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Logarithmic derivatives of densities for jump processes Atsushi - - PowerPoint PPT Presentation

Logarithmic derivatives of densities for jump processes Atsushi TAKEUCHI Osaka City University (JAPAN) June 30, 2009 City University of Hong Kong Workshop on Stochastic Analysis and Finance (June 29 - July 3, 2009) A. Takeuchi (Osaka


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Logarithmic derivatives of densities for jump processes

Atsushi TAKEUCHI

Osaka City University (JAPAN) June 30, 2009 City University of Hong Kong

Workshop on ”Stochastic Analysis and Finance” (June 29 - July 3, 2009)

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 1 / 25

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Preliminaries

dν: the L´ evy measure on R0 := R\{0}

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 2 / 25

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SLIDE 3

Preliminaries

dν: the L´ evy measure on R0 := R\{0} ∫

|θ|≤1

|θ|dν + ∫

|θ|>1

|θ|pdν < ∞ for any p ≥ 1, there exists α > 0 such that lim inf

ρ↘0

ρα ∫

R0

( |θ/ρ|2 ∧ 1 ) dν > 0, there exists a C1-density g(θ) such that lim

|θ|→∞

|g(θ)| = 0.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 2 / 25

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SLIDE 4

Preliminaries

dν: the L´ evy measure on R0 := R\{0} ∫

|θ|≤1

|θ|dν + ∫

|θ|>1

|θ|pdν < ∞ for any p ≥ 1, there exists α > 0 such that lim inf

ρ↘0

ρα ∫

R0

( |θ/ρ|2 ∧ 1 ) dν > 0, there exists a C1-density g(θ) such that lim

|θ|→∞

|g(θ)| = 0. a0(ε, y), a(ε, y) ∈ C1,∞

1+,b(R × R)

b(ε, y, θ) ∈ C1,∞,∞

1+,b

(R × R × R0) inf

y∈R inf θ∈R0

  • 1 + b′(ε, y, θ)
  • > 0,

lim

|θ|↘0 b(ε, y, θ) = 0

inf

y∈R a(ε, y)2 > 0,

inf

y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 2 / 25

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SLIDE 5

Example 1.1

Let a, b, c > 0, and 0 ≤ β < 1. Define dν = a { ebθI(θ<0) + e−cθI(θ>0) } dθ |θ|1+β which is a special case of CGMY process.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 3 / 25

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SLIDE 6

Example 1.1

Let a, b, c > 0, and 0 ≤ β < 1. Define dν = a { ebθI(θ<0) + e−cθI(θ>0) } dθ |θ|1+β which is a special case of CGMY process. In particular, gamma process: b = +∞, β = 0 variance gamma process: β = 0 tempered stable process: b = +∞, 0 < β < 1 inverse Gaussian process: b = +∞, β = 1/2.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 3 / 25

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SLIDE 7

For each (ε, x) ∈ R2, consider the stochastic differential equation:

✓ ✏

dxt = a0(ε, xt)dt+a(ε, xt)◦dWt+ ∫

R0

b(ε, xt−, θ)dJ, x0 = x

✒ ✑

{Wt ; t ∈ [0, T ]}: 1-dimensional Brownian motion dJ: the Poisson random measure on [0, T ] × R0 dt dν: the intensity d ˜ J = dJ − dt dν, dJ = I(|θ|≤1)d ˜ J + I(|θ|>1)dJ

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 4 / 25

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SLIDE 8

For each (ε, x) ∈ R2, consider the stochastic differential equation:

✓ ✏

dxt = a0(ε, xt)dt+a(ε, xt)◦dWt+ ∫

R0

b(ε, xt−, θ)dJ, x0 = x

✒ ✑

{Wt ; t ∈ [0, T ]}: 1-dimensional Brownian motion dJ: the Poisson random measure on [0, T ] × R0 dt dν: the intensity d ˜ J = dJ − dt dν, dJ = I(|θ|≤1)d ˜ J + I(|θ|>1)dJ The associated infinitesimal generator is

Lεf(y) = Aε

0f(y) + AεAε

2 f(y) + ∫

R0

{ Bε

θf(y) − I(|θ|≤1)Bε θf(y)

} dν ( Bε

θf(y) := f(y + b(ε, y, θ)) − f(y)

)

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 4 / 25

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SLIDE 9

Proposition 1.2

The mapping R ∋ x − → xt ∈ R has a C1-modification such that Zt := ∂xxt satisfies the linear SDE:

dZt = a′

0(ε, xt)Ztdt + a′(ε, xt)Zt ◦ dWt +

R0

b′(ε, xt−, θ)Zt−dJ.

