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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Survival Probability in the Life Annuity Insurance Model with Stochastic Return on Investments</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Tatiana A. Belkina</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Nadezhda B. Konyukhova</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Bohdan V. Slavko</string-name>
          <email>slavkobogdan@gmail.com</email>
          <xref ref-type="aff" rid="aff3">3</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Central Economics and Mathematics Institute of RAS</institution>
          ,
          <addr-line>Moscow</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Dorodnicyn Computing Center of RAS FRC CSC of RAS</institution>
          ,
          <addr-line>Moscow</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Higher School of Economics</institution>
          ,
          <addr-line>Moscow</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
        <aff id="aff3">
          <label>3</label>
          <institution>National Research University</institution>
        </aff>
      </contrib-group>
      <abstract>
        <p>We investigate the survival probability in the life annuity, or pension, insurance model when whole of the surplus (or a xed its part) is invested into a risky asset with the price following the geometric Brownian motion. For the case of exponential distribution of revenue sizes, we formulate a singular boundary value problem for linear integrodi erential equation and prove that the survival probability as a function of the initial surplus is the unique solution of this problem. Moreover, asymptotic representations for the survival probability both for small and large values of initial surplus are obtained. The e cient algorithm for the numerical calculation of the survival probability is described. Using computational experiments, we show that in the pension insurance business risky investments play a very important role in strengthening of the insurers solvency in a zone of small sizes of the surplus.</p>
      </abstract>
      <kwd-group>
        <kwd>life annuity insurance</kwd>
        <kwd>dual risk model</kwd>
        <kwd>survival probability</kwd>
        <kwd>investment</kwd>
        <kwd>risky asset</kwd>
        <kwd>geometric Brownian motion</kwd>
        <kwd>exponential distribution of revenue sizes</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>Introduction and Statement of the Problem
We consider the life annuity insurance model [9] (so called \dual risk model",
see, e. g., [2]), where the surplus or equity of a company (in the absence of
investments) is of the form</p>
      <p>Rt = u</p>
      <p>
        N(t)
ct + X Zk; t
k=1
0:
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
Here Rt is the surplus of a company at time t 0; u is the initial surplus, c is
the life annuity rate (or the pension payments per unit of time), assumed to be
deterministic and xed. N (t) is a homogeneous Poisson process with intensity
&gt; 0 that, for any t &gt; 0, determines the number of random revenues up to
the time t; Zk (k = 1; 2; : : : ) are independent identically distributed random
variables with a distribution function F (z) (F (0) = 0, EZ1 = m &lt; 1) that
determine the revenue sizes and are assumed to be independent of N (t). These
revenues arise at the moments of the death of policyholders.
      </p>
      <p>
        In comparison with the classical non-life collective risk model (so called
Cramer-Lundberg (CL) model, see [9]), the circumstances in (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) are reversed:
in the classical model second and third summands have opposite signs. Since
the \claims" in the dual model are negative (the jumps of the process (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) are
positive), this model is also called the insurance model with negative risk sums
or compound Poisson model with negative claims [3].
      </p>
      <p>Let now the whole surplus be continuously invested into risky asset with
price St following the geometric Brownian motion
dSt =</p>
    </sec>
    <sec id="sec-2">
      <title>Stdt +</title>
    </sec>
    <sec id="sec-3">
      <title>StdBt; t</title>
      <p>
        0;
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
where is the expected return rate, is the volatility, Bt is a standard Brownian
motion.
      </p>
      <p>Then the resulting surplus process Xt is governed by the equation
dXt =</p>
    </sec>
    <sec id="sec-4">
      <title>Xtdt +</title>
    </sec>
    <sec id="sec-5">
      <title>XtdBt + dRt; t</title>
      <p>
        0;
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
with the initial condition X0 = u, where Rt is de ned by (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ).
      </p>
      <p>
        Remark 1. For the case when only xed part of the surplus is invested into
risky asset while the rest part is invested into a risk free asset with xed return
rate, the equation (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is valued with modi ed parameters for the corresponding
surplus process (see, e. g., [4]).
      </p>
      <p>
        Denote '(u) = P (Xt 0; t 0) the survival probability (i. e., the
probability that bankruptcy will never happen); (u) = 1 '(u) is the ruin probability.
Let '0(u) = P (Rt 0; t 0) be the survival probability for the process (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
and 0(u) = 1 '0(u) be the corresponding ruin probability (in the absence of
investments).
