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Ginibre point process and its Palm measures: absolute continuity and - - PowerPoint PPT Presentation

. . Ginibre point process and its Palm measures: absolute continuity and singularity . . . . . Tomoyuki SHIRAI 1 2 Kyushu University Dec. 7, 2011 1 Joint work with Hirofumi Osada (Kyushu University) 2 10th workshop on stochastic


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. . . . . .

. . . . . . .

Ginibre point process and its Palm measures: absolute continuity and singularity

Tomoyuki SHIRAI 1 2

Kyushu University

  • Dec. 7, 2011

1Joint work with Hirofumi Osada (Kyushu University) 2”10th workshop on stochastic analysis on large scale interacting systems”

at Kochi University, Dec. 5–7, 2011.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Contents

. ..

1

Ginibre point process and determinantal point process . ..

2

Main results . ..

3

Absolute continuity . ..

4

Singularity

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre matrix ensemble and complex eigenvalues

MN : the space of N × N complex matrices ∼ = CN2 PN(dX) = Z −1

N exp(−TrX ∗X)dX,

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre matrix ensemble and complex eigenvalues

MN : the space of N × N complex matrices ∼ = CN2 PN(dX) = Z −1

N exp(−TrX ∗X)dX,

  • r equivalently,

Random matrix whose entries are all i.i.d. standard complex Gaussian. It is called Ginibre matrix ensemble of size N.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

3 / 26

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. . . . . .

Ginibre matrix ensemble and complex eigenvalues

MN : the space of N × N complex matrices ∼ = CN2 PN(dX) = Z −1

N exp(−TrX ∗X)dX,

  • r equivalently,

Random matrix whose entries are all i.i.d. standard complex Gaussian. It is called Ginibre matrix ensemble of size N. Probability density of complex eigenvalues was computed by Ginibre(1965) as follows: p(N)(z1, . . . , zN) = 1 ∏N

k=1 k!

1≤i<j≤N

|zi − zj|2 = 1 ∏N

k=1 k!

det(zj−1

i

)N

i,j=1

with respect to the standard complex Gaussian measure λ⊗N(dz1 . . . dzN) with λ(dz) = π−1e−|z|2dz.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Random complex eigenvalues

30 20 10 10 20 30 30 20 10 10 20 30

Ginibre N100

30 20 10 10 20 30 30 20 10 10 20 30

Ginibre N400

30 20 10 10 20 30 30 20 10 10 20 30

Ginibre N900

Figure: N = 100, 400, 900

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Random complex eigenvalues

30 20 10 10 20 30 30 20 10 10 20 30

Ginibre N100

30 20 10 10 20 30 30 20 10 10 20 30

Ginibre N400

30 20 10 10 20 30 30 20 10 10 20 30

Ginibre N900

Figure: N = 100, 400, 900

Bai showed that 1

N

∑N

i=1 δzi/ √ N w

→ Uniform(D1) almost surely

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Ginibre point process as determinantal point process

.

Definition (Determinantal point process (DPP))

. . . . . . . . DPP is a point process having deteminantal correlation functions ρn(z1, z2, . . . , zn) = det(K(zi, zj)n

i,j=1)

for some K(z, w) relative to a Radon measure λ(dz) = g(z)dz.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Ginibre point process as determinantal point process

.

Definition (Determinantal point process (DPP))

. . . . . . . . DPP is a point process having deteminantal correlation functions ρn(z1, z2, . . . , zn) = det(K(zi, zj)n

i,j=1)

for some K(z, w) relative to a Radon measure λ(dz) = g(z)dz. The N-particle Ginibre point process on C is rotation invariant DPP

  • n C whose kernel relative to λ(dz) = π−1e−|z|2dz is given by

K (N)(z, w) =

N−1

k=0

(zw)k k!

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre point process as determinantal point process

.

