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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook Large deviations for Brownian intersection measures Chiranjib Mukherjee Prague, September, 2011 Brownian intersection Brownian Intersection measure


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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations for Brownian intersection measures

Chiranjib Mukherjee Prague, September, 2011

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Brownian intersection

Brownian paths do intersect

W1, . . . , Wp independent Brownian motions in Rd running until times t1, . . . , tp. Typically, here d ≥ 2.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Brownian intersection

Brownian paths do intersect

W1, . . . , Wp independent Brownian motions in Rd running until times t1, . . . , tp. Typically, here d ≥ 2. Look at their path intersections: St =

p

  • i=1

Wi[0, ti) t = (t1, . . . , tp) ∈ (0, ∞)p

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Brownian intersection

Brownian paths do intersect

W1, . . . , Wp independent Brownian motions in Rd running until times t1, . . . , tp. Typically, here d ≥ 2. Look at their path intersections: St =

p

  • i=1

Wi[0, ti) t = (t1, . . . , tp) ∈ (0, ∞)p Dvoretzky, Erd¨

  • s, Kakutani and Taylor showed St is

non-empty with positive probability iff      d = 2, p ∈ N d = 3, p = 2 d ≥ 4, p = 1.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure

Intensity of the intersections

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure

Intensity of the intersections

A measure is naturally defined on St: ℓt(A) =

  • A

dy

p

  • i=1

ti ds δy(Wi(s)) A ⊂ Rd

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SLIDE 7

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure

Intensity of the intersections

A measure is naturally defined on St: ℓt(A) =

  • A

dy

p

  • i=1

ti ds δy(Wi(s)) A ⊂ Rd For p = 1, ℓt is the single path occupation measure: ℓ(i)

t (A) =

t ds 1A(Ws) i = 1, . . . , p

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SLIDE 8

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure

Intensity of the intersections

A measure is naturally defined on St: ℓt(A) =

  • A

dy

p

  • i=1

ti ds δy(Wi(s)) A ⊂ Rd For p = 1, ℓt is the single path occupation measure: ℓ(i)

t (A) =

t ds 1A(Ws) i = 1, . . . , p Note: If ℓ(i)

t

would have a Lebesgue density ℓ(i)

t (y), so would

ℓt and ℓt(y) =

p

  • i=1

ℓ(i)

t (y)

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SLIDE 9

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure

Intensity of the intersections

A measure is naturally defined on St: ℓt(A) =

  • A

dy

p

  • i=1

ti ds δy(Wi(s)) A ⊂ Rd For p = 1, ℓt is the single path occupation measure: ℓ(i)

t (A) =

t ds 1A(Ws) i = 1, . . . , p Note: If ℓ(i)

t

would have a Lebesgue density ℓ(i)

t (y), so would

ℓt and ℓt(y) =

p

  • i=1

ℓ(i)

t (y)

makes sense only in d = 1!

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SLIDE 10

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure

Intensity of the intersections

A measure is naturally defined on St: ℓt(A) =

  • A

dy

p

  • i=1

ti ds δy(Wi(s)) A ⊂ Rd For p = 1, ℓt is the single path occupation measure: ℓ(i)

t (A) =

t ds 1A(Ws) i = 1, . . . , p Note: If ℓ(i)

t

would have a Lebesgue density ℓ(i)

t (y), so would

ℓt and ℓt(y) =

p

  • i=1

ℓ(i)

t (y)

makes sense only in d = 1! Goal: Make precise the above as t ↑ ∞ (in particular, d ≥ 2).

