On L evy Insurance Risk Models: A Review and New Directions Manuel - - PowerPoint PPT Presentation

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On L evy Insurance Risk Models: A Review and New Directions Manuel - - PowerPoint PPT Presentation

On L evy Insurance Risk Models: A Review and New Directions Manuel Morales University of Montreal with Erhan Bayraktar (University of Michigan), Zied Ben-Salah and Hassan Omidi (University of Montreal) and H el` ene Gu erin


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SLIDE 1

On L´ evy Insurance Risk Models: A Review and New Directions

Manuel Morales University of Montreal with Erhan Bayraktar (University of Michigan), Zied Ben-Salah and Hassan Omidi (University of Montreal) and H´ el` ene Gu´ erin (Universit´ e de Rennes) Tokyo, September 2013

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Introduction

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SLIDE 3

Introduction

This talk is about :

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Introduction

This talk is about :

◮ Presenting a short review of existing Levy insurance risk

models and the ruin problem

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SLIDE 5

Introduction

This talk is about :

◮ Presenting a short review of existing Levy insurance risk

models and the ruin problem

◮ Presenting our Work (in Progress)

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SLIDE 6

Introduction

This talk is about :

◮ Presenting a short review of existing Levy insurance risk

models and the ruin problem

◮ Presenting our Work (in Progress) ◮ Defining new path-dependent quantities that are relevant in

risk theory.

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SLIDE 7

Introduction

This talk is about :

◮ Presenting a short review of existing Levy insurance risk

models and the ruin problem

◮ Presenting our Work (in Progress) ◮ Defining new path-dependent quantities that are relevant in

risk theory.

◮ Deriving expressions for these new quantities.

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SLIDE 8

Introduction

This talk is about :

◮ Presenting a short review of existing Levy insurance risk

models and the ruin problem

◮ Presenting our Work (in Progress) ◮ Defining new path-dependent quantities that are relevant in

risk theory.

◮ Deriving expressions for these new quantities.

This is done through the use of recent developments in first-passage times for L´ evy processes.

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SLIDE 9

L´ evy Insurance Risk Models

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L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

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L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi.

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SLIDE 12

L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi. ◮ Brownian motion: Perturbed Model (Dufresne and Gerber

(1991)): Xt = Nt

i=1 Yi + Wt.

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SLIDE 13

L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi. ◮ Brownian motion: Perturbed Model (Dufresne and Gerber

(1991)): Xt = Nt

i=1 Yi + Wt. ◮ Gamma Process: Dufresne, Gerber and Shiu (1991)

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SLIDE 14

L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi. ◮ Brownian motion: Perturbed Model (Dufresne and Gerber

(1991)): Xt = Nt

i=1 Yi + Wt. ◮ Gamma Process: Dufresne, Gerber and Shiu (1991) ◮ α-stable risk process: Furrer (1998)

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SLIDE 15

L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi. ◮ Brownian motion: Perturbed Model (Dufresne and Gerber

(1991)): Xt = Nt

i=1 Yi + Wt. ◮ Gamma Process: Dufresne, Gerber and Shiu (1991) ◮ α-stable risk process: Furrer (1998) ◮ General perturbed case: Huzak et al. (2004)

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SLIDE 16

L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi. ◮ Brownian motion: Perturbed Model (Dufresne and Gerber

(1991)): Xt = Nt

i=1 Yi + Wt. ◮ Gamma Process: Dufresne, Gerber and Shiu (1991) ◮ α-stable risk process: Furrer (1998) ◮ General perturbed case: Huzak et al. (2004) ◮ EDPF for a perturbed subordinator: Morales (2003),

Garrido and Morales (2006) and Morales (2007)

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L´ evy Insurance Risk Models

Now we find models of the form R(t) = u + ct − X(t) , t 0 , where X is a spectrally positive L´ evy process.