      </p>
      <p>For the case of exponential distribution of revenue sizes, the following
theorem is proved in [10].</p>
      <p>
        Theorem 1. Let F (z) = 1 e z=m, m &gt; 0, := 2 = 2 1. Then:
1) if &gt; 0 then (u) = Ku (1 + o(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )); u ! 1, for some K &gt; 0;
2) if 0 then (u) = 1 for any u.
      </p>
      <p>The formulation of this theorem is exactly the same as in [8], [14] for the
non-life insurance model.</p>
      <p>For the ruin probability 0(u), it is easy to obtain an integro-di erential
equation (IDE) using the obvious modi cations of the \di erential argument" (see,
e. g., [9]). In the case of exponential distribution of revenue sizes and if the safety
loading is positive, i. e., the inequality m &gt; c is valid, this IDE has an exact
solution satisfying boundary conditions limu!+0 0(u) = 1, limu!1 0(u) = 0;
this solution has the form
0(u) = exp f ( =c
1=m)ug :</p>
      <p>
        Such slow decay as in Theorem 1 is in contrast with the exponential
representation (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) in corresponding model without investment. This fact leads to
the following conclusion, which has been made earlier for various models with
non-heavy-tailed distributions of claims: investment of the whole surplus into
risky assets in a zone of large values of the surplus impair the insurers solvency.
The same conclusion remains true when only xed part of the surplus is invested
into risky assets (so called simple investment strategies), see [4] and references
therein.
      </p>
      <p>At the same time, the studies of optimal investment strategies, which
maximize the survival probabilities in various settings of a problem for the CL model,
show that the risky assets play a crucial role in strengthening of the insurer's
solvency in a zone of small sizes of the surplus (see, e. g., [5] and references
therein). The same conclusions concern the simple investment strategies for CL
model and some its modi cations, see [6].</p>
      <p>The main goal of our paper is to identify the impact of simple investment
strategies on the solvency in the dual risk model not only in the case of large
surplus levels but also in the case of its small levels. For this purpose, we use the
approach based on so called su ciency theorems [4], which state that the
solutions of singular problems for linear IDEs, generated by in nitesimal operators
of the resulting surplus processes, de ne the corresponding survival
probabilities. This approach is rather di erent from the one used in [10] and eliminates
the need a priory to prove the twice continuously di erentiability of the survival
probability as well as the justi cation of boundary conditions. Solving the
singular problem for IDE, we calculate the survival probability as a function of the
initial surplus on the whole nonnegative semi-axis by means of the proposed
algorithm; some results of numerical experiments are described. These results allow
us to make conclusions about impact of the simple risky investment strategies
on the solvency in the life annuity insurance model.
2</p>
      <sec id="sec-5-1">
        <title>Some Preliminary Results</title>
        <p>
          Recall at rst that the in nitesimal generator A (see, e. g., [11]) of the process
Xt de ned by (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) has the form
(Af )(u) = 1 2u2f 00(u) + f 0(u)( u
2
c)
f (u) +
        </p>
        <p>
          Z 1
0
f (u + z) dF (z); (
          <xref ref-type="bibr" rid="ref5">5</xref>
          )
for any function f from a certain subclass D of the space C2(IR+) of real-valued,
twice continuously di erentiable on (0; 1) functions.
        </p>
        <p>In the assumption '(u) 2 D, where '(u) is the survival probability of the
process Xt, some considerations based on the generalized Ito's formula and the
complete probability formula allow us to write the following equation for u &gt; 0:
(A')(u) = 0
(6)
(see [10]; for the corresponding equation in the CL model with stochastic return
on investment, see, e. g., [13]).</p>
        <p>
          For the case of exponential distribution of revenue sizes, namely when
As noted in [10], the life annuity insurance case is rather di erent from the
nonlife insurance one because the change of two signs to the opposite ones in the
equation de ning the dynamics of the reserve leads to technical complications. In
contrast to the non-life insurance case, the risk process (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) may leave the positive
half-axis only in a continuous way. In [10] it was emphasized that the main
di culty in deriving the IDE is to prove the smoothness of the ruin probability.
The other di culty is to establish lower and upper asymptotic bounds for ruin
probability in order to identify boundary conditions at in nity for the survival
probability as the solution of the IDE. The smoothness of the ruin probability
is studied in [10] using a method based on integral representations; as a tool for
the proof of the asymptotic bounds for the ruin probability some theorems of
the renewal theory are used.