Definition (Determinantal point process (DPP))

. . . . . . . . DPP is a point process having deteminantal correlation functions ρn(z1, z2, . . . , zn) = det(K(zi, zj)n

i,j=1)

for some K(z, w) relative to a Radon measure λ(dz) = g(z)dz. The N-particle Ginibre point process on C is rotation invariant DPP

  • n C whose kernel relative to λ(dz) = π−1e−|z|2dz is given by

K (N)(z, w) =

N−1

k=0

(zw)k k!

N→∞

→ ezw =: K(z, w)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre point process as determinantal point process

.

Definition (Determinantal point process (DPP))

. . . . . . . . DPP is a point process having deteminantal correlation functions ρn(z1, z2, . . . , zn) = det(K(zi, zj)n

i,j=1)

for some K(z, w) relative to a Radon measure λ(dz) = g(z)dz. The N-particle Ginibre point process on C is rotation invariant DPP

  • n C whose kernel relative to λ(dz) = π−1e−|z|2dz is given by

K (N)(z, w) =

N−1

k=0

(zw)k k!

N→∞

→ ezw =: K(z, w) When correlation functions converge uniformly on any compacts, corresponding point processes converge weakly to a limit.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Ginibre point process

Ginibre point process on C is defined as DPP with a kernel K(z, w) = ezw, λ(dz) = π−1e−|z|2dz

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre point process

Ginibre point process on C is defined as DPP with a kernel K(z, w) = ezw, λ(dz) = π−1e−|z|2dz In particular, ρ1(z) = g(z)K(z, z) = π−1 ρ2(z, w) ≤ ρ1(z)ρ1(w) · · · negative correlation

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Ginibre point process

Ginibre point process on C is defined as DPP with a kernel K(z, w) = ezw, λ(dz) = π−1e−|z|2dz In particular, ρ1(z) = g(z)K(z, z) = π−1 ρ2(z, w) ≤ ρ1(z)ρ1(w) · · · negative correlation Ginibre p.p. on C is invariant under translations and rotations.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Poisson and Ginibre

10 5 5 10 10 5 5 10

Poisson

10 5 5 10 10 5 5 10

Ginibre

Figure: Poisson(left) and Ginibre(right)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Variance and large deviations for the number of points

ξ(Dr) is the number of points inside the disk of radius r. .

.

.

1 Variance

Poisson case: Var(ξ(Dr)) = r 2 Ginibre case: Var(ξ(Dr)) ∼ r √π

.

.

.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Variance and large deviations for the number of points

ξ(Dr) is the number of points inside the disk of radius r. .

.

.

1 Variance

Poisson case: Var(ξ(Dr)) = r 2 Ginibre case: Var(ξ(Dr)) ∼ r √π

.

.

.

2 Large deviations

Poisson case: P(r −2ξ(Dr) ≈ a) ∼ exp(−I(a)r 2) Ginibre case: P(r −2ξ(Dr) ≈ a) ∼ exp(−J(a)r 4)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre point process is considered as a Gibbs measure?

Formal expression: µ = Z −1 ∏

i<j

|zi − zj|2e− ∑

i |zi|2 ∞

i=1

dzi = Z −1 exp  − ∑

i

|zi|2 + 2 ∏

i<j

log |zi − zj|  

i=1

dzi

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre point process is considered as a Gibbs measure?

Formal expression: µ = Z −1 ∏

i<j

|zi − zj|2e− ∑

i |zi|2 ∞

i=1

dzi = Z −1 exp  − ∑

i

|zi|2 + 2 ∏

i<j

log |zi − zj|  

i=1

dzi 2-body potential Φ(z, w) = −2 log |z − w| is not even bounded.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Palm measure

We focus on the (reduced) Palm measure of a simple point process µ defined as follows: for a = (a1, a2, . . . , an) ∈ Rn µa(·) := µ(· −

n

i=1

δai | ξ({ai}) ≥ 1, ∀i = 1, 2, . . . n)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Palm measure

We focus on the (reduced) Palm measure of a simple point process µ defined as follows: for a = (a1, a2, . . . , an) ∈ Rn µa(·) := µ(· −

n

i=1

δai | ξ({ai}) ≥ 1, ∀i = 1, 2, . . . n) For a Poisson point process Π, it is well-known that Πa = Π