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Wiener Sausages

Construction of intersection measure

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Wiener Sausages

Construction of intersection measure

Le Gall (1986) looked at Wiener sausages: S(i)

ǫ,t = {x ∈ Rd : |x − Wi(ri)| < ǫ}

i = 1, . . . , p

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Wiener Sausages

Construction of intersection measure

Le Gall (1986) looked at Wiener sausages: S(i)

ǫ,t = {x ∈ Rd : |x − Wi(ri)| < ǫ}

i = 1, . . . , p Normalise Lebesgue measure on the intersection of the sausages dℓǫ,t(y) = sd(ǫ) 1∩p

i=1S(i) ǫ ,t(y) dy

where

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Wiener Sausages

Construction of intersection measure

Le Gall (1986) looked at Wiener sausages: S(i)

ǫ,t = {x ∈ Rd : |x − Wi(ri)| < ǫ}

i = 1, . . . , p Normalise Lebesgue measure on the intersection of the sausages dℓǫ,t(y) = sd(ǫ) 1∩p

i=1S(i) ǫ ,t(y) dy

where sd(ǫ) =      π−p logp( 1

ǫ)

if d = 2 (2πǫ)−2 if d = 3 and p = 2

2 ωd(d−2) ǫ2−d

if d ≥ 3 and p = 1.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Wiener Sausages

Intersection measure: scaling limit of Lebesgue measure on sausages

Le Gall shows limit ǫ ↓ 0 gives the Brownian intersection measure: lim

ǫ→0 ℓǫ,t(A) = ℓt(A) in Lq for q ∈ [1, ∞)

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics

Single path measure

Look at one path. Fix i ∈ {1, . . . , p}.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics

Single path measure

Look at one path. Fix i ∈ {1, . . . , p}. Wi running in a compact set B in Rd until its first exit time τi from B.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics

Single path measure

Look at one path. Fix i ∈ {1, . . . , p}. Wi running in a compact set B in Rd until its first exit time τi from B. Make sure the path does not leave B by time t: Pt(·) = P(· ∩ {t < τi}).

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics

Single path measure

Look at one path. Fix i ∈ {1, . . . , p}. Wi running in a compact set B in Rd until its first exit time τi from B. Make sure the path does not leave B by time t: Pt(·) = P(· ∩ {t < τi}). Normalise the occupation measure: 1

t ℓ(i) t

∈ M1(B)

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics

Single path measure

Look at one path. Fix i ∈ {1, . . . , p}. Wi running in a compact set B in Rd until its first exit time τi from B. Make sure the path does not leave B by time t: Pt(·) = P(· ∩ {t < τi}). Normalise the occupation measure: 1

t ℓ(i) t

∈ M1(B) Want to study: Behavior of 1

t ℓ(i) t , as t ↑ ∞.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞:

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞: µ ∈ M1(B). Pt 1 t ℓ(i)

t

≈ µ

  • =
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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞: µ ∈ M1(B). Pt 1 t ℓ(i)

t

≈ µ

  • = exp [−t (I(µ) + o(1))]

t ↑ ∞ where

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞: µ ∈ M1(B). Pt 1 t ℓ(i)

t

≈ µ

  • = exp [−t (I(µ) + o(1))]

t ↑ ∞ where I(µ) =

  • 1

2

dx

  • 2

2

if dµ

dx ∈ H1 0(B)

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞: µ ∈ M1(B). Pt 1 t ℓ(i)

t

≈ µ

  • = exp [−t (I(µ) + o(1))]

t ↑ ∞ where I(µ) =

  • 1

2

dx

  • 2

2

if dµ

dx ∈ H1 0(B)

∞ else

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SLIDE 27

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞: µ ∈ M1(B). Pt 1 t ℓ(i)

t

≈ µ

  • = exp [−t (I(µ) + o(1))]

t ↑ ∞ where I(µ) =

  • 1

2

dx

  • 2

2

if dµ

dx ∈ H1 0(B)

∞ else Upshot: 1

t ℓ(i) t

possess densities ψ2 = dµ

dx , for large t.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large t-asymptotics for single path measure

Path densities show up

[Donsker-Varadhan (1975-83)], [G¨ artner (1977)]:

1 t ℓ(i) t

large deviation principle (LDP) in M1(B) under Pt as t ↑ ∞: µ ∈ M1(B). Pt 1 t ℓ(i)

t

≈ µ

  • = exp [−t (I(µ) + o(1))]

t ↑ ∞ where I(µ) =

  • 1

2

dx

  • 2

2

if dµ

dx ∈ H1 0(B)

∞ else Upshot: 1

t ℓ(i) t

possess densities ψ2 = dµ

dx , for large t.

