Ruin Probabilities in a Diffusion Environment Jan Grandell & - - PowerPoint PPT Presentation

ruin probabilities in a diffusion environment
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Ruin Probabilities in a Diffusion Environment Jan Grandell & - - PowerPoint PPT Presentation

Ruin Probabilities in a Diffusion Environment Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne New Frontiers in Applied Probability, Sandbjerg, 2nd of August Cox Models OrnsteinUhlenbeck Intensities


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Ruin Probabilities in a Diffusion Environment

Jan Grandell & Hanspeter Schmidli

KTH Stockholm & University of Cologne

New Frontiers in Applied Probability, Sandbjerg, 2nd of August

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

1

Cox Models

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

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Cox Models

2

Ornstein–Uhlenbeck Intensities

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

1

Cox Models

2

Ornstein–Uhlenbeck Intensities

3

Subexponential Claim Sizes

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

1

Cox Models

2

Ornstein–Uhlenbeck Intensities

3

Subexponential Claim Sizes

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital c: premium rate

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital c: premium rate {Nt}: A single point process

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital c: premium rate {Nt}: A single point process {Yi}: iid,

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital c: premium rate {Nt}: A single point process {Yi}: iid, independent of {Nt}

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital c: premium rate {Nt}: A single point process {Yi}: iid, independent of {Nt} G(y): distribution function of Yi, G(0) = 0

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Risk Model

Xt = x + ct −

Nt

  • i=1

Yi x: initial capital c: premium rate {Nt}: A single point process {Yi}: iid, independent of {Nt} G(y): distribution function of Yi, G(0) = 0 µn = I I E[Y n

i ],

µ = µ1, h(r) = I I E[erY − 1].

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Diffusion Intensities

Let {Zt} be a diffusion process following the stochastic differential equation dZt = b(Zt) dWt + a(Zt) dt for some Brownian motion {Wt}. We assume that there is a strong solution.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Diffusion Intensities

Let {Zt} be a diffusion process following the stochastic differential equation dZt = b(Zt) dWt + a(Zt) dt for some Brownian motion {Wt}. We assume that there is a strong solution. Let Λ(t) = t

0 ℓ(Zs) ds for some function ℓ. We define

N(t) = ˜ N(Λ(t)) , where {˜ Nt} is a Poisson process with rate 1.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Diffusion Intensities

Let {Zt} be a diffusion process following the stochastic differential equation dZt = b(Zt) dWt + a(Zt) dt for some Brownian motion {Wt}. We assume that there is a strong solution. Let Λ(t) = t

0 ℓ(Zs) ds for some function ℓ. We define

N(t) = ˜ N(Λ(t)) , where {˜ Nt} is a Poisson process with rate 1. Thus, given {Zt}, the claim number process {Nt} is conditionally an inhomogeneous Poisson process with rate {ℓ(Zt)}.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Martingale

The process M = {g(Zt)e−r(Xt−x)−θ(r)t} is a martingale if

1 2b2(z)g′′(z) + a(z)g′(z) + [ℓ(z)h(r) − θ − cr−]g(z) = 0 .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Martingale

The process M = {g(Zt)e−r(Xt−x)−θ(r)t} is a martingale if

1 2b2(z)g′′(z) + a(z)g′(z) + [ℓ(z)h(r) − θ − cr−]g(z) = 0 .

Suppose we found a solution with a positive g(z). This is only possible if θ = θ(r) depends on the important parameter r.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Martingale

The process M = {g(Zt)e−r(Xt−x)−θ(r)t} is a martingale if

1 2b2(z)g′′(z) + a(z)g′(z) + [ℓ(z)h(r) − θ − cr−]g(z) = 0 .

Suppose we found a solution with a positive g(z). This is only possible if θ = θ(r) depends on the important parameter r. We norm g, such that limt→∞ I I E[g(Zt)] = 1.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Consider the measure Q[A] = I I E[g(ZT)e−r(XT −x)−θ(r)T; A] I I E[g(Z0)] .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Consider the measure Q[A] = I I E[g(ZT)e−r(XT −x)−θ(r)T; A] I I E[g(Z0)] . The process ({Xt, Zt)} remains a Cox model with claim size distribution Q[Y ≤ x] = (h(r) + 1)−1 x ery dG(y) ,

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Consider the measure Q[A] = I I E[g(ZT)e−r(XT −x)−θ(r)T; A] I I E[g(Z0)] . The process ({Xt, Zt)} remains a Cox model with claim size distribution Q[Y ≤ x] = (h(r) + 1)−1 x ery dG(y) , claim intensity ℓ(Zt)(h(r) + 1),