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Palm measure

We focus on the (reduced) Palm measure of a simple point process µ defined as follows: for a = (a1, a2, . . . , an) ∈ Rn µa(·) := µ(· −

n

i=1

δai | ξ({ai}) ≥ 1, ∀i = 1, 2, . . . n) For a Poisson point process Π, it is well-known that Πa = Π More generally, for a Gibbs measure (with nice potential U), it is well-known that dµa dµ (ξ) ∝ e−U(a|ξ) where U(a|ξ) is the energy from the other configuration ξ.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Ginibre point process and its Palm measure

Palm measure of DPP is again a DPP and its kernel is given by K α(z, w) = K(z, w) − K(z, α)K(α, w) K(α, α)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Ginibre point process and its Palm measure

Palm measure of DPP is again a DPP and its kernel is given by K α(z, w) = K(z, w) − K(z, α)K(α, w) K(α, α) For Ginibre point process (K(z, w) = ezw), K 0(z, w) = K(z, w) − K(z, 0)K(0, w) K(0, 0) = ezw − 1 with respect to λ(dz) = π−1e−|z|2dz =: g(z)dz.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Ginibre point process and its Palm measure

Palm measure of DPP is again a DPP and its kernel is given by K α(z, w) = K(z, w) − K(z, α)K(α, w) K(α, α) For Ginibre point process (K(z, w) = ezw), K 0(z, w) = K(z, w) − K(z, 0)K(0, w) K(0, 0) = ezw − 1 with respect to λ(dz) = π−1e−|z|2dz =: g(z)dz. In particular, the particle density under Palm measure is reduced to ρ0

1(z) = g(z)K 0(z, z) = π−1(1 − e−|z|2).

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Questions

.

.

.

1 Are Ginibre p.p. µ and its Palm measure µa absolutely continuous?

.

.

.

2 Are Palm measures of Ginibre p.p. µa and µb absolutely continuous?

.

.

.

3 Give a criterion for absolute continuity between general DPPs in

terms of kernel K and base measure λ.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Absolute continuity for Poisson p.p

.

Theorem (A.V.Skorohod, Y.Takahashi)

. . . . . . . . Let Πλ be a Poisson point process with intensity λ. Then, Πλ ∼ Πρ are equivalent to the following: (i) λ ∼ ρ (ii) Hellinger distance between λ and ρ is finite d(λ, ρ)2 = 1 2 ∫

R

(√ dρ dλ − 1 )2 dλ < ∞ Moreover, D(Πλ, Πρ)2 := 1 2 ∫

R

(√ dΠρ dΠλ − 1 )2 dΠλ = 1 − e−d(λ,ρ)2

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Main results

µ : Ginibre point process on C µx : the Palm measure of µ given that there are points at x ∈ Cm. .

Theorem

. . . . . . . . Let x ∈ Cm and y ∈ Cn, where m, n = 0, 1, 2, . . . . Then the following holds. (i) If m = n, then µx and µy are mutually absolutely continuous. (ii) If m ̸= n, then µx and µy are sigular each other.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Main results

µ : Ginibre point process on C µx : the Palm measure of µ given that there are points at x ∈ Cm. .

Theorem

. . . . . . . . Let x ∈ Cm and y ∈ Cn, where m, n = 0, 1, 2, . . . . Then the following holds. (i) If m = n, then µx and µy are mutually absolutely continuous. (ii) If m ̸= n, then µx and µy are sigular each other. When µ is Gibbs, µx << µ. So, we would say that Ginibre is not Gibbs in the ordinary sense. Osada introduced a weak notion of Gibbs measure, quasi-Gibbs property.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Related results

Consider the zeros of the (hyperbolic) Gaussian analytic function X(z) =

n=0

ζnzn

  • n D1

where ζn, n = 0, 1, 2, . . . i.i.d. NC(0, 1). Peres-Vir´ ag showed that zeros of X(z) form DPP associated with Bergman kernel K(z, w) = π−1(1 − zw)−2 and Lebesgue measure on D1. Halroyd-Soo showed that the zero process µX and its Palm measure µ0

X are mutually absolutely continuous.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Absolute continuity

.