Our Goal: Similar statement for intersection measure ℓt, for large t?

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

  • ccupation measure and intersection measure

ℓ(1)

t , . . . , ℓ(p) t

  • ccupation measures of p paths running until

time t in a bounded domain B until first exit times τ1, . . . , τp.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

  • ccupation measure and intersection measure

ℓ(1)

t , . . . , ℓ(p) t

  • ccupation measures of p paths running until

time t in a bounded domain B until first exit times τ1, . . . , τp. ℓt the intersection measure of p paths.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

  • ccupation measure and intersection measure

ℓ(1)

t , . . . , ℓ(p) t

  • ccupation measures of p paths running until

time t in a bounded domain B until first exit times τ1, . . . , τp. ℓt the intersection measure of p paths. Make sure no path exits B before time t: Pt(·) = P

  • ·

t < τ1 ∧ · · · ∧ τp

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

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SLIDE 33

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

  • = exp
  • − t
  • I(µ; µ1, . . . , µp)

+ o(1)

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SLIDE 34

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

  • = exp
  • − t
  • I(µ; µ1, . . . , µp)

+ o(1)

  • I(µ; µ1, . . . , µp) = 1

2

p

i=1 ∇ψi2 2 , if

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

  • = exp
  • − t
  • I(µ; µ1, . . . , µp)

+ o(1)

  • I(µ; µ1, . . . , µp) = 1

2

p

i=1 ∇ψi2 2 , if

    

dµi dx = ψ2 i , ψi ∈ H1 0(B), ψi2 = 1

  • ccupation densities for large t
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SLIDE 36

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

  • = exp
  • − t
  • I(µ; µ1, . . . , µp)

+ o(1)

  • I(µ; µ1, . . . , µp) = 1

2

p

i=1 ∇ψi2 2 , if

    

dµi dx = ψ2 i , ψi ∈ H1 0(B), ψi2 = 1

  • ccupation densities for large t

dµ dx = ψ2p

intersection density for large t

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SLIDE 37

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

  • = exp
  • − t
  • I(µ; µ1, . . . , µp)

+ o(1)

  • I(µ; µ1, . . . , µp) = 1

2

p

i=1 ∇ψi2 2 , if

    

dµi dx = ψ2 i , ψi ∈ H1 0(B), ψi2 = 1

  • ccupation densities for large t

dµ dx = ψ2p

intersection density for large t ψ2p = p

i=1 ψ2 i

intersection density as product of occupation densities

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Intersection densities as product of occupation densities

Pt

  • ℓt

tp ≈ µ; ℓ(1)

t

t ≈ µ1, . . . , ℓ(p)

t

t ≈ µp

  • = exp
  • − t
  • I(µ; µ1, . . . , µp)

+ o(1)

  • I(µ; µ1, . . . , µp) = 1

2

p

i=1 ∇ψi2 2 , if

    

dµi dx = ψ2 i , ψi ∈ H1 0(B), ψi2 = 1

  • ccupation densities for large t

dµ dx = ψ2p

intersection density for large t ψ2p = p

i=1 ψ2 i

intersection density as product of occupation densities else, I = ∞ identically

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Large deviations: diverging time

Extension of classical theory

Theorem (K¨

  • nig/M (2011))

The family of tuples ℓt

tp ; ℓ(1)

t

t , . . . , ℓ(p)

t

t

  • satisfies a LDP under Pt, as

t ↑ ∞, with rate function I(µ; µ1, . . . , µp) = 1 2

p

  • i=1

∇ψi2

2

if µ and µ1, . . . , µp have densities ψ2p and ψ2

1, . . . , ψ2 p respectively,

ψi ∈ H1

0(B), ψi2 = 1 and ψ2p = p i=1 ψ2 i , else I = ∞.