Zt is invertible a.s.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 5 / 25

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SLIDE 10

Proposition 1.2

The mapping R ∋ x − → xt ∈ R has a C1-modification such that Zt := ∂xxt satisfies the linear SDE:

dZt = a′

0(ε, xt)Ztdt + a′(ε, xt)Zt ◦ dWt +

R0

b′(ε, xt−, θ)Zt−dJ.

Zt is invertible a.s. The mapping R ∋ ε − → xt ∈ R has a C1-modification such that Ht := ∂εxt satisfies the SDE:

dHt = a′

0(ε, xt)Htdt + a′(ε, xt)Ht ◦ dWt +

R0

b′(ε, xt−, θ)Ht−dJ + ∂εa0(ε, xt)dt + ∂εa(ε, xt) ◦ dWt + ∫

R0

∂εb(ε, xt−, θ)dJ.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 5 / 25

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Existence of smooth densities

Let ˜ b(ε, y, θ) := [ ∂θb/(1 + b′) ] (ε, y, θ) θ.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 6 / 25

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Existence of smooth densities

Let ˜ b(ε, y, θ) := [ ∂θb/(1 + b′) ] (ε, y, θ) θ. Under the conditions inf

y∈R a(ε, y)2 > 0 and inf y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0,

there exists α > 0 such that lim inf

ρ↘0

ρα ∫

R0

( |θ/ρ|2 ∧ 1 ) dν > 0, there exists γ > 0 such that inf

y∈R

{ |a(ε, y)/ρ|2 + ∫

R0

( ˜ b(ε, y, θ)/ρ

  • 2 ∧ 1

) dν } ≥ c ρ−γ for 0 < ρ < 1.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 6 / 25

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SLIDE 13

Existence of smooth densities

Let ˜ b(ε, y, θ) := [ ∂θb/(1 + b′) ] (ε, y, θ) θ. Under the conditions inf

y∈R a(ε, y)2 > 0 and inf y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0,

there exists α > 0 such that lim inf

ρ↘0

ρα ∫

R0

( |θ/ρ|2 ∧ 1 ) dν > 0, there exists γ > 0 such that inf

y∈R

{ |a(ε, y)/ρ|2 + ∫

R0

( ˜ b(ε, y, θ)/ρ

  • 2 ∧ 1

) dν } ≥ c ρ−γ for 0 < ρ < 1. Then, for each (x, ε) ∈ R2, there exists a smooth density px,ε

T (y) for xT . (cf. [T. 2002])

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 6 / 25

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SLIDE 14

Main problem

CLG(R) = {f ∈ C(R) ; |f(y)| ≤ c (1 + |y|)} F = { n ∑

k=1

αk fk IAk ; αk ∈ R, fk ∈ CLG(R), Ak ⊂ R: interval } < >

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 7 / 25

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SLIDE 15

Main problem

CLG(R) = {f ∈ C(R) ; |f(y)| ≤ c (1 + |y|)} F = { n ∑

k=1

αk fk IAk ; αk ∈ R, fk ∈ CLG(R), Ak ⊂ R: interval } < Goal > For ϕ ∈ F, compute the differentials of E [ϕ(xT )] in x ∈ R and ε ∈ R: ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Γx

T

] ∂ε (E[ϕ(xT )]) = E [ ϕ(xT ) Γε

T

] ∂2

x (E[ϕ(xT )]) = E

[ ϕ(xT ) ˜ Γx

T

] (logarithmic derivatives of px,ε

T (y), computations of the Greeks)

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 7 / 25

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Sensitivity with respect to the initial point Theorem 1 (Sensitivity in x ∈ R, [T. ’08] )

For ϕ ∈ F, it holds that ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Γx

T

] , Γx

T = Lx T − V x T

AT + Kx

T

A2

T

.