Theorem

. . . . . . . . For any x, y ∈ Cn, two Palm measures µx and µy of the Ginibre point process are mutually absolutely continuous and its Radon-Nikodym density is given by dµx dµy (ξ) = 1 Zxy lim

r→∞

|zi|<br

|x − zi|2 |y − zi|2 where ξ = ∑

i δzi, |x − z|2 = ∏n j=1 |xj − z|2 and

Zxy = det(K(xi, xj))n

i,j=1

det(K(yi, yj))n

i,j=1

The infinite product of the RHS is conditionally convergent.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Radon-Nikodym density

For simplicity, x ∈ C and ξ = ∑

i δzi

µx(z1, . . . , zn) ∝ ∏n

i=1 |x − zi|2 ∏ i<j |zi − zj|2 exp(− ∑n i=1 |zi|2)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Radon-Nikodym density

For simplicity, x ∈ C and ξ = ∑

i δzi

µx(z1, . . . , zn) ∝ ∏n

i=1 |x − zi|2 ∏ i<j |zi − zj|2 exp(− ∑n i=1 |zi|2)

Radon-Nikodym density is µx(z1, . . . , zn) µy(z1, . . . , zn) =

n

i=1

|x − zi|2 |y − zi|2 =

n

i=1

|1 − x/zi|2 |1 − y/zi|2 →?

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Radon-Nikodym density

For simplicity, x ∈ C and ξ = ∑

i δzi

µx(z1, . . . , zn) ∝ ∏n

i=1 |x − zi|2 ∏ i<j |zi − zj|2 exp(− ∑n i=1 |zi|2)

Radon-Nikodym density is µx(z1, . . . , zn) µy(z1, . . . , zn) =

n

i=1

|x − zi|2 |y − zi|2 =

n

i=1

|1 − x/zi|2 |1 − y/zi|2 →? The canonical infinite product (of order 2)

i=1

(1 − x zi ) exp ( x zi + x2 2z2

i

) is absolutely covergent, but ∏∞

i=1(1 − x zi ) itself is not since the

number of zeros ξ(Dr) inside the disk Dr grows like r2.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Small fluctuation

ξ(Dr) is the number of points inside the disk of radius r.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

Small fluctuation

ξ(Dr) is the number of points inside the disk of radius r. While var(ξ(Dr)) = O(r2) under Poisson p.p., var(ξ(Dr)) = O(r) as r → ∞ under Ginibre p.p.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

18 / 26

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. . . . . .

Small fluctuation

ξ(Dr) is the number of points inside the disk of radius r. While var(ξ(Dr)) = O(r2) under Poisson p.p., var(ξ(Dr)) = O(r) as r → ∞ under Ginibre p.p. This small fluctuation property makes the series ∑

|zi|<br

1 zi , ∑

|zi|<br

1 z2

i

to be conditionally convergent, and hence ∏∞

i=1(1 − x zi ) is conditinally

convergent.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

18 / 26

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. . . . . .

Small fluctuation

ξ(Dr) is the number of points inside the disk of radius r. While var(ξ(Dr)) = O(r2) under Poisson p.p., var(ξ(Dr)) = O(r) as r → ∞ under Ginibre p.p. This small fluctuation property makes the series ∑

|zi|<br

1 zi , ∑

|zi|<br

1 z2

i

to be conditionally convergent, and hence ∏∞

i=1(1 − x zi ) is conditinally

convergent. The situation is similar to sin πz πz = ∏

i∈Z\{0}

(1 − z i ) =

i=1

(1 − z i )(1 − z −i ) =

i=1

(1 − z2 i2 )

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

Interacting Brownian Motion under Ginibre p.p.

