Efficient estimation for ergodic diffusions sampled at high frequency
Michael Sørensen Department of Mathematical Sciences University of Copenhagen, Denmark http://www.math.ku.dk/∼michael
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Efficient estimation for ergodic diffusions sampled at high frequency Michael Srensen Department of Mathematical Sciences University of Copenhagen, Denmark http://www.math.ku.dk/ michael . p.1/42 Discretely observed diffusion R p dX
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n
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n
n
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n
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n
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n
n
N
θ fj(x; θ)]
θ f(x; θ) = Eθ(f(X∆; θ) | X0 = x)
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n
N
θ fj(x; θ)]
θ fj(Xti−1; θ)] | Xt1, · · · , Xti−1) = 0
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n
N
θ fj(x; θ)]
θ fj(Xti−1; θ)] | Xt1, · · · , Xti−1) = 0
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n
N
θ fj(x; θ)]
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n
N
θ fj(x; θ)]
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n
N
θ fj(x; θ)]
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n
N
θ fj(x; θ)]
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x# s(x; θ)dx =
ℓ
ℓ
x#
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x# s(x; θ)dx =
ℓ
ℓ
x#
θ (x, y) = µθ(x)p(∆, x, y; θ)
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θ0 (g(∆, θ)) = 0
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θ0 (g(∆, θ)) = 0
D
θ0 Vθ0(ST θ0)−1
θ0
θ0
n
n
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n
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n
n
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n
n
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n
n
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n
θ V −1 θ
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n
n
n
n
n
θ V −1 θ
n
θ V −1 θ
θ fθ(Xti−1))
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n
n
n
n
θ V −1 θ
n
θ V −1 θ
θ fθ(Xti−1))
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n
n
n
n
θ V −1 θ
n
θ V −1 θ
θ fθ(Xti−1))
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n
N
θ fj(x; θ)]
θ fj(x; θ) = Eθ(fj(X∆; θ) | X0 = x)
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n
N
θ fj(x; θ)]
θ fj(x; θ) = Eθ(fj(X∆; θ) | X0 = x)
θ fj(x; θ) = fj(x; θ)+∆
2σ2(x; θ)∂2
xfj(x; θ)
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0 , . . . , Xtn n
i = i∆n, i = 0, . . . , n.
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x# s(x; θ)dx =
ℓ
ℓ xk˜
x# b(y;α) v(y;β)dy
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x# s(x; θ)dx =
ℓ
ℓ xk˜
x# b(y;α) v(y;β)dy
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x# s(x; θ)dx =
ℓ
ℓ xk˜
x# b(y;α) v(y;β)dy
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t ∂i2 y ∂i3 α ∂i4 β f, ij = 1, . . . kj, j = 1, 2,
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t ∂i2 y ∂i3 α ∂i4 β f, ij = 1, . . . kj, j = 1, 2,
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t ∂i2 y ∂i3 α ∂i4 β f, ij = 1, . . . kj, j = 1, 2,
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n
i , Xtn i−1; θ)
i , Xtn i−1; θ) | Xtn i−1) = ∆κ
nR(∆n, Xtn
i−1; θ)
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n
i , Xtn i−1; θ)
i , Xtn i−1; θ) | Xtn i−1) = ∆κ
nR(∆n, Xtn
i−1; θ)
2∆2g(2)(y, x; θ)+∆3R(∆, y, x; θ)
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n
i , Xtn i−1; θ)
i , Xtn i−1; θ) | Xtn i−1) = ∆κ
nR(∆n, Xtn
i−1; θ)
2∆2g(2)(y, x; θ)+∆3R(∆, y, x; θ)