        </p>
        <p>As mentioned above in the introduction, in this paper we apply the approach
based on su ciency theorems (developed in [4] for the CL model and its
modi cation with stochastic premiums; see also the earlier paper [13]) which allows
us to avoid the a-priori proof of the the smoothness of the ruin probability as
well as the justi cation of the boundary conditions at in nity.</p>
        <p>For this purpose, we need a few preliminary propositions.</p>
        <p>
          Lemma 1. For the survival probability '(u) of the process (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) with the initial
condition X0 = u, the following relation is valid:
'(0) = 0;
(10)
i. e., the ruin occurs immediately at zero initial surplus.
        </p>
        <p>The proof of this lemma is obvious due to the negativity of the deterministic
component and we omit it. We provide below several statements concerning the
properties of the solutions to IDE (8) satisfying the various conditions.
Lemma 2. Let in IDE (8) the parameters c, , , m be xed positive numbers
and is arbitrary xed number. Then if there exists a solution '(u) to IDE (8)
with conditions
lim '(u) = 0;
u!+0
lim '(u) = 1;
u!1
then this solution is unique.</p>
        <p>This lemma can be easily proved by contradiction using the linearity of IDE.</p>
        <p>To formulate some further auxiliary propositions, we will use also the
following limiting conditions:
ul!im+0 j'0(u)j &lt; 1;
lim u'00(u) = 0:
u!+0
lim u'0(u) = 0;
u!1
lim u2'00(u) = 0:
u!1
Lemma 3. Let in IDE (8) the parameters c, , , m be xed positive numbers
and is arbitrary xed number. If there exists the solution '(u) of IDE (8),
satisfying conditions (11), (12), then
(11)
(12)
(13)
(14)
(15)
(16)
1 2u2'000(u) +
2
u +
2u
c</p>
        <p>'00(u) +
1
2m
2u2
+
de ned on IR+, with conditions (11){(13).
u
m
c</p>
        <p>'0(u) = 0; (17)
0
'(u)
1;
moreover,
The rst part of this statement may be proved by contradiction (see the proof of
a similar assertion in [6]). Let us prove the second part of the statement. Indeed,
from the IDE (8) and conditions (11) and (12) we have the relation</p>
        <p>Z 1
m 0
wherefrom, taking into account the proved above relation (14), the conditions (11)
and positiveness of c and other parameters, we conclude that (15) is valid.</p>
        <p>The following lemma is essential auxiliary statement for further study of
the initial problem.</p>
        <p>Lemma 4. Let in IDE (8) all the parameters c, , , m be xed positive
numbers. Then the singular IDE problem (8), (11){(13) is equivalent to the singular
problem for ODE
Proof. Let '(u) be satisfying IDE (8). Let us show that it satis es also ODE (17).
It is easy to check that, for the operator (9), the following relation is valid:
d
du
1 2u2'000(u) + 2u'00(u) + ( u
2
The obvious linear combination of IDEs (8) and (19), which exclude the integral
term (Jm')(u), leads to ODE (17).</p>
        <p>Conversely, let now '^(u) be satisfying ODE (17) and conditions (11) and (13).
Let us show that it satis es also the IDE (8). Denote g(u) the left-hand side of
the equation (8) with function '^(u). Then
g(u) =
'^(u) + (Jm'^)(u) + ( u
c)'^0(u) + 1 2u2'^00(u);
2
g0(u) =
[(Jm'^)(u)</p>
        <p>'^(u)] + (
Hence,
g0(u)
m
g(u)
m
=</p>
        <p>)'^0(u) +
+ ( u + 2u
c)'^00(u) + 1 2u2'^000(u):</p>
        <p>2
1
2m
2u2 '^00(u) + 1 2u2'^000(u);
2
and, in view of the fact that the function '^(u) is a solution of ODE (17), we
obtain</p>
        <p>The solution of ODE (20) has the form
u c
m</p>
        <p>'^0(u) +
+
u + 2u c
g0(u)
g(u)
m</p>
        <p>= 0:
g(u) = C exp (u=m); u &gt; 0;
where C is an arbitrary constant. It is easy to see that for the function '^(u),
which satis es conditions (11) and (13), the following relation is valid:
lim
u!+1 m u
1 Z 1
'^(s) exp ( (s
u)=m)ds = 1:
(20)
(21)
Then, taking into account the de nition of g(u), equality (22) and conditions (11),
(13) we conclude that the equality limu!1 g(u) = 0 holds. Consequently, in view
of positiveness m, the constant C in (21) should be equal to zero for this solution,
i. e., g(u) 0. Thus, '^(u) is the solution of IDE (8).</p>
        <p>It remains to note that the whole set of conditions is the same for the two
considered problems for IDE and ODE, and lemma is proved.</p>
        <p>To establish a connection between the original problem of the survival
probability investigation and a singular problem for IDE, we need also the following
statement which we call the su ciency theorem [4].</p>
        <p>Theorem 2. Let in IDE (8) all the parameters be positive numbers and the
inequality</p>
        <p>2 &gt; 2
be ful lled. Suppose IDE (8) has a twice continuously di erentiable on (0; 1)
solution '(u) subject to conditions
0
'(u)
1;
The proof of this theorem is completely analogous to the proof of Theorem 3.1
in [4].