AT = T + ∫ T ∫

R0

|θ|2 dJ, v(ε, t, θ) = [1 + b′ ∂θb ] (ε, xt, θ) Zt |θ|2, Lx

t =

∫ t Zs a(ε, xs) dWs, V x

t =

∫ t ∫

R0

∂θ { g(θ)v(ε, s, θ) } g(θ) d ˜ J, Kx

t =

∫ t ∫

R0

2θv(ε, s, θ)dJ

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 8 / 25

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SLIDE 17

Remark 4.1

Recall AT = T + ∫ T ∫

R0

|θ|2dJ. Let N λ

T = T

R0

( e−λ|θ|2 − 1 ) dν. Under the condition on dν: lim inf

ρ↘0

ρα ∫

R0

( |θ/ρ|2 ∧ 1 ) dν > 0,

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 9 / 25

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SLIDE 18

Remark 4.1

Recall AT = T + ∫ T ∫

R0

|θ|2dJ. Let N λ

T = T

R0

( e−λ|θ|2 − 1 ) dν. Under the condition on dν: lim inf

ρ↘0

ρα ∫

R0

( |θ/ρ|2 ∧ 1 ) dν > 0, it holds that, for any p > 1, E [ A−p

T

] = 1 Γ(p) ∫ ∞ λp−1E [ exp ( −λAT − N λ

T

)] eNλ

T dλ

≤ c ∫ ∞ λp−1 exp [ −λT − c T ∫

R0

{ (λ|θ|2) ∧ 1 } dν ] dλ ≤ c ∫ ∞ λp−1 exp [ −λT − c λα/2T ] dλ < ∞.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 9 / 25

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SLIDE 19

Key Lemmas

Let ϕ ∈ C2

K(R) for a while. Recall

stochastic differential equation: dxt = a0(ε, xt)dt + a(ε, xt) ◦ dWt + ∫

R0

b(ε, xt−, θ)dJ x0 = x infinitesimal generator: Lε = Aε

0 + AεAε

2 + ∫

R0

{ Bε

θ − I(|θ|≤1)Bε θ

} dν ( Bε

θf(y) := f(y + b(ε, y, θ)) − f(y)

)

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 10 / 25

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SLIDE 20

Let u(t, x) := E [ ϕ ( xT −t ) x0 = x ] (t ∈ [0, T ), x ∈ R).

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 11 / 25

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SLIDE 21

Let u(t, x) := E [ ϕ ( xT −t ) x0 = x ] (t ∈ [0, T ), x ∈ R). Then, we see u ∈ C1,2

b

([0, T ) × R), ∂tu + Lεu = 0, lim

t↗T u(t, x) = ϕ(x).

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 11 / 25

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Let u(t, x) := E [ ϕ ( xT −t ) x0 = x ] (t ∈ [0, T ), x ∈ R). Then, we see u ∈ C1,2

b

([0, T ) × R), ∂tu + Lεu = 0, lim

t↗T u(t, x) = ϕ(x).

Applying the Itˆ

  • formula to u(t, xt) for 0 ≤ t < T , we have

u(t, xt) = u(0, x) + ∫ t u′(s, xs)a(ε, xs)dWs + ∫ t ∫

R0

θu(s, xs−)d ˜

J.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 11 / 25

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SLIDE 23

Let u(t, x) := E [ ϕ ( xT −t ) x0 = x ] (t ∈ [0, T ), x ∈ R). Then, we see u ∈ C1,2

b

([0, T ) × R), ∂tu + Lεu = 0, lim

t↗T u(t, x) = ϕ(x).

Applying the Itˆ

  • formula to u(t, xt) for 0 ≤ t < T , we have

u(t, xt) = u(0, x) + ∫ t u′(s, xs)a(ε, xs)dWs + ∫ t ∫

R0

θu(s, xs−)d ˜

J.

Taking the limit as t ↗ T enables us to get the following lemma.