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure LDP

Large deviations: diverging time

Specialising onto the first entry of tuples, (µ, µ1, . . . , µp) → µ and use the contraction principle to get

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Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure LDP

Large deviations: diverging time

Specialising onto the first entry of tuples, (µ, µ1, . . . , µp) → µ and use the contraction principle to get Corollary The family of measures ℓt

tp

  • satisfies a large deviation principle,

under Pt, as t ↑ ∞, with rate function J(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), ||ψi||2 = 1, p

  • i=1

ψ2

i = dµ

dx

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SLIDE 42

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure LDP

Large deviations: diverging time

Specialising onto the first entry of tuples, (µ, µ1, . . . , µp) → µ and use the contraction principle to get Corollary The family of measures ℓt

tp

  • satisfies a large deviation principle,

under Pt, as t ↑ ∞, with rate function J(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), ||ψi||2 = 1, p

  • i=1

ψ2

i = dµ

dx

  • p = 1: We recover classical Donsker-Varadhan theory for one path.
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SLIDE 43

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

A related problem: Upper tail asymptotics

large intersections in a set

U ⊂ B

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SLIDE 44

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

A related problem: Upper tail asymptotics

large intersections in a set

U ⊂ B Study: P(ℓ(U) > a) as a ↑ ∞?

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SLIDE 45

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

A related problem: Upper tail asymptotics

large intersections in a set

U ⊂ B Study: P(ℓ(U) > a) as a ↑ ∞? [K¨

  • nig and M¨
  • rters (2001)]:

lim

a→∞ a− 1

p log P [ℓ(U) > a] = −Θ(U)

for Θ(U) = inf p 2 ||∇ψ||2

2 : ψ ∈ H1 0(B), ||1Uψ||2 2p = 1

  • .
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SLIDE 46

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Euler-Lagrange equations

Minimiser(s) to Θ(U) exist(s). Every minimising ψ solves △ψ(x) = −2 pΘ(U)ψ2p−1(x) 1U(x) for x ∈ B\∂U

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SLIDE 47

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Euler-Lagrange equations

Minimiser(s) to Θ(U) exist(s). Every minimising ψ solves △ψ(x) = −2 pΘ(U)ψ2p−1(x) 1U(x) for x ∈ B\∂U Open: For p > 1, is the minimizer or the solution ψ unique? (unique if U = B(0; 1) and B = R3, rotational symmetry)

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SLIDE 48

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Euler-Lagrange equations

Minimiser(s) to Θ(U) exist(s). Every minimising ψ solves △ψ(x) = −2 pΘ(U)ψ2p−1(x) 1U(x) for x ∈ B\∂U Open: For p > 1, is the minimizer or the solution ψ unique? (unique if U = B(0; 1) and B = R3, rotational symmetry) p = 1:

the solution is unique (Rayleigh-Ritz)

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SLIDE 49

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Euler-Lagrange equations

Minimiser(s) to Θ(U) exist(s). Every minimising ψ solves △ψ(x) = −2 pΘ(U)ψ2p−1(x) 1U(x) for x ∈ B\∂U Open: For p > 1, is the minimizer or the solution ψ unique? (unique if U = B(0; 1) and B = R3, rotational symmetry) p = 1:

the solution is unique (Rayleigh-Ritz) ψ2 appears as large-a density of the occupation measure on U.

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SLIDE 50

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Euler-Lagrange equations

Minimiser(s) to Θ(U) exist(s). Every minimising ψ solves △ψ(x) = −2 pΘ(U)ψ2p−1(x) 1U(x) for x ∈ B\∂U Open: For p > 1, is the minimizer or the solution ψ unique? (unique if U = B(0; 1) and B = R3, rotational symmetry) p = 1:

the solution is unique (Rayleigh-Ritz) ψ2 appears as large-a density of the occupation measure on U.