◮ Compound Poisson Process: Classical Model (Cramer and

Lundberg): Xt = Nt

i=1 Yi. ◮ Brownian motion: Perturbed Model (Dufresne and Gerber

(1991)): Xt = Nt

i=1 Yi + Wt. ◮ Gamma Process: Dufresne, Gerber and Shiu (1991) ◮ α-stable risk process: Furrer (1998) ◮ General perturbed case: Huzak et al. (2004) ◮ EDPF for a perturbed subordinator: Morales (2003),

Garrido and Morales (2006) and Morales (2007)

◮ A generalized EDPF: Biffis and Morales (2010) and Biffis

and Kyprianou (2010)

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Our Model

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Our Model

We study the following L´ evy risk process R(t) := x + c t − X(t) , t 0 , (1) where X is a spectrally positive L´ evy process

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Our Model

We study the following L´ evy risk process R(t) := x + c t − X(t) , t 0 , (1) where X is a spectrally positive L´ evy process Laplace exponent ψX(z) := −1 t ln E[e−zXt] , z 0 , (2)

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Our Model

We study the following L´ evy risk process R(t) := x + c t − X(t) , t 0 , (1) where X is a spectrally positive L´ evy process Laplace exponent ψX(z) := −1 t ln E[e−zXt] , z 0 , (2)

ψX(z) = iaz + b2 2 z2 +

  • R
  • 1 − eizx + izxI{(−1,1)}(x)
  • ν(dx) ,

(3)

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Our Model

We study the following L´ evy risk process R(t) := x + c t − X(t) , t 0 , (1) where X is a spectrally positive L´ evy process Laplace exponent ψX(z) := −1 t ln E[e−zXt] , z 0 , (2)

ψX(z) = iaz + b2 2 z2 +

  • R
  • 1 − eizx + izxI{(−1,1)}(x)
  • ν(dx) ,

(3)

alternatively, X(t) = at + bW (t) + J(t) , t > 0 , (4)

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Advantages of Levy Models

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Advantages of Levy Models

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Advantages of Levy Models

◮ These seem to be good models for the aggregate claims.

Distribution might be in closed-form unlike the compound Poisson case.

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Advantages of Levy Models

◮ These seem to be good models for the aggregate claims.

Distribution might be in closed-form unlike the compound Poisson case.

◮ The ruin problem is well-understood [Biffis and Morales

(2010)].

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Advantages of Levy Models

◮ These seem to be good models for the aggregate claims.

Distribution might be in closed-form unlike the compound Poisson case.

◮ The ruin problem is well-understood [Biffis and Morales

(2010)].

◮ Expressions for non-ruin path-dependent quantities seem to be

at hand.

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Infinite- and Finite-time Horizon EDPF

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Infinite- and Finite-time Horizon EDPF

Definition

The Infinte-time EDPF φ is defined by φδ(x) := E

  • e−δτxw
  • |Rτx|, Rτx−, Rτx−
  • I{τx<∞}|R0 = x
  • ,

(5) where δ > 0 and w is a penalty function on R3

+ with

w(0, 0, 0) = w0 > 0.

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Infinite- and Finite-time Horizon EDPF

Definition

The Infinte-time EDPF φ is defined by φδ(x) := E

  • e−δτxw
  • |Rτx|, Rτx−, Rτx−
  • I{τx<∞}|R0 = x
  • ,

(5) where δ > 0 and w is a penalty function on R3

+ with

w(0, 0, 0) = w0 > 0.

Definition

The Finte-time EDPF φt is defined by φδ

t(x) := E

  • e−δτxw
  • |Rτx|, Rτx−, Rτx−
  • I{τx<t}|R0 = x
  • ,

(6) where δ > 0 and w is a penalty function on R3

+ with

w(0, 0, 0) = w0 > 0.

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Illustration for drawdown related variables

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Illustration for drawdown related variables

September-03-13 6:07 PM 1

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Applications

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Applications

Inside the EDPF we have the distributions (both infinite- and finite-time horizon versions) of

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Applications

Inside the EDPF we have the distributions (both infinite- and finite-time horizon versions) of

◮ |R(τ)| is the deficit at ruin,

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Applications

Inside the EDPF we have the distributions (both infinite- and finite-time horizon versions) of

◮ |R(τ)| is the deficit at ruin, ◮ R(τ−) is the surplus level prior to ruin,

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Applications

Inside the EDPF we have the distributions (both infinite- and finite-time horizon versions) of

◮ |R(τ)| is the deficit at ruin, ◮ R(τ−) is the surplus level prior to ruin, ◮ R(τ−) is last minimum before ruin.

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Applications

Inside the EDPF we have the distributions (both infinite- and finite-time horizon versions) of

◮ |R(τ)| is the deficit at ruin, ◮ R(τ−) is the surplus level prior to ruin, ◮ R(τ−) is last minimum before ruin.

All of which give information about how ruin occurs as functions

  • f the initial level x
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Applications

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Applications

Deficit |R(τx)|: ✩

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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level. ✩

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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level.