Lemma 5.1

ϕ(xT ) = E [ϕ(xT )] + ∫ T u′(s, xs)a(ε, xs)dWs + ∫ T ∫

R0

θu(s, xs−)d ˜

J

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 11 / 25

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SLIDE 24

Lemma 5.2

T ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Lx

T

]

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 12 / 25

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SLIDE 25

Lemma 5.2

T ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Lx

T

] Proof of Lemma 5.2 We have already seen in Lemma 5.1 that

ϕ(xT ) = E[ϕ(xT )] + ∫ T u′(s, xs)a(ε, xs)dWs + ∫ T ∫

R0

θu(s, xs−)d ˜

J

Multiplying the above equality by Lx

T =

∫ T Zt a(ε, xt)dWt, we have (RHS) = E [∫ T u′(t, xt)a(ε, xt)dWt ∫ T Zt a(ε, xt) dWt ] = ∫ T E [ u′(t, xt)Zt ] dt = ∫ T ∂x (E[u(t, xt)]) dt = (LHS)

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 12 / 25

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SLIDE 26

Lemma 5.3

∂x ( E [ ϕ(xT ) ∫ T ∫

R0

|θ|2dJ ]) = −E [ ϕ(xT ) V x

T

]

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 13 / 25

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SLIDE 27

Lemma 5.3

∂x ( E [ ϕ(xT ) ∫ T ∫

R0

|θ|2dJ ]) = −E [ ϕ(xT ) V x

T

] Proof of Lemma 5.3 We have already seen in Lemma 5.1 that

ϕ(xT ) = E[ϕ(xT )] + ∫ T u′(s, xs)a(ε, xs)dWs + ∫ T ∫

R0

θu(s, xs−)d ˜

J

Multiplying the above equality by ∫ T ∫

R0

|θ|2d ˜ J, we have

E [ ϕ(xT ) ∫ T ∫

R0

|θ|2d ˜ J ] = E [∫ T ∫

R0

θu(t, xt)|θ|2dt dν

] .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 13 / 25

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SLIDE 28

Recall V x

T =

∫ T ∫

R0

∂θ{g(θ) v(ε, t, θ)} g(θ) d ˜

  • J. Since

lim

|θ|→∞ g(θ) = 0, we

see that

E [ ϕ(xT ) V x

T

] = E [∫ T ∫

R0

θu(t, xt) ∂θ {g(θ)v(ε, t, θ)}

g(θ) dt dν ] = −E [∫ T ∫

R0

u′(t, xt + b(ε, xt, θ)) (1 + b′(ε, xt, θ)) Zt|θ|2dt dν ] ( ∵ lim

|θ|→∞ g(θ) = 0, v(ε, t, θ) =

[1 + b′ ∂θb ] (ε, xt, θ)Zt|θ|2 ) = −∂x ( E [∫ T ∫

R0

u(t, xt + b(ε, xt, θ))|θ|2dt dν ]) = −∂x ( E [ ϕ(xT ) ∫ T ∫

R0

|θ|2dJ ]) .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 14 / 25

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SLIDE 29

Proof of Theorem 1

It is sufficient to study ϕ ∈ C2

K(R), instead of ϕ ∈ F, via the standard

density argument.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 15 / 25

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SLIDE 30

Proof of Theorem 1

It is sufficient to study ϕ ∈ C2

K(R), instead of ϕ ∈ F, via the standard

density argument. Our goal is ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) {Lx

T − V x T

AT + Kx

T

A2

T

}] .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 15 / 25

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SLIDE 31

Proof of Theorem 1

It is sufficient to study ϕ ∈ C2

K(R), instead of ϕ ∈ F, via the standard

density argument. Our goal is ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) {Lx

T − V x T

AT + Kx

T

A2

T

}] . We have already obtained ∂x (E[ϕ(xT ) AT ]) = E [ ϕ(xT ) { Lx

T − V x T

}] .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 15 / 25

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SLIDE 32

Proof of Theorem 1

It is sufficient to study ϕ ∈ C2

K(R), instead of ϕ ∈ F, via the standard

density argument. Our goal is ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) {Lx