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Consider the measure Q[A] = I I E[g(ZT)e−r(XT −x)−θ(r)T; A] I I E[g(Z0)] . The process ({Xt, Zt)} remains a Cox model with claim size distribution Q[Y ≤ x] = (h(r) + 1)−1 x ery dG(y) , claim intensity ℓ(Zt)(h(r) + 1), and generator of the diffusion ˜ Af = ga + b2g′ g f ′ + 1

2b2f ′′ .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Typically, the function θ(r) will be convex. Since I I EQ[Xt] = I I EII

P[Xtg(Zt)e−rXte−θ(r)t]

we have = d dr I I EII

P[g(Zt)e−rXte−θ(r)t]

= I I EII

P

d dr g(Zt)

  • e−rXte−θ(r)t

− I I EQ[Xt] − tθ′(r) .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Typically, the function θ(r) will be convex. Since I I EQ[Xt] = I I EII

P[Xtg(Zt)e−rXte−θ(r)t]

we have = d dr I I EII

P[g(Zt)e−rXte−θ(r)t]

= I I EII

P

d dr g(Zt)

  • e−rXte−θ(r)t

− I I EQ[Xt] − tθ′(r) . Typically, dividing by t and letting t → ∞, the first term will

  • vanish. Thus t−1I

I EQ[Xt] will converge to −θ′(r).

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Change of Measure

Typically, the function θ(r) will be convex. Since I I EQ[Xt] = I I EII

P[Xtg(Zt)e−rXte−θ(r)t]

we have = d dr I I EII

P[g(Zt)e−rXte−θ(r)t]

= I I EII

P

d dr g(Zt)

  • e−rXte−θ(r)t

− I I EQ[Xt] − tθ′(r) . Typically, dividing by t and letting t → ∞, the first term will

  • vanish. Thus t−1I

I EQ[Xt] will converge to −θ′(r). Hence the safety loading condition will not be fulfilled for r ≥ r0, where r0 is the solution to θ′(r) = 0. That means that Q[Tu < ∞] = 1 if and only if r ≥ r0.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

1

Cox Models

2

Ornstein–Uhlenbeck Intensities

3

Subexponential Claim Sizes

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Ornstein–Uhlenbeck Intensities

Consider the Ornstein–Uhlenbeck process dZt = −aZt dt + b dWt .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Ornstein–Uhlenbeck Intensities

Consider the Ornstein–Uhlenbeck process dZt = −aZt dt + b dWt . We consider the intensity λt = Z 2

t .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Randomly Generated Intensity

2 4 6 8 10 1 2 3 4 5 6 Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Equation

We have to solve

1 2b2g′′(z) − azg′(z) − [θ(r) + cr − z2h(r)]g(z) = 0 .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Equation

We have to solve

1 2b2g′′(z) − azg′(z) − [θ(r) + cr − z2h(r)]g(z) = 0 .

We try g(z) = κekz2 for some k < a

b2 . The restriction is in order

to ensure that I I E[g(Z0)] < ∞. From I I E[g(Z0)] = 1 we find κ =

  • 1 − b2k/a.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Equation

We have to solve

1 2b2g′′(z) − azg′(z) − [θ(r) + cr − z2h(r)]g(z) = 0 .

We try g(z) = κekz2 for some k < a

b2 . The restriction is in order

to ensure that I I E[g(Z0)] < ∞. From I I E[g(Z0)] = 1 we find κ =

  • 1 − b2k/a.

The equation reduces to

1 2b2(4z2k2 + 2k) − 2az2k − (θ(r) + cr) + z2h(r) = 0 .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Solution

2b2k2 − 2ak + h(r) = 0 , b2k = θ(r) + cr .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Solution

2b2k2 − 2ak + h(r) = 0 , b2k = θ(r) + cr . Thus we find k = a 2b2 −

  • a2

4b4 − h(r) 2b2 , θ(r) = a −

  • a2 − 2b2h(r)

2 − cr , and κ =

  • 1

2 +

  • 1

4 − b2h(r) 2a2 .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Martingale

M is a martingale. The generator of the diffusion after the change

  • f measure becomes
  • Af (z) = −(a − 2kb2)zf ′(z) + 1

2b2f ′′(z) .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Martingale

M is a martingale. The generator of the diffusion after the change

  • f measure becomes
  • Af (z) = −(a − 2kb2)zf ′(z) + 1

2b2f ′′(z) .

Hence under Q the process Z is an Ornstein–Uhlenbeck process with the same diffusion coefficient b and drift −

  • a2 − 2b2h(r) z.