◮ Ruin-based risk measures could then be constructed.

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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level.

◮ Ruin-based risk measures could then be constructed.

VaRx

α

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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level.

◮ Ruin-based risk measures could then be constructed.

VaRx

α

The smallest deficit in the top 5% worst case scenarios. ✩

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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level.

◮ Ruin-based risk measures could then be constructed.

VaRx

α

The smallest deficit in the top 5% worst case scenarios.

◮ P(|R(τx)| > VaRx α) = α .

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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level.

◮ Ruin-based risk measures could then be constructed.

VaRx

α

The smallest deficit in the top 5% worst case scenarios.

◮ P(|R(τx)| > VaRx α) = α . ◮ VaRx 0.05. If ruin occurs, we can expect to observe (five times

  • ut of a hundred) a deficit of at least ✩ VaRx

0.05 when we start

  • ff with a level x.
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Applications

Deficit |R(τx)|:

◮ If we were able to readily compute F|R(τx)| we would have a

family of distributions indexed by the initial reserve level.

◮ Ruin-based risk measures could then be constructed.

VaRx

α

The smallest deficit in the top 5% worst case scenarios.

◮ P(|R(τx)| > VaRx α) = α . ◮ VaRx 0.05. If ruin occurs, we can expect to observe (five times

  • ut of a hundred) a deficit of at least ✩ VaRx

0.05 when we start

  • ff with a level x.

◮ It gives a solvency argument to set an appropriate initial

reserve x.

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Applications

✩ ✩

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Applications

Last minimum R(τ−): ✩ ✩

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Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level. ✩ ✩

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Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. ✩ ✩

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Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. VaRx

α

✩ ✩

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Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. VaRx

α

The smallest last minimum in the top 5% worst case scenarios. ✩ ✩

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SLIDE 54

Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. VaRx

α

The smallest last minimum in the top 5% worst case scenarios.

◮ P(R(τ−) > VaRx α) = α .

✩ ✩

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Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. VaRx

α

The smallest last minimum in the top 5% worst case scenarios.

◮ P(R(τ−) > VaRx α) = α . ◮ VaRx 0.05. In those cases when ruin occurs, the last minimum

will be observed to be (ninety five times out of a hundred) smaller than ✩ VaRx

0.05 when starting off with a level x.

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Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. VaRx

α

The smallest last minimum in the top 5% worst case scenarios.

◮ P(R(τ−) > VaRx α) = α . ◮ VaRx 0.05. In those cases when ruin occurs, the last minimum

will be observed to be (ninety five times out of a hundred) smaller than ✩ VaRx

0.05 when starting off with a level x. ◮ Does it give a warning level?

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SLIDE 57

Applications

Last minimum R(τ−):

◮ If we were able to readily compute FR(τ−) we would have a

family of distributions indexed by the initial reserve level.

◮ Due to its non-local nature at ruin, ruin-based risk measures

could be used to set warning levels. VaRx

α

The smallest last minimum in the top 5% worst case scenarios.

◮ P(R(τ−) > VaRx α) = α . ◮ VaRx 0.05. In those cases when ruin occurs, the last minimum

will be observed to be (ninety five times out of a hundred) smaller than ✩ VaRx

0.05 when starting off with a level x. ◮ Does it give a warning level? ◮ Do you want to be below a reserve level of ✩ VaRx 0.05!!!!

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Computing the EDPF

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Computing the EDPF

Theorem (Biffis and Morales (2010))

Let φδ

G denote the Generalized EDPF. Moreover, let K denote the

exponential distribution with mean σ2/2c and density k. Then, φG is given by φδ

G(x) =

  • w0 e−ρx (1 − K(x)) + HG(x)
  • n0

g∗(n)(x) , x 0 . (7)

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Computing the EDPF

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Computing the EDPF

Functions involved are

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Computing the EDPF

Functions involved are

◮ The function g is given by

g(y) = 1 c y e−ρ(y−s)k(y−s) +∞

s

e−ρ(x−s)νS(dx) + Gρ(s)

  • ds ,

(8) with the function Gρ defined through its Laplace transform +∞ e−ξxGρ(x)dx = Ψ

J(ξ) − Ψ J(ρ)

ρ − ξ , ξ 0 , (9) and ρ the unique non-negative solution of the generalized Lundberg equation cr + ΨS−Z(r) = δ .