T − V x T

AT + Kx

T

A2

T

}] . We have already obtained ∂x (E[ϕ(xT ) AT ]) = E [ ϕ(xT ) { Lx

T − V x T

}] . Thus, we have to consider how to get rid of AT = T + ∫ T ∫

R0

|θ|2dJ.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 15 / 25

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SLIDE 33

Remark that E[ϕ(xT )] = E [ϕ(xT )AT AT ] = ∫ ∞ M λ

T Eλ[ϕ(xT )AT ]dλ,

where dPλ dP

  • FT

= exp { − ∫ T ∫

R0

λ|θ|2dJ − ∫ T ∫

R0

( e−λ|θ|2 − 1 ) dt dν } M λ

T = exp

{ −λT − ∫ T ∫

R0

( 1 − e−λ|θ|2) dt dν } : deterministic

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 16 / 25

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SLIDE 34

Remark that E[ϕ(xT )] = E [ϕ(xT )AT AT ] = ∫ ∞ M λ

T Eλ[ϕ(xT )AT ]dλ,

where dPλ dP

  • FT

= exp { − ∫ T ∫

R0

λ|θ|2dJ − ∫ T ∫

R0

( e−λ|θ|2 − 1 ) dt dν } M λ

T = exp

{ −λT − ∫ T ∫

R0

( 1 − e−λ|θ|2) dt dν } : deterministic From the Girsanov theorem, we see that, under Pλ, {Wt ; t ∈ [0, T ]}: the Brownian motion, dJ: the Poisson random measure with the intensity e−λ|θ|2dt dν, d ˜ Jλ = dJ − e−λ|θ|2dt dν: the martingale measure.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 16 / 25

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SLIDE 35

We have already seen that ∂x ( Eλ[ϕ(xT )AT ] ) = Eλ[ ϕ(xT ) { Lx

T − V x,λ T

}] .  V x,λ

t

:= ∫ t ∫

R0

∂θ { e−λ|θ|2g(θ)v(ε, s, θ) } e−λ|θ|2g(θ) d ˜ Jλ  

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 17 / 25

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SLIDE 36

We have already seen that ∂x ( Eλ[ϕ(xT )AT ] ) = Eλ[ ϕ(xT ) { Lx

T − V x,λ T

}] .  V x,λ

t

:= ∫ t ∫

R0

∂θ { e−λ|θ|2g(θ)v(ε, s, θ) } e−λ|θ|2g(θ) d ˜ Jλ   Hence we have

∫ ∞ M λ

T Eλ[

ϕ(xT )Lx

T

] dλ = E [(∫ ∞ e−λAT dλ ) ϕ(xT )Lx

T

] = E [ ϕ(xT ) Lx

T

AT ] .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 17 / 25

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SLIDE 37

We have already seen that ∂x ( Eλ[ϕ(xT )AT ] ) = Eλ[ ϕ(xT ) { Lx

T − V x,λ T

}] .  V x,λ

t

:= ∫ t ∫

R0

∂θ { e−λ|θ|2g(θ)v(ε, s, θ) } e−λ|θ|2g(θ) d ˜ Jλ   Hence we have

∫ ∞ M λ

T Eλ[

ϕ(xT )Lx

T

] dλ = E [(∫ ∞ e−λAT dλ ) ϕ(xT )Lx

T

] = E [ ϕ(xT ) Lx

T

AT ] .

Since V x,λ

T

= V x

T − λKx T , we see that

∫ ∞ M λ

T Eλ[

ϕ(xT ) V x,λ

T

] dλ = E [∫ ∞ e−λAT ϕ(xT ) { V x

T − λKx T

} dλ ] = E [ ϕ(xT ) {V x

T

AT − Kx

T

A2

T

}] .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 17 / 25

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SLIDE 38

✓ ✏

∂x (E[ϕ(xT )]) = E [ ϕ(xT ) {Lx

T − V x T

AT + Kx

T

A2

T

}]

✒ ✑

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 18 / 25

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SLIDE 39

✓ ✏

∂x (E[ϕ(xT )]) = E [ ϕ(xT ) {Lx

T − V x T

AT + Kx

T

A2

T

}]