Z will turn back to its mean more slowly than under I I P if r > 0. The (stationary under Q) drift of the process X under Q is then c − b2 2

  • a2 − 2b2h(r)

˜ h(r)h′(r) ˜ h(r) = −θ′(r) .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Cram´ er–Lundberg Inequalities

Let R be the (non-trivial) solution to θ(r) = 0. Then ψ(u) = I I EQ

  • 1

g(ZTu) eR(u+XTu ) e−Ru < κ−1e−Ru .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Cram´ er–Lundberg Inequalities

Let R be the (non-trivial) solution to θ(r) = 0. Then ψ(u) = I I EQ

  • 1

g(ZTu) eR(u+XTu ) e−Ru < κ−1e−Ru . In the same way we obtain the two finite-time Lundberg inequalities ψ(u, yu) < κ−1e−R(0,y)u , (y < y0) , ψ(u) − ψ(u, yu) < κ−1e−R(y,∞)u , (y > y0) , where y0 = 1/θ′(R), R(0, y) = supr≥0 r − yθ(r) and R(y, ∞) = supr≥0 r − yθ(r).

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Cram´ er–Lundberg Approximation

Using a renewal approach we get lim

u→∞ ψ(u) eRu = C I

I EII

P[g(Z0)]

for some constant C.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

1

Cox Models

2

Ornstein–Uhlenbeck Intensities

3

Subexponential Claim Sizes

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Subexponential Distributions

A distribution function is called subexponential, if for some and therefore all n ≥ 2 lim

y→∞

1 − F ∗n(y) 1 − F(y) = n .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Subexponential Distributions

A distribution function is called subexponential, if for some and therefore all n ≥ 2 lim

y→∞

1 − F ∗n(y) 1 − F(y) = n . A distribution function F(y) is in the class S∗, if µF < ∞ and lim

x→∞

x (1 − F(x − y))(1 − F(y)) 1 − F(x) dy = 2µF . For example are the Pareto, the Weibull and the Lognormal distributions in S∗. F ∈ S∗ implies F(y) and F s(y) = µ−1

F

y

0 1 − F(z) dz are in S.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Exponential Moments of the Intensity

Let ε > 0, S = inf{t > 0 : Zt = ε}, T1 = inf{t > S : Zt = 0}. Lemma Let either Z0 = 0 or Z0 be normally distributed with mean zero and variance b2/(2a). There exists a γ > 0 such that exp

  • γ

S1

0 (1 + Z 2 t ) dt

  • is integrable.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Exponential Moments of the Intensity

Let ε > 0, S = inf{t > 0 : Zt = ε}, T1 = inf{t > S : Zt = 0}. Lemma Let either Z0 = 0 or Z0 be normally distributed with mean zero and variance b2/(2a). There exists a γ > 0 such that exp

  • γ

S1

0 (1 + Z 2 t ) dt

  • is integrable.

Proof. Construct an appropriate martingale.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Tails

Lemma Let either Z0 = 0 or Z0 be normally distributed with mean zero and variance b2/(2a). Then lim

x→∞

I I P N(S1)

  • k=1

Yk > x

  • I

I P[−X(S1) > x] = 1 .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Tails

Lemma Let either Z0 = 0 or Z0 be normally distributed with mean zero and variance b2/(2a). Then lim

x→∞

I I P N(S1)

  • k=1

Yk > x

  • I

I P[−X(S1) > x] = 1 . This shows that −X(S1) and cS1 − X(S1) have the same distribution tail.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

The Asymptotic Behaviour

Theorem Suppose that both G(x) and G s(x) are subexponential, and that Z0 = 0 or that Z0 is normally distributed with mean zero and variance b2/(2a). Then lim

u→∞

ψ(u) 1 − G s(u) = µb2/(2a) c − µb2/(2a) = µb2 2ac − µb2 .

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Extensions

λt = m + Z 2

t or λt = (m + Zt)2.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Extensions

λt = m + Z 2

t or λt = (m + Zt)2.

Markov modulation, dZt = −a(Jt)Zt dt + b(Jt) dWt or λt = mJ(t) + Z 2

t for a Markov chain J.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Cox Models Ornstein–Uhlenbeck Intensities Subexponential Claim Sizes

Extensions

λt = m + Z 2

t or λt = (m + Zt)2.

Markov modulation, dZt = −a(Jt)Zt dt + b(Jt) dWt or λt = mJ(t) + Z 2

t for a Markov chain J.

Claim size distribution depends on λt: Yi ∼ Fλ(t).

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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References

References

Asmussen, S., S. and Schmidt, V. (1999). Tail probabilities for non-standard risk and queueing processes with subexponential

  • jumps. Adv. in Appl. Probab. 31, 422–447.

Grandell, J. and S. (2011). Ruin probabilities in a diffusion

  • environment. J. Appl. Probab. 48A, 39–50.

Jan Grandell & Hanspeter Schmidli KTH Stockholm & University of Cologne Ruin Probabilities in a Diffusion Environment

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Thank you for your attention