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Computing the EDPF

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Computing the EDPF

◮ The function HG is given by

HG(u) = 1 c u e−ρ(u−s)k(u−s) +∞

s

e−ρ(x−s)χG(x, s) dx ds , (10) where, for x, s > 0, the function χG is defined as χG(x, s) = +∞

x+

w(y − x, x, s)νS−Z(dy) . (11)

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Three examples

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Three examples

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Three examples

◮ θ-process with parameter λ = 3/2

ψX(z) = 1 2σ2z2 + µz − c

  • α + z/β coth
  • π
  • α + z/β
  • +c√α coth
  • π√α
  • ,
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Three examples

◮ θ-process with parameter λ = 3/2

ψX(z) = 1 2σ2z2 + µz − c

  • α + z/β coth
  • π
  • α + z/β
  • +c√α coth
  • π√α
  • ,

◮ θ-process with parameter λ = 5/2

ψX(z) = 1 2σ2z2 + µz + c (α + z/β)

3 2 coth

  • π
  • α + z/β
  • −cα

3 2 coth

  • π√α
  • ,
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Three examples

◮ θ-process with parameter λ = 3/2

ψX(z) = 1 2σ2z2 + µz − c

  • α + z/β coth
  • π
  • α + z/β
  • +c√α coth
  • π√α
  • ,

◮ θ-process with parameter λ = 5/2

ψX(z) = 1 2σ2z2 + µz + c (α + z/β)

3 2 coth

  • π
  • α + z/β
  • −cα

3 2 coth

  • π√α
  • ,

◮ β-process with parameter λ ∈ (0, 3) \ {1, 2}

ψX(z) = 1 2σ2z2 + µz + cB(1 + α + z/β, 1 − λ) −cB(1 + α, 1 − λ) .

where B(x, y) = Γ(x)Γ(y)/Γ(x + y) is the Beta function.

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Three examples

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Three examples

These were introduced in Kuznetsov (2009) with first-passage times problems in mind. Features

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Three examples

These were introduced in Kuznetsov (2009) with first-passage times problems in mind. Features

◮ Good risk models equivalent to GIG, IG and Gamma.

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Three examples

These were introduced in Kuznetsov (2009) with first-passage times problems in mind. Features

◮ Good risk models equivalent to GIG, IG and Gamma. ◮

π(x) ∼ |x|−λ, as x → 0− , π(x) ∼ eβ(1+α)x, as x → −∞ .

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Three examples

These were introduced in Kuznetsov (2009) with first-passage times problems in mind. Features

◮ Good risk models equivalent to GIG, IG and Gamma. ◮

π(x) ∼ |x|−λ, as x → 0− , π(x) ∼ eβ(1+α)x, as x → −∞ .

◮ No closed-form densities

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SLIDE 75

Three examples

These were introduced in Kuznetsov (2009) with first-passage times problems in mind. Features

◮ Good risk models equivalent to GIG, IG and Gamma. ◮

π(x) ∼ |x|−λ, as x → 0− , π(x) ∼ eβ(1+α)x, as x → −∞ .

◮ No closed-form densities ◮ Infinite series expressions for the L´

evy measures π(x) =

  • m≥1

bmeρmx .

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SLIDE 76

Three examples

These were introduced in Kuznetsov (2009) with first-passage times problems in mind. Features

◮ Good risk models equivalent to GIG, IG and Gamma. ◮

π(x) ∼ |x|−λ, as x → 0− , π(x) ∼ eβ(1+α)x, as x → −∞ .

◮ No closed-form densities ◮ Infinite series expressions for the L´

evy measures π(x) =

  • m≥1

bmeρmx .

◮ Quasi-closed form expressions for the EPDF in both infinite-

and finite- time horizon!!!!

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SLIDE 77

Main Results: Infinite-time Horizon

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Main Results: Infinite-time Horizon

The discounted joint density of all three quantities under these three models is given in the following result.

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Main Results: Infinite-time Horizon

The discounted joint density of all three quantities under these three models is given in the following result.

Theorem

For δ ≥ 0, x > 0, y > 0, z > 0 and u ∈ (0, z ∧ x) E

  • e−δτxI(|Rτx| < y ; Rτx− < z ; Rτx− < u) I{τx<∞}|R0 = x
  • =

Φ(δ) δ

  • n≥1

cnζne−ζnx σ2 2 +

  • m≥1

bm(1 − e−ρmy) ρm(Φ(δ) + ρm) ×

  • e(ζn−ρm)u − 1

ζn − ρm − e−(Φ(δ)+ρm)z × e(Φ(δ)+ζn)u − 1 Φ(δ) + ζn , where Φ(δ) as the unique positive solution to ψX(z) = δ (generalized Lundberg equation).