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ℓ
2
ℓ
yg(0, x, x; θ)µθ0(x)dx = 0
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ℓ
2
ℓ
yg(0, x, x; θ)µθ0(x)dx = 0
ℓ Aθ0(x)µθ0(x)dx is invertible, where
1 2∂βv(x; β)∂2
yg1(0, x, x; θ)
1 2∂βv(x; β)∂2
yg2(0, x, x; θ)
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D
ℓ
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ℓ
ℓ
yg2(0, x, x; θ)µθ0(x)dx
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ℓ
ℓ
yg2(0, x, x; θ)µθ0(x)dx
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ℓ
ℓ
yg2(0, x, x; θ)µθ0(x)dx
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yg2(0, x, x; θ) = 0,
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11
22
ℓ
2
ℓ
yg2(0, x, x; θ0)]2µθ0(x)dx
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ℓ (∂αb(x;α0))2 v(x;β0)
1 2
ℓ
v(x;β0)
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ℓ (∂αb(x;α0))2 v(x;β0)
1 2
ℓ
v(x;β0)
yg2(0, x, x; θ) = ∂βv(x; β)/v(x; β)2
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ℓ (∂αb(x;α0))2 v(x;β0)
1 2
ℓ
v(x;β0)
yg2(0, x, x; θ) = ∂βv(x; β)/v(x; β)2
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n
i−1, ∆; θ)(Xtn i − F(∆, Xtn i−1; θ))
i−1, ∆; θ)
i − F(∆, Xtn i−1; θ))2 − φ(∆, Xtn i−1; θ)
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n
i−1, ∆; θ)(Xtn i − F(∆, Xtn i−1; θ))
i−1, ∆; θ)
i − F(∆, Xtn i−1; θ))2 − φ(∆, Xtn i−1; θ)
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n
i−1, ∆; θ)(Xtn i − F(∆, Xtn i−1; θ))
i−1, ∆; θ)
i − F(∆, Xtn i−1; θ))2 − φ(∆, Xtn i−1; θ)
yg2(0, x, x; θ)
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N
θ fj(x; θ)]
θ
n
i−1, ∆n; θ)[f(Xtn i ; θ) − π∆n
θ
i−1; θ)]
θ f(x; θ) = Eθ(f(X∆; θ) | X0 = x)
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1(x)
1 (x)
2(x)
2 (x)
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1(x)
1 (x)
2(x)
2 (x)
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n
i−1, ∆n; θ)[f(Xtn i ) − π∆n
θ
i−1)]
θ f(x)][f(X∆) − π∆ θ f(x)]T | X0 = x
θ f T (x)
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θ f(x)]
2(0, x, x; θ) = 0
1(0, x, x; θ) = ∂αb(x; α)/v(x; β)
yg∗ 2(0, x, x; θ) = ∂βv(x; β)/v(x; β)2
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2σ2(x; θ) d2
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2σ2(x; θ) d2
θ ϕ(x) = Eθ(ϕ(X∆)|X0 = x) = e−λθ∆ϕ(x)
θ
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θ ϕ(x) = e−λθ∆ϕ(x):
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t + bXt + c)dWt,
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t + bXt + c)dWt,
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t + bXt + c)dWt,
n
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t + 2ρν
1 2 Zt + (1 + ρ2)ν}dWt
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skewness parameter 0
−4 −2 2 4 0.0 0.1 0.2 0.3 0.4 0.5 0.6skewness parameter 0.5
−4 −2 2 4 0.0 0.1 0.2 0.3 0.4 0.5 0.6skewness parameter 1
−4 −2 2 4 0.0 0.1 0.2 0.3 0.4 0.5 0.6skewness parameter 2
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t dWt
n
n
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t dWt
n
n
2 , π 2 ),
2σ2, ϕ = βγ/(β − 1 2σ2)
(ρ(1−ϕ)σ−2− 1
2 , ρ(1+ϕ)σ−2− 1 2 )
n
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n
N
n
θ fj(x)
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θ ϕi(x; θ) = e−λi(θ)∆ϕi(x; θ)
i
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j
θ κk(x) − ∂θi[e−λj(θ)∆ϕj(x; θ)]
i
j
θ κr+s(x)
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j
θ κk(x) − ∂θi[e−λj(θ)∆ϕj(x; θ)]
i
j
θ κr+s(x)
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θ κi(x) = Eθ(κ(X∆)i | X0 = x)
θ to both sides of
i
i
θ κj(x),
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