3</p>
      </sec>
      <sec id="sec-5-2">
        <title>Main Theorem</title>
        <p>For the considered case of the exponential distribution of revenue sizes, we
establish the following statement.</p>
        <p>Theorem 3. Let F (z) be of the form (7), all the parameters , 2, m, c, be
xed positive constants, and let the condition (23) be satis ed. Then the following
assertions hold:</p>
        <p>
          (I) the survival probability '(u) of the process (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) with initial condition
X0 = u is the solution to the singular boundary value IDE problem (8), (11);
(II) this solution is unique and satis es the following relations:
0
'(u)
1;
(23)
(24)
(25)
(26)
(27)
(28)
where
and
        </p>
        <p>0
(IV) '(u) has the asymptotic representations
ul!im+0 j (u)j &lt; 1;
lim u (u) = 0;
u!1
lim u 0(u) = 0;
u!+0
lim u2 0(u) = 0;
u!1
Z 1</p>
        <p>(s)ds = 1;
'(u)</p>
        <p>D1</p>
        <p>1 !
u + X Dkuk=k ;
k=2
u
+0;
D1 = '0(+0);
D2 = (
D3 =</p>
        <p>D2(2 +
+ c=m) =c;
2
+ c=m)</p>
        <p>=m =(2c);
Dk+1 = [Dk(k(k
1) 2=2 + k
+ c=m)
where (u) = '0(u) is the solution of the following singular problem for ODE:
where K &gt; 0 is a constant;</p>
        <p>
          (V) as u ! +0, the behavior of the survival probability derivatives depends
on the relations between the parameters, in particular on a sign of the coe cient
ir = ( )m c: (
          <xref ref-type="bibr" rid="ref1">1</xref>
          ) if ir 0, then limu!+0 '00(u) 0, moreover, the solution
' is concave on IR+; (
          <xref ref-type="bibr" rid="ref2">2</xref>
          ) if ir &lt; 0, then limu!+0 '00(u) &gt; 0, the solution ' is
convex in a some neighborhood of zero and has an in exion point.
        </p>
        <p>Sketch of the proof. At rst, we need to establish the existence and uniqueness
of the solution to the problem (29){(32) and to study its asymptotic behaviors
for large and small values of u. For this purpose, we have to investigate the
singular problems (29), (30) and (29), (31) separately, taking into account that
ODE (28) has irregular singular points at zero and in nity (about singular points
for ODEs see, e. g. [15]).</p>
        <p>By using methods of the investigation of ODEs with singular points [15],
[12] we obtain asymptotic representation for families of solutions to this
singular problems (see also [6] and references therein for analogous investigation
(30)
(31)
(32)
(33)
(34)
(35)
(36)
(37)
with application of these methods for CL model with investment in details). As
result we have that ODE (29) for small u &gt; 0 has a two-parameter family of
solutions (u; D1; C1) and for these solutions the following asymptotic
representation holds:
(u; D1; C1) =
= D1 (1 +
1(u)) + C1 exp
2c=( 2u) u 2 = 2 (1 +</p>
        <p>
          2(u));
+0, the function
u
+0;
u ! 0: (38)
1(u) can be
(39)
Here C1 is a parameter, 2(u) = o(
          <xref ref-type="bibr" rid="ref1">1</xref>
          ), u !
represented by asymptotic series
where the coe cients Dk, k = 2; 3; : : : , may be found from the recurrence
relations (34){(36).
        </p>
        <p>It is obvious that the conditions (30) hold for all the solutions of the family
(u; D1; C1), i. e., for all the solutions to ODE (29).</p>
        <p>
          Under condition (23), ODE (29) has a one-parameter family of solutions
(u; C2) which are integrable at in nity. For these solutions, the following
asymptotic representation holds as u ! 1:
(u; C2) = C2u 2 = 2 (1 + o(
          <xref ref-type="bibr" rid="ref1">1</xref>
          ));
0(u; C2) =
        </p>
        <p>
          C2u 2 = 2 (1 + o(
          <xref ref-type="bibr" rid="ref1">1</xref>
          )): (40)
2
2u
It is obvious that the conditions (31) hold for all solutions of this family (i. e.,
for all integrable at in nity solutions of (29)) i the condition (23) is ful lled.