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SLIDE 80

Non-ruin quantities

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Non-ruin quantities

Let us define, Dt = X t − Xt , where X t is the running supremum process X t = sups∈[0,t] Xs. We are interested primarily in the following stopping-times: τa = inf{t > 0 | Dt > a} , ρ = sup{t ∈ [0, τa] | X t = Xt} , for some predetermined value a > 0.

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Non-ruin quantities

Let us define, Dt = X t − Xt , where X t is the running supremum process X t = sups∈[0,t] Xs. We are interested primarily in the following stopping-times: τa = inf{t > 0 | Dt > a} , ρ = sup{t ∈ [0, τa] | X t = Xt} , for some predetermined value a > 0. These are the times of the first drawdown larger than a and the last time that the reserve was at its supremum before the a-drawdown.

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Non-ruin quantities

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Non-ruin quantities

Related quantities are:

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Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

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Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

◮ τa − ρ

speed of depletion ,

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Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

◮ τa − ρ

speed of depletion ,

◮ X τa

the maximum of X at the first-passage time,

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Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

◮ τa − ρ

speed of depletion ,

◮ X τa

the maximum of X at the first-passage time,

◮ X τa

the minimum of X at the first-passage time,

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SLIDE 89

Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

◮ τa − ρ

speed of depletion ,

◮ X τa

the maximum of X at the first-passage time,

◮ X τa

the minimum of X at the first-passage time,

◮ Dτa−

drawdown size just before it crosses the level a,

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SLIDE 90

Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

◮ τa − ρ

speed of depletion ,

◮ X τa

the maximum of X at the first-passage time,

◮ X τa

the minimum of X at the first-passage time,

◮ Dτa−

drawdown size just before it crosses the level a,

◮ Dτa − a

the overshoot of the drawdown process over the level a.

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SLIDE 91

Non-ruin quantities

Related quantities are:

◮ Dτa

size of drawdown ,

◮ τa − ρ

speed of depletion ,

◮ X τa

the maximum of X at the first-passage time,

◮ X τa

the minimum of X at the first-passage time,

◮ Dτa−

drawdown size just before it crosses the level a,

◮ Dτa − a

the overshoot of the drawdown process over the level a.

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SLIDE 92

Illustration for drawdown related variables

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SLIDE 93

Illustration for drawdown related variables

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SLIDE 94

Expressions

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SLIDE 95

Expressions

Work is not complete but a very advance stage.

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SLIDE 96

Expressions

Work is not complete but a very advance stage. Key issues:

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SLIDE 97

Expressions

Work is not complete but a very advance stage. Key issues:

◮ All expressions are given in terms of scale functions ,

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SLIDE 98

Expressions

Work is not complete but a very advance stage. Key issues:

◮ All expressions are given in terms of scale functions , ◮ Expressions are tractable for exponential jumps,

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SLIDE 99

Expressions

Work is not complete but a very advance stage. Key issues:

◮ All expressions are given in terms of scale functions , ◮ Expressions are tractable for exponential jumps, ◮ And potentially some classes of subordinators,

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SLIDE 100

Expressions

Work is not complete but a very advance stage. Key issues:

◮ All expressions are given in terms of scale functions , ◮ Expressions are tractable for exponential jumps, ◮ And potentially some classes of subordinators, ◮ Expressions for the speed of depletion seems to be the most

complicated of all.

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SLIDE 101

Non-ruin quantities

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SLIDE 102

Non-ruin quantities

We are currently studying the following particular cases: R(t) := x + c t − X(t) , t 0 , (12) where X is

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SLIDE 103

Non-ruin quantities

We are currently studying the following particular cases: R(t) := x + c t − X(t) , t 0 , (12) where X is

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SLIDE 104

Non-ruin quantities

We are currently studying the following particular cases: R(t) := x + c t − X(t) , t 0 , (12) where X is

◮ Compound Poisson Process: Exponential claims

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SLIDE 105

Non-ruin quantities

We are currently studying the following particular cases: R(t) := x + c t − X(t) , t 0 , (12) where X is

◮ Compound Poisson Process: Exponential claims ◮ Gamma Process

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SLIDE 106

Non-ruin quantities

We are currently studying the following particular cases: R(t) := x + c t − X(t) , t 0 , (12) where X is