Katori-Tanemura and Osada independently (by using different techniques) constructed diffusion processes of ∞-particles invariant under some DPPs on R. Osada also constructed a diffusion process invariant under Ginibre point process. It is formally given as ∞-dimensional SDE dX i

t = dBi t − X i t + lim r→∞

|X i

t |<r,j̸=i

X i

t − X j t

|X i

t − X j t |2 dt

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

For singularity: Kostlan’s theorem

Y1, Y2, . . . are indepedent and Yi ∼ Γ(i, 1), the sum of i exponential random variables with mean 1. {|z1|2, |z2|2, . . . } d = {Y1, Y2, . . . } as a set where ξ = ∑

i δzi is a Ginibre point configuration.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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. . . . . .

For singularity: Kostlan’s theorem

Y1, Y2, . . . are indepedent and Yi ∼ Γ(i, 1), the sum of i exponential random variables with mean 1. {|z1|2, |z2|2, . . . } d = {Y1, Y2, . . . } as a set where ξ = ∑

i δzi is a Ginibre point configuration.

Under the Palm measure conditioned at the origin, we see that {|z1|2, |z2|2, . . . } d = {Y2, Y3, . . . } as a set

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

For singularity: Kostlan’s theorem

Y1, Y2, . . . are indepedent and Yi ∼ Γ(i, 1), the sum of i exponential random variables with mean 1. {|z1|2, |z2|2, . . . } d = {Y1, Y2, . . . } as a set where ξ = ∑

i δzi is a Ginibre point configuration.

Under the Palm measure conditioned at the origin, we see that {|z1|2, |z2|2, . . . } d = {Y2, Y3, . . . } as a set Kakutani’s dichotomy for two independent infinite sequences of probability measures M = (µ1, µ2, . . . ), and N = (ν1, ν2, . . . ),

i=1

R

√ µi(t)νi(t)dt > 0 or = 0 ⇐ ⇒ M ∼ N or M ⊥ N

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

  • Dec. 7, 2011

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. . . . . .

For singularity: Kostlan’s theorem

Y1, Y2, . . . are indepedent and Yi ∼ Γ(i, 1), the sum of i exponential random variables with mean 1. {|z1|2, |z2|2, . . . } d = {Y1, Y2, . . . } as a set where ξ = ∑

i δzi is a Ginibre point configuration.

Under the Palm measure conditioned at the origin, we see that {|z1|2, |z2|2, . . . } d = {Y2, Y3, . . . } as a set Kakutani’s dichotomy for two independent infinite sequences of probability measures M = (µ1, µ2, . . . ), and N = (ν1, ν2, . . . ),

i=1

R

√ µi(t)νi(t)dt > 0 or = 0 ⇐ ⇒ M ∼ N or M ⊥ N By some calculation, we see that, (Y1, Y2, . . . ) ⊥ (Y2, Y3, . . . ).

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-44
SLIDE 44

. . . . . .

The zeros of Gaussian analytic function

GAF X(z) = ∑∞

n=0 ζnzn, where ζn ∼ NC(0, 1)

Y1, Y2, . . . are indepedent and Yi ∼ U1/2i

i

. {|z1|2, |z2|2, . . . } d = {Y1, Y2, . . . } as a set where ξ = ∑

i δzi is the zeros of the above GAF X.

Under the Palm measure conditioned at the origin, we see that {|z1|2, |z2|2, . . . } d = {Y2, Y3, . . . } as a set By some calculation, we see that (Y1, Y2, . . . ) ∼ (Y2, Y3, . . . ).

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-45
SLIDE 45

. . . . . .

Image measures

Image measures inherit absolute continuity but not necessarily singluarity.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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SLIDE 46

. . . . . .

Image measures

Image measures inherit absolute continuity but not necessarily singluarity. Our situation is like this. The RHSs have the same distribution by Kostlan’s theorem.

i=1

C ∋ (Y1, Y2, . . . ) →

i=1

δYi ∈ Conf ([0, ∞)) Conf (C) ∋

i=1

δzi →

i=1

δ|zi|2 ∈ Conf ([0, ∞))

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-47
SLIDE 47

. . . . . .