✒ ✑

In a similar manner, we can derive other sensitivity formulae: ∂2

x (E[ϕ(xT )]) = E

[ ϕ(xT ) ˜ Γx

T

] : Gamma ∂ε (E[ϕ(xT )]) = E [ ϕ(xT ) Γε

T

] : Vega etc.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 18 / 25

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SLIDE 40

✓ ✏

∂x (E[ϕ(xT )]) = E [ ϕ(xT ) {Lx

T − V x T

AT + Kx

T

A2

T

}]

✒ ✑

In a similar manner, we can derive other sensitivity formulae: ∂2

x (E[ϕ(xT )]) = E

[ ϕ(xT ) ˜ Γx

T

] : Gamma ∂ε (E[ϕ(xT )]) = E [ ϕ(xT ) Γε

T

] : Vega etc. Under the hypoelliptic situation, instead of the uniform ellipticity, the martingale method can be applied to the sensitivity on E [ ϕ ( 1 T ∫ T xt dt )] .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 18 / 25

slide-41
SLIDE 41

Remark

We have already obtained in Theorem 1 that

✓ ✏

Under the uniformly elliptic condition: (a) inf

y∈R a(ε, y)2 > 0,

(b) inf

y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0,

it holds that Γx

T = Lx T − V x T

AT + Kx

T

A2

T

, AT = T + ∫ T ∫

R0

|θ|2dJ.

✒ ✑

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 19 / 25

slide-42
SLIDE 42

Remark

We have already obtained in Theorem 1 that

✓ ✏

Under the uniformly elliptic condition: (a) inf

y∈R a(ε, y)2 > 0,

(b) inf

y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0,

it holds that Γx

T = Lx T − V x T

AT + Kx

T

A2

T

, AT = T + ∫ T ∫

R0

|θ|2dJ.

✒ ✑

[Question]: Can we study the same problem in the case where either (a)

  • r (b) is satisfied?
  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 19 / 25

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SLIDE 43

[Lemma 5.2] T ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Lx

T

]

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 20 / 25

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SLIDE 44

[Lemma 5.2] T ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Lx

T

]

Corollary 7.1

Under the condition inf

y∈R a(ε, y)2 > 0, then Γx T = Lx T

T holds.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 20 / 25

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SLIDE 45

[Lemma 5.2] T ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Lx

T

]

Corollary 7.1

Under the condition inf

y∈R a(ε, y)2 > 0, then Γx T = Lx T

T holds.

Remark 7.2

The condition on the measure dν is not necessary.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 20 / 25

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SLIDE 46

[Lemma 5.2] T ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Lx

T

]

Corollary 7.1

Under the condition inf

y∈R a(ε, y)2 > 0, then Γx T = Lx T

T holds.

Remark 7.2

The condition on the measure dν is not necessary.

Remark 7.3

In case of b(ε, y, θ) ≡ 0, the formula Γx

T = Lx T

T ( = 1 T ∫ T Zt a(ε, xt) dWt ) is well known as the Bismut formula.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 20 / 25

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SLIDE 47

[Lemma 5.3] ∂x ( E [ ϕ(xT ) ∫ T ∫

R0

|θ|2dJ ]) = −E [ ϕ(xT ) V x

T

]

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 21 / 25

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SLIDE 48

[Lemma 5.3] ∂x ( E [ ϕ(xT ) ∫ T ∫

R0

|θ|2dJ ]) = −E [ ϕ(xT ) V x

T

]

Corollary 7.4

Under the condition inf

y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0, then it holds that

Γx

T = −

V x

T

∫ T ∫

R0

|θ|2dJ + Kx

T

(∫ T ∫

R0

|θ|2dJ )2 .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 21 / 25

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SLIDE 49

[Lemma 5.3] ∂x ( E [ ϕ(xT ) ∫ T ∫

R0

|θ|2dJ ]) = −E [ ϕ(xT ) V x

T

]

Corollary 7.4

Under the condition inf

y∈R inf θ∈R0 ∂θb(ε, y, θ)2 > 0, then it holds that

Γx

T = −

V x

T

∫ T ∫

R0

|θ|2dJ + Kx

T

(∫ T ∫

R0

|θ|2dJ )2 .

