q at time t: For q = 1/2, H (q) (P, Q) is not symmetric in P, Q; nonetheless it can be thought of as measuring the degree of separation between measures.
In the markovian case Z ∈ M a,mark it can be shown that h = h(t, Z t ) for a bivariate deterministic function and in the completely deterministic case Z ∈ M a,det h = h(t) is a deterministic increasing function of t alone.When Z ∈ M a,det note that the Hellinger integral is given by Now we consider the Merton problem for the power utility function U (x) = x p /p with p < 0. Its Legendre transform is given by V (y) = −y q /q, q = p p − 1 ∈ (0, 1).( For this utility, the dual Merton problem (3.15) can be rewritten in terms of the q-Hellinger integral: v(y) = −q −1 sup Q∈M a y q H (q) T (P, Q) (4.20) General theory implies that the optimizer for (4.20) in our Lévy market will be deterministic and thus can be found by solving Remark.The problem of (4.22) is solved independently for each value of t and determines (β, Y ) at that time.Thus we see that the optimal martingale measure is that which minimizes the relative rate of decrease of the Hellinger integral at every instant of time.Put another way, we see that the Hellinger process measures the rate that Q moves away from P , and the optimal martingale measure is that Q for which this rate is minimized at each instant of time.
A direct calculation using the generalized Ito formula [11] leads to an explicit formula for the Hellinger process 5 Generalized Hellinger processes We now show that much of the previous section remains true for more general concave functions of the density process Z t defined by the pair Q P .We consider the three important special cases of utility functions and their Legendre transforms: (1)

27)
Remark: The third is called the "'entropy" case : Note that in this case the domain of U is IR, and V is no longer a decreasing function.
We shall now define generalized Hellinger processes which correspond to these three utility functions.They are predictable increasing processes which can be written as the integral of a positive deterministic function when Z ∈ M a,det .Furthermore, exactly as in the previous section they lead to the solution of the deterministic dual problem (3.15) defined by the given utility function.
1. Case of q < 0: Now we notice that Z q is a positive sub-martingale which can be decomposed uniquely into Z q = Z q − • h (q) + martingale (5.28)where h (q) is an increasing predictable process we will call the q-Hellinger process of order q < 0. The explicit formula for h (q) is h [Y s (y) q − 1 − q(Y s (y) − 1)] ν(dy)ds, 0 ≤ t ≤ T (5.29) 2. Logarithmic case: Here there is a unique increasing predictable process we will call the log-Hellinger process, or h L , such that log Z = −h L + martingale (5.30) It is given by Proof.We need only reproduce the proof of Theorem 4.2

Conclusion
We have derived a number of examples of generalized Hellinger processes h t which have the interpretation that they measure an infinitesimal rate of separation of two measures Q and P .When applied to the financial problem of Merton, we see that the optimal pricing measure for a given utility function is that martingale measure Q for which the rate of separation given by the corresponding h t is minimized.