Idea of the proof for singularity (1)

Define a function on the configuration space FN(ξ) := 1 N

N

k=1

(ξ(Dk) − k) for ξ = ∑

i

δzi where ξ(Dk) is the number of point inside the disk Dk of radius √ k. . . . . . . . . .

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-48
SLIDE 48

. . . . . .

Idea of the proof for singularity (1)

Define a function on the configuration space FN(ξ) := 1 N

N

k=1

(ξ(Dk) − k) for ξ = ∑

i

δzi where ξ(Dk) is the number of point inside the disk Dk of radius √ k. Since ξ(Dk), k = 1, 2, . . . , n are correlated, var(FN) = O(N) under Poisson p.p. Π. . . . . . . . . .

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-49
SLIDE 49

. . . . . .

Idea of the proof for singularity (1)

Define a function on the configuration space FN(ξ) := 1 N

N

k=1

(ξ(Dk) − k) for ξ = ∑

i

δzi where ξ(Dk) is the number of point inside the disk Dk of radius √ k. Since ξ(Dk), k = 1, 2, . . . , n are correlated, var(FN) = O(N) under Poisson p.p. Π. .

Proposition

. . . . . . . . Under Ginibre p.p. and its Palm measures, var(FN) = O(1) by negative correlation.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-50
SLIDE 50

. . . . . .

Idea of the proof for singularity (2)

FN(ξ) := 1 N

N

k=1

(ξ(Dk) − k) for ξ = ∑

i δzi

.

Theorem

. . . . . . . . For m ∈ N and 0m = (0, 0, . . . , 0) ∈ Cm, then lim

N→∞ FN(ξ) = −m,

weakly in L2(µ0m)

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-51
SLIDE 51

. . . . . .

Idea of the proof for singularity (2)

FN(ξ) := 1 N

N

k=1

(ξ(Dk) − k) for ξ = ∑

i δzi

.

Theorem

. . . . . . . . For m ∈ N and 0m = (0, 0, . . . , 0) ∈ Cm, then lim

N→∞ FN(ξ) = −m,

weakly in L2(µ0m) From this theorem, we see that for 0n ∈ Cn and 0m ∈ Cm with n ̸= m, µ0n and µ0m are mutually singular, µ0n ⊥ µ0m.

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-52
SLIDE 52

. . . . . .

Idea of the proof for singularity (2)

FN(ξ) := 1 N

N

k=1

(ξ(Dk) − k) for ξ = ∑

i δzi

.

Theorem

. . . . . . . . For m ∈ N and 0m = (0, 0, . . . , 0) ∈ Cm, then lim

N→∞ FN(ξ) = −m,

weakly in L2(µ0m) From this theorem, we see that for 0n ∈ Cn and 0m ∈ Cm with n ̸= m, µ0n and µ0m are mutually singular, µ0n ⊥ µ0m. For general a ∈ Cn and b ∈ Cm, µa ∼ µ0n ⊥ µ0m ∼ µb

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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slide-53
SLIDE 53

. . . . . .

Concluding remarks and open questions

.

.

.

1 Absolute continuity for general DPP. Can we give a criterion for

absolute continuity in terms of K(z, w) and λ(dz)? More concretely, radially symmetric DPP on C may be next target, for example. .

.

.

2 Is it true that singularity are inherited via two mappings:

i=1

C ∋ (Y1, Y2, . . . ) →

i=1

δYi ∈ Conf ([0, ∞)) Conf (C) ∋

i=1

δzi →

i=1

δ|zi|2 ∈ Conf ([0, ∞)) .

.

.

3 Point processes on C defines probability measures on entire functions

by Hadamard product. How does a point process affect random entire function? Can we say something about absolute continuity from properties of random entire functions obtained from point processes?

Tomoyuki SHIRAI (Kyushu University) Ginibre point process and its Palm measures

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SLIDE 54

. . . . . .

舟木さん,: 還暦おめでとうございます.

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