        </p>
        <p>
          Thus, if the condition (23) is ful lled, then there exists one-parameter
family of solutions to the problem (29)-(31). All the solutions of the equation (29)
are bounded at zero, and all bounded and integrable at in nity solutions
belong to this family and have the asymptotic representations (38) and (40). The
condition (32) extracts the unique solution from this family. It is clear that
this solution satis es the conditions (30) and (31). Then, taking into account
Lemma 4, it is easy to see that the function '(u) de ned by the formula (28)
is the solution to the IDE problem (8), (11){(13) and has the asymptotic
representations (33) and (37). Therefore, according to Lemma 3, the relations (14)
also hold and, in view of Theorem 2, for any u 2 IR+, the value of '(u) is the
survival probability for the process (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) with initial state X0 = u. In accordance
to Lemma 2 (about the uniqueness) this probability as a function of u satis es
conditions (12) and (13) with necessity. In view of Lemma 3, we have also that
the inequalities (15) take place, and, in accordance to the asymptotic
representation (33), we conclude that '00(+0) and the expression + c=m are of the
same sign. The sketch of the proof is completed.
4
        </p>
      </sec>
      <sec id="sec-5-3">
        <title>Numerical Examples</title>
        <p>The studies given in previous sections allow us to suggest computationally simple
and theoretically justi ed algorithm for numerical calculation of the survival
probability in the considered model. This algorithm requires to solve the singular
Cauchy problem from in nity (29), (31) with the normalizing condition (32).
Then it remains to use the relation (28) (recall that all the solutions of ODE (29)
are bounded as u ! +0 and all the integrable at in nity solutions form the
one-parameter family). To solve numerically the problem (29), (31) we realize
previously the equivalent transfer of the limit conditions (31) from in nity to
a large nite point using the results [7], [12]. For the rst approximation, such
approach yields boundary condition at a nite point u = u1 1 as follows
2
2u1
(u1)
(the same relation follows also from (40)).</p>
        <p>For general ODE systems with pole-type singular points, the theory of
boundary condition transfer from singular points is developed; such transfer can be
realized by construction of the stable initial manifolds, or the Lyapunov manifolds
of conventional stability, at the neighborhoods of singular points (see, e. g., [1]
and references therein). On the application of such approach in actuarial
mathematics, see [6] and references therein.</p>
        <p>
          Numerical experiments (see in particular Figs. 1, 2) show that risky
investments improves survival probability at a zone of small values of initial surplus
in the case of positive safety loading (Fig. 2). Moreover, risky investments make
survival possible in the case of negative safety loading, see Fig. 1 (in this case
survival is impossible without investments).
To study the impact of investments with stochastic return on survival
probability in the life annuity insurance model we use the approach based on so called
su ciency theorem and the existence theorems for the corresponding singular
problems for IDEs (see [4]). This uni ed approach eliminates need to proof
regularity of the survival probability as well as to use its upper and lower bounds.
Moreover, the solving of above singular problem for IDE leads to calculation of
the survival probability on all the non-negative semi-axis. We reduce the
problem (8), (11) to a certain initial problem from in nity for some second order
ODE with respect to the derivative of the survival probability with normalizing
condition. As a result of calculations, we conclude in particular that if the value
of safety loading ( m c) in the model (
          <xref ref-type="bibr" rid="ref1">1</xref>
          ) is negative or su ciently small and
the surplus is small too, then the use of the risky investments allows to increase
the survival probability signi cantly.
6. Belkina, T.A., Konyukhova, N.B., Kurochkin, S.V.: Dynamical insurance models
with investment: Constraint singular problems for integro-di erential equations.
        </p>
        <p>
          Comput. Math. Math. Phys. 56(
          <xref ref-type="bibr" rid="ref1">1</xref>
          ), 47-98 (2016)
7. Birger, E.S., Lyalikova, N.B.: Discovery of the solutions of certain systems of
differential equations with a given condition at in nity, I. U.S.S.R. Comput. Maths.
Math. Phys. 5(6), 1{17 (1965); On nding the solutions for a given condition at
in nity of certain systems of ordinary di erential equations, II. U.S.S.R. Comput.
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