◮ Compound Poisson Process: Exponential claims ◮ Gamma Process ◮ Theta Processes

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SLIDE 107

Expressions

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SLIDE 108

Expressions

Let {W (q), q ≥ 0} be the q-scale function of the process X, i.e. for every q ≥ 0, W (q) : R − → [0, ∞) such that W (q)(y) = 0 for all y < 0 satisfying ∞ e−λyW (q)(y)dy = 1 ψ(λ) − q , λ > Φ(q) . (13)

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SLIDE 109

Compound Poisson - exponential jumps

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SLIDE 110

Compound Poisson - exponential jumps

Probability of ruin before the first a-sized drawdown:

Px[X τa < 0] = λeµy−λ(a,0)(x∨a)

  • eλ(a,0)x − W (x ∧ a)

W (a) eλ(a,0)(x∨a)

  • ×
  • λ(a, 0)

λ(a, 0) + µe−µ(x∨a) − e−aµ

  • ×
  • −1

aλθ2(1 + θ) e

−aµθ 1+θ

[1 + θ − e

−aµθ 1+θ ] +

1 aλθ2

  • ×
  • 1 − e

−a2µθ 1+θ

  • − aµ

λθ

  • ,
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SLIDE 111

Compound Poisson - exponential jumps

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SLIDE 112

Compound Poisson - exponential jumps

Probability measure for the maximum level at drawdown time

Px(X τa ∈ dv) =

  • −1

aθ(1 + θ)(1 + (1 − a)θ) e

−aµθ 1+θ

[1 + θ − e

−aµθ 1+θ ]

× + 1 θ + θ2(1 − a)

  • ×
  • e−aµ − e

−aµθ 1+θ

  • + 1

θ(1 − e−aµ)

  • F0,0,a(v − x)dv,

for v ≥ x.

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SLIDE 113

Compound Poisson - exponential jumps

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SLIDE 114

Compound Poisson - exponential jumps

Probability measure of overshoot over drawdown level a:

Px (Dτa − a ∈ dh) =       −1 aθ(1 + θ)(1 + (1 − a)θ) e

−aµθ 1+θ

[1 + θ − e

−aµθ 1+θ ] +

1 θ + θ2(1 − a)    ×

  • e−aµ − e

−aµθ 1+θ

  • +

1 θ (1 − e−aµ)

  • µe−µhdh ,

for h ∈ (0, ∞).

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SLIDE 115

Compound Poisson - exponential jumps

Probability measure of overshoot over drawdown level a:

Px (Dτa − a ∈ dh) =       −1 aθ(1 + θ)(1 + (1 − a)θ) e

−aµθ 1+θ

[1 + θ − e

−aµθ 1+θ ] +

1 θ + θ2(1 − a)    ×

  • e−aµ − e

−aµθ 1+θ

  • +

1 θ (1 − e−aµ)

  • µe−µhdh ,

for h ∈ (0, ∞). It does not depend on the initial level x.

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SLIDE 116

Compound Poisson - exponential jumps

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SLIDE 117

Compound Poisson - exponential jumps

Bivariate Laplace transform of the speed of depletion variables:

Ex (e−qτa−rρ) = λ λ(a, q + r) [W (q)(a) − e−µaW (q)(0)] −

  • λµ

λ(a, q + r) e−µa + λ λ(a, q) λ(a, q + r) e−µa

  • ×
  • 1

(Φ(q) + µ)c + λµ (Φ(q) + µ)3c2 − λµ(Φ(q) + µ)c e(Φ(q)+µ)a − 1

(Φ(q) + µ) (Φ(q) + µ)2c − λµ

  • e

λµa (Φ(q)+µ)c − 1

  • .

(14)

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SLIDE 118

Compound Poisson - exponential jumps

Bivariate Laplace transform of the speed of depletion variables:

Ex (e−qτa−rρ) = λ λ(a, q + r) [W (q)(a) − e−µaW (q)(0)] −

  • λµ

λ(a, q + r) e−µa + λ λ(a, q) λ(a, q + r) e−µa

  • ×
  • 1

(Φ(q) + µ)c + λµ (Φ(q) + µ)3c2 − λµ(Φ(q) + µ)c e(Φ(q)+µ)a − 1

(Φ(q) + µ) (Φ(q) + µ)2c − λµ

  • e

λµa (Φ(q)+µ)c − 1

  • .

