Analytic Urns Philippe Flajolet, INRIA Rocquencourt, F . With Kim - - PDF document

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Analytic Urns Philippe Flajolet, INRIA Rocquencourt, F . With Kim - - PDF document

January 20, 2003 Analytic Urns Philippe Flajolet, INRIA Rocquencourt, F . With Kim Gabarro and Helmut Pekari, Barcelona 1 General: BALLS and one or more URNS. Two kinds of models Balls-and-bins: Throw balls at random into a number


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SLIDE 1

January 20, 2003

Analytic Urns

Philippe Flajolet, INRIA Rocquencourt, F . With Kim Gabarro and Helmut Pekari, Barcelona

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SLIDE 2

General: BALLS and one or more URNS. Two kinds of models

“Balls-and-bins”: Throw balls at random into a

number of urns. = Random allocations. Basic in the analysis of hashing algorithms; also SAT problem, cf V . Puyhaubert. = Techniques: Exponential generating functions and saddle point. Poissonization &c.

Kolchin et al., Random Allocations, 1978.

“Urn models”: One urn contains balls whose

nature may randomly change according to ball drawn and finite set of rules.

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SLIDE 3

Here: URNS with BALLS of TWO COLOURS Type I Type II Black White RULES are given by a

✁ ✂ ✁ Matrix

The composition of the urn at time 0 is fixed. At time

✄ , a ball in

the urn is randomly chosen and its colour is inspected (thus the ball is drawn, looked at and then placed back in the urn): if it is black, then

black and

white balls are subsequently inserted; if it is white, then,

black balls and

✞ white balls are

inserted.

drawn added

✟ ✠ ✡ ✠ ☛ ☞ ✡ ✌ ✍✏✎

3

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SLIDE 4 ✑ Drawing with replacement = ✒ ✒ ✒ ✒

.

✑ Drawing without replacement = ✓ ✔ ✒ ✒ ✓ ✔

.

✑ Laplace’s “melancholic” model [1811]: if a ball is

drawn, it is repainted black no matter what its colour is.

✒ ✒ ✔ ✓ ✔ ✑ Ehrenfest & Ehrenfest = ¨

Uber zwei bekannte Einw ¨ ande gegen das Boltzmannsche

  • Theorem,
  • 1923. Irreversibility contradicts Ergodicity.

Exchanges of basic balls (“atoms of heat”) between two urns, one cold and one hot

✖ ✓ ✔ ✔ ✔ ✓ ✔

Bernoulli [1768], Laplace [1812].

4

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SLIDE 5 ✗ P´
  • lya Eggenberger model. A ball is drawn at

random and then replaced, together with

✘ balls
  • f the same colour.
✘ ✙ ✙ ✘

A model of positive influence. Closed form.

✗ “Adverse influence” model ✙ ✘ ✘ ✙

Used in epidemiology, etc.

✗ The special search tree model ✚ ✛ ✜ ✢ ✚ ✜

Yao [1978]; Bagchi and Pal [1985]; Aldous et al [1988]; Prodinger & Panholzer [1998]

5

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SLIDE 6

Johnson & Kotz, Urn Models and their Application, Wiley 1973 Here case of a

✣ ✤ ✣ -matrix ✥ ✦ ✧ ★

with constant row-sum

✩ ✩ ✪ ✫✭✬ ✥ ✮ ✦ ✬ ✧ ✮ ★✰✯

At time

size

✲✴✳ satisfies ✲✴✳ ✬ ✲✴✵ ✮ ✪ ✱ .

Constant increment

A problem with three parameters + two initial conditions.

Kotz, Mahmoud, Robert [2000] show “pathologies’ in some of the other cases. Huge literature: Math. Reviews TITLE=urn : Number of Matches=186’’

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SLIDE 7

Lead to amazingly wide variety of behaviours, special functions, and limit distributions. Methods

✷ Difference equations and explicit solutions. ✷ Same but with probability generating functions. ✷ Connection with branching processes. ✷ Stochastic differential equations [KMR] ✷ Martingales [Gouet]

Here: A frontal attack: — PDE of snapshots at time

— Usual solution for quasilinear PDE — Bivariate GF and singularity perturbation Conformal mapping argument, Abelian integrals

  • ver Fermat curves
✹✻✺ ✼ ✽✾✺ ✿ ❀

+ Special solutions with elliptic functions

7

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SLIDE 8

Part I

The

❁❃❂❅❄ model—basic equations ❆ ❁ ❄ ❇ ❆ ❄ ❈ Insertions in a 2–3 tree: 2–node ❉❊

3–node; 3–node

❉❊

(2–node + 2–node).

❈ Fringe-balanced 2–3 tree analogous to

median-of-three quicksort. Mahmoud [1998]; Panholzer–Prodinger [1998]

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SLIDE 9

Evolution is:

  • ■❍
❏▲❑ ❋ ▼✾◆❖❋ ▼◗P❘●❙❍ ❚❯ ❱ ❯❲ ◆❳❏

with probability

❋ ▼▲P❘● ❨ ❩❳❬

with probability

❭ ◆ ❋ ▼◗P❘● ❨

. Let

❪ ▼▲❫❵❴ ❍ ❛❝❜❞❋ ▼ ❍ ❡❣❢ , ❪ ▼ ❜✐❤❥❢❧❦❅❍ ❴ ❪ ▼◗❫♠❴ ❤ ❴

, and

♥ ❜♣♦rqs❤t❢✉❦❅❍ ▼▲✈❘● ❪ ▼ ❜✐❤❥❢✇❤ ▼ ❍ ▼▲❫❵❴ ❪ ▼◗❫♠❴ ❤ ❴ ♦ ▼ q

whose elicitation is our main target. Lemma: PDE satisfied by BGF of probabilities is

❜✐❤②①③♦④◆ ❤t❢✰⑤ ♥ ⑤ ♦ ❩ ❜ ❭ ◆ ❤⑦⑥⑧❢✰⑤ ♥ ⑤ ❤ ❩ ❤⑦①⑨♥ ❩ ❤⑦⑩✏❍ ❶❸❷
  • PROOF. Each
❪ ▼

is determined from previous one by

⑤❺❹

= a differential recurrence. Gives PDE for bivariate generating function

♥ .

Take

❪❼❻ ❜✐❤❥❢ that satisfies PDE and write ❽ ❦❅❍ ❪ ❻ ❜✐❤t❢ ❩ ♥ ❜♣♦rq❾❤❥❢ . then, we get a homogeneous PDE. ❜❿❤⑦①➀♦➁◆ ❤❥❢ ⑤ ❽ ⑤ ♦ ❩ ❜ ❭ ◆ ❤⑦⑥➂❢ ⑤ ❽ ⑤ ❤ ❩ ❤⑦① ❽ ❍ ❶❸❷

with

❪ ❻ ❜✐❤t❢➃❍ ❜ ❭ ◆ ❤✾⑥➂❢
  • ➅➄
⑥ ❹ ❻ ➆ ⑩➇❜ ❭ ◆ ➆ ⑥➈❢ P❃➉➊➄ ⑥➌➋ ➆ ❷

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SLIDE 10

Quasilinear first-order PDE’s are reducible to ODEs.

➍ ➎✇➏②➐➒