Jan 12, 2011 - Integral representations. Continuous versions of Ïλ and βN,p ... Let Ïλ be the Poisson measure: supp
On Continuous Versions of Poisson and Binomial Distributions Andrii Ilienko National Technical University of Ukraine, Kiev January 12, 2011
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Problem statement Problem statement
Let πλ be the Poisson measure:
Integral representations
supp πλ = {0, 1, 2, . . . }, Continuous versions of πλ and βN,p
e−λ λk , πλ {k} = k!
Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
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Problem statement Problem statement
Let πλ be the Poisson measure:
Integral representations
supp πλ = {0, 1, 2, . . . }, Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
e−λ λk , πλ {k} = k!
βN,p be the binomial measure: supp πλ = {0, 1, 2, . . . , N},
βN,p
!
N k p (1 − p)N−k . {k} = k
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Problem statement Problem statement
Let πλ be the Poisson measure:
Integral representations
supp πλ = {0, 1, 2, . . . }, Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
e−λ λk , πλ {k} = k!
βN,p be the binomial measure: supp πλ = {0, 1, 2, . . . , N},
βN,p
!
N k p (1 − p)N−k . {k} = k
The central aim of the talk is consideration of absolutely continuous versions of πλ and βN,p .
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Problem statement Integral representations
In other words, we spread measures πλ and βN,p continuously onto [0, ∞) and [0, N + 1], respectively.
Continuous versions of πλ and βN,p Limit theorem
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Moments of continuous Poisson distribution An application to the Γ-process
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Problem statement Integral representations
In other words, we spread measures πλ and βN,p continuously onto [0, ∞) and [0, N + 1], respectively.
Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution
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How to spread NATURALLY? And what is NATURALLY?
An application to the Γ-process
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Problem statement Integral representations
In other words, we spread measures πλ and βN,p continuously onto [0, ∞) and [0, N + 1], respectively.
Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
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How to spread NATURALLY? And what is NATURALLY? We use integral representations of Fπ (·) and Fβ (·) via complete and incomplete Euler Γ- and B-functions.
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Integral representations Problem statement Integral representations Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
Recall classical definitions: R∞
−t x−1 e t dt, x > 0; 0 R∞ incomplete Γ-function: Γλ (x) = λ e−t t x−1 dt, x > 0; R1 B-function: B(x, y) = 0 t x−1 (1 − t)y−1 dt, x, y > 0; R1 incomplete B-function: B p (x, y) = p t x−1 (1 − t)y−1 dt, x, y > 0;
Γ-function: Γ(x) =
here λ > 0, 0 < p < 1.
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Problem statement Integral representations Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
Lemma 1 (Probabilistic folklore). Distribution functions Fπ ≔ πλ (−∞, x) , x ∈ R and Fβ ≔ βN,p (−∞, x) , x ∈ R admit following representations:
Γλ ⌈x⌉ Fπ (x) = · 1{x>0} , Γ ⌈x⌉ B p ⌈x⌉, N + 1 − ⌈x⌉ Fβ (x) = · 1{0N} . B ⌈x⌉, N + 1 − ⌈x⌉
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Problem statement Integral representations Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
Lemma 1 (Probabilistic folklore). Distribution functions Fπ ≔ πλ (−∞, x) , x ∈ R and Fβ ≔ βN,p (−∞, x) , x ∈ R admit following representations:
Γλ ⌈x⌉ Fπ (x) = · 1{x>0} , Γ ⌈x⌉ B p ⌈x⌉, N + 1 − ⌈x⌉ Fβ (x) = · 1{0N} . B ⌈x⌉, N + 1 − ⌈x⌉
Proof is a simple calculus.
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Continuous versions of πλ and βN,p Problem statement Integral representations
Lemma 1 makes it possible to introduce the NATURAL continuous counterparts of discrete measures πλ and βN,p .
Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
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Continuous versions of πλ and βN,p Problem statement Integral representations Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution
Lemma 1 makes it possible to introduce the NATURAL continuous counterparts of discrete measures πλ and βN,p . Definition 1. By continuous Poisson distribution with parameter λ > 0 we will mean the probabilistic measure π˜ λ with Γλ (x) Fπ˜ (x) ≔ π˜ λ (−∞, x) = · 1{x>0} , Γ(x)
x ∈ R.
An application to the Γ-process
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Continuous versions of πλ and βN,p Problem statement Integral representations Continuous versions of πλ and βN,p Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
Lemma 1 makes it possible to introduce the NATURAL continuous counterparts of discrete measures πλ and βN,p . Definition 1. By continuous Poisson distribution with parameter λ > 0 we will mean the probabilistic measure π˜ λ with Γλ (x) Fπ˜ (x) ≔ π˜ λ (−∞, x) = · 1{x>0} , Γ(x)
x ∈ R.
Definition 2. By continuous binomial distribution with parameters y > 0, 0 < p < 1 we will mean the probabilistic measure β˜ N,p with B p (x, y + 1 − x) ˜ · 1{0 0. 0
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Problem statement Integral representations Continuous versions of πλ and βN,p
Theorem 4. The Laplace transform of mk has the form: k! m ˆ k (s) = , k s ln (1 + s)
s > 0.
Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
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Problem statement Integral representations
Theorem 4. The Laplace transform of mk has the form: k! m ˆ k (s) = , k s ln (1 + s)
Continuous versions of πλ and βN,p
s > 0.
Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
The double Laplace transform of the family (˜πλ , λ > 0) is (Laplace-Stieltjes w.r.t. measure and Laplace w.r.t. λ) ϕ(p, ˆ s) ≔
"
−px−sλ
e (0,∞)×(0,∞)
1 ln(1 + s) π˜ λ (dx) dλ = , s p + ln(1 + s) p, s > 0.
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An application to the Γ-process Problem statement Integral representations Continuous versions of πλ and βN,p
Consider Γ-process X = X(t), t ≥ 0 , i.e. L´evy process with the transition density βαt αt−1 −βx ft (x) = x e , Γ(αt)
x ≥ 0.
Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
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An application to the Γ-process Problem statement Integral representations Continuous versions of πλ and βN,p
Consider Γ-process X = X(t), t ≥ 0 , i.e. L´evy process with the transition density βαt αt−1 −βx ft (x) = x e , Γ(αt)
x ≥ 0.
Limit theorem Moments of continuous Poisson distribution An application to the Γ-process
The continuous Poisson distribution π˜ λ finds a use for study of the process X. Theorem 5. Let τc be the hitting time of the level c > 0. Then the r.v. ατc has the π˜ βc -distribution.
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