(14)

It does not depend on the initial level x.

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SLIDE 119

Remarks and Further Work

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SLIDE 120

Remarks and Further Work

◮ Technically, if we know the q- scale function of a risk L´

evy process then similar expressions can be found,

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SLIDE 121

Remarks and Further Work

◮ Technically, if we know the q- scale function of a risk L´

evy process then similar expressions can be found,

◮ Next step would to work out expressions for theta and beta

processes [Morales and Kuznetsov (2011)]

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SLIDE 122

Remarks and Further Work

◮ Technically, if we know the q- scale function of a risk L´

evy process then similar expressions can be found,

◮ Next step would to work out expressions for theta and beta

processes [Morales and Kuznetsov (2011)]

◮ Gamma processes

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SLIDE 123

Remarks and Further Work

◮ Technically, if we know the q- scale function of a risk L´

evy process then similar expressions can be found,

◮ Next step would to work out expressions for theta and beta

processes [Morales and Kuznetsov (2011)]

◮ Gamma processes ◮ Carry out numerical computation and empirical analysis

slide-124
SLIDE 124

Remarks and Further Work

◮ Technically, if we know the q- scale function of a risk L´

evy process then similar expressions can be found,

◮ Next step would to work out expressions for theta and beta

processes [Morales and Kuznetsov (2011)]

◮ Gamma processes ◮ Carry out numerical computation and empirical analysis ◮ Design risk measures with these quantities

slide-125
SLIDE 125

References

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SLIDE 126

References

  • 1. Biffis, E. and Morales, M. (2010). On the Expected

Discounted Penalty Function of Three Ruin-related Random Variables in a General L´ evy Risk Model. Insurance: Mathematics and Economics.

slide-127
SLIDE 127

References

  • 1. Biffis, E. and Morales, M. (2010). On the Expected

Discounted Penalty Function of Three Ruin-related Random Variables in a General L´ evy Risk Model. Insurance: Mathematics and Economics.

  • 2. Biffis, E. and Kyprianou, A. (2010). A note on scale functions

and the time value of ruin for L´ evy risk processes. Insurance: Mathematics and Economics.

slide-128
SLIDE 128

References

  • 1. Biffis, E. and Morales, M. (2010). On the Expected

Discounted Penalty Function of Three Ruin-related Random Variables in a General L´ evy Risk Model. Insurance: Mathematics and Economics.

  • 2. Biffis, E. and Kyprianou, A. (2010). A note on scale functions

and the time value of ruin for L´ evy risk processes. Insurance: Mathematics and Economics.

  • 3. Kuznetsov, A. (2009). On the Wiener-Hopf Factorization for

a Family of L´ evy Processes Realated to the Theta and Beta

  • Families. Working paper.
slide-129
SLIDE 129

References

  • 1. Biffis, E. and Morales, M. (2010). On the Expected

Discounted Penalty Function of Three Ruin-related Random Variables in a General L´ evy Risk Model. Insurance: Mathematics and Economics.

  • 2. Biffis, E. and Kyprianou, A. (2010). A note on scale functions

and the time value of ruin for L´ evy risk processes. Insurance: Mathematics and Economics.

  • 3. Kuznetsov, A. (2009). On the Wiener-Hopf Factorization for

a Family of L´ evy Processes Realated to the Theta and Beta

  • Families. Working paper.
  • 4. Mijatovic, A. and Pistorius, M. (2011). On the drawdown of

completely asymmetric Levy processes ARXIV

slide-130
SLIDE 130

References

  • 1. Biffis, E. and Morales, M. (2010). On the Expected

Discounted Penalty Function of Three Ruin-related Random Variables in a General L´ evy Risk Model. Insurance: Mathematics and Economics.

  • 2. Biffis, E. and Kyprianou, A. (2010). A note on scale functions

and the time value of ruin for L´ evy risk processes. Insurance: Mathematics and Economics.

  • 3. Kuznetsov, A. (2009). On the Wiener-Hopf Factorization for

a Family of L´ evy Processes Realated to the Theta and Beta

  • Families. Working paper.
  • 4. Mijatovic, A. and Pistorius, M. (2011). On the drawdown of

completely asymmetric Levy processes ARXIV

  • 5. Zhang, H. and Hadjiliadis, O. (2011). Drawdowns and the

Speed of Market Crash. Methodology and Computing in Applied Probability.