Upshot: ψ2p should be the large-a density of the intersection measure on U.

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SLIDE 51

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Law of large masses

Let L =

ℓ ℓ(U) be the normalised probability on U.

slide-52
SLIDE 52

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Law of large masses

Let L =

ℓ ℓ(U) be the normalised probability on U.

M = {µ ∈ M1(U) : µ( dx) = ψ2p(x) dx, ψ minimises Θ(U)}

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SLIDE 53

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Law of large masses

Let L =

ℓ ℓ(U) be the normalised probability on U.

M = {µ ∈ M1(U) : µ( dx) = ψ2p(x) dx, ψ minimises Θ(U)} [K¨

  • nig and M¨
  • rters (2005)]

lim

a↑∞ P[d(L, M) > ǫ| ℓ(U) > a] = 0

where d weakly metrises M1(U)

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SLIDE 54

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Law of large masses

Let L =

ℓ ℓ(U) be the normalised probability on U.

M = {µ ∈ M1(U) : µ( dx) = ψ2p(x) dx, ψ minimises Θ(U)} [K¨

  • nig and M¨
  • rters (2005)]

lim

a↑∞ P[d(L, M) > ǫ| ℓ(U) > a] = 0

where d weakly metrises M1(U) Upshot: Law of large numbers: L → ψ2p under P(·| ℓ(U) > a), a ↑ ∞

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SLIDE 55

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Minimisers and path behavior

Law of large masses

Let L =

ℓ ℓ(U) be the normalised probability on U.

M = {µ ∈ M1(U) : µ( dx) = ψ2p(x) dx, ψ minimises Θ(U)} [K¨

  • nig and M¨
  • rters (2005)]

lim

a↑∞ P[d(L, M) > ǫ| ℓ(U) > a] = 0

where d weakly metrises M1(U) Upshot: Law of large numbers: L → ψ2p under P(·| ℓ(U) > a), a ↑ ∞ Large deviations: What is the exponential decay rate?

slide-56
SLIDE 56

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Intersection measure until exit times

Large deviations: diverging mass

Theorem (K¨

  • nig/M (2011))

The normalized probability measures L =

ℓ ℓ(U) satisfy a large

deviation principle under P(·|ℓ(U) > a), as a ↑ ∞, with rate function Λ(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), p

  • i=1

ψ2

i = dµ

dx

  • − Θ(U).
slide-57
SLIDE 57

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Outlook

Questions we can chew on

Study the variational formula for the rate function: J(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), ||ψi||2 = 1, p

  • i=1

ψ2

i = dµ

dx

slide-58
SLIDE 58

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Outlook

Questions we can chew on

Study the variational formula for the rate function: J(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), ||ψi||2 = 1, p

  • i=1

ψ2

i = dµ

dx

  • Open question: Can the minimisers be taken at

ψ1 = · · · = ψp? same optimal strategy?

slide-59
SLIDE 59

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Outlook

Questions we can chew on

Study the variational formula for the rate function: J(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), ||ψi||2 = 1, p

  • i=1

ψ2

i = dµ

dx

  • Open question: Can the minimisers be taken at

ψ1 = · · · = ψp? same optimal strategy? If so, rate function is much simpler! J(µ) = p 2

dµ dx 1

2p

  • 2

2

slide-60
SLIDE 60

Brownian intersection Brownian Intersection measure Main results: Large deviations Outlook

Outlook

Questions we can chew on

Study the variational formula for the rate function: J(µ) = inf 1 2

p

  • i=1

||∇ψi||2

2 : ψi ∈ H1 0(B), ||ψi||2 = 1, p

  • i=1

ψ2

i = dµ

dx

  • Open question: Can the minimisers be taken at

ψ1 = · · · = ψp? same optimal strategy? If so, rate function is much simpler! J(µ) = p 2

dµ dx 1

2p

  • 2

2

Extend it to unbounded domains.: For p = 2, B = R3