Remark 7.5

The condition on the measure dν is essential.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 21 / 25

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SLIDE 50

Example 1: L´ evy processes

xt = x + γt + σWt + ∫ t ∫

R0

δ θ dJ (γ ∈ R, σ ≥ 0, δ ≥ 0)

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 22 / 25

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SLIDE 51

Example 1: L´ evy processes

xt = x + γt + σWt + ∫ t ∫

R0

δ θ dJ (γ ∈ R, σ ≥ 0, δ ≥ 0) If σ > 0 and δ > 0, we have

Γx

T =

WT σ − ∫ T ∫

R0

{ g(θ)|θ|2}′ δg(θ) d ˜ J T + ∫ T ∫

R0

|θ|2 dJ + ∫ T ∫

R0

2θ3 δ dJ ( T + ∫ T ∫

R0

|θ|2 dJ )2 ,

If σ > 0, we have Γx

T = WT

σ T ,

If δ > 0, we have

Γx

T =

− ∫ T ∫

R0

{ g(θ)|θ|2}′ δg(θ) d ˜ J ∫ T ∫

R0

|θ|2 dJ + ∫ T ∫

R0

2θ3 δ dJ (∫ T ∫

R0

|θ|2 dJ )2 .

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 22 / 25

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SLIDE 52

Example 2: Geometric L´ evy processes

(γ, σ, δ) ∈ R × [0, +∞) × [0, +∞), x ∈ (0, +∞) Xt = γt + σWt + ∫ t ∫

R0

δθ dJ : L´ evy process xt = x exp [Xt] : geometric L´ evy process

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 23 / 25

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SLIDE 53

Example 2: Geometric L´ evy processes

(γ, σ, δ) ∈ R × [0, +∞) × [0, +∞), x ∈ (0, +∞) Xt = γt + σWt + ∫ t ∫

R0

δθ dJ : L´ evy process xt = x exp [Xt] : geometric L´ evy process For the Itˆ

  • formula, we have

dxt = { γ + ∫

|θ|≤1

(eδθ − 1 − δθ)dν } xtdt + σxt ◦ dWt + ∫

R0

(eδθ − 1)xt−dJ.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 23 / 25

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SLIDE 54

Example 2: Geometric L´ evy processes

(γ, σ, δ) ∈ R × [0, +∞) × [0, +∞), x ∈ (0, +∞) Xt = γt + σWt + ∫ t ∫

R0

δθ dJ : L´ evy process xt = x exp [Xt] : geometric L´ evy process For the Itˆ

  • formula, we have

dxt = { γ + ∫

|θ|≤1

(eδθ − 1 − δθ)dν } xtdt + σxt ◦ dWt + ∫

R0

(eδθ − 1)xt−dJ. Write h(y) := ey. Since ∂x (ϕ(xt)) = ϕ′(xt) xt x = 1 x∂X ((ϕ ◦ h)(X + Xt))

  • X=log x,

we can compute the weight Γx

T by using the results in Example 1.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 23 / 25

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SLIDE 55

Conclusion

Stochastic differential equations with jumps Under the uniform ellipticity on a and b (, a or b), we have ∂x (E[ϕ(xT )]) = E [ ϕ(xT ) Γx

T

] , etc. There are some approaches to attack the sensitivity analysis.

the Girsanov transform the Malliavin calculus on the Wiener-Poisson space the martingale method

We make use of the Kolmogorov backward equation for Lε. The models can be of pure-jump type, and of infinite-activity type.

  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 24 / 25

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SLIDE 56

References

[1] Cass, T. R., and Friz, P. K. (2007): arXiv:math/0604311v3. [2] Davis, M. H. A., and Johansson, M. P. (2006): Stoch. Processes Appl., 116 101–129. [3] El-Khatib, Y., and Privault, N. (2004): Finance Stoch., 8 161–179. [4] Kawai, R. and T. (2008): under revision. [5] Kawai, R. and T. (2008): submitted for publication. [6]

  • T. (2002): Osaka J. Math., 39 523 – 559.

[7]

  • T. (2008): submitted for publication.

[8]

  • T. (2009): in preparation.
  • A. Takeuchi (Osaka City Univ. )

Logarithmic derivatives for jump processes June 30, 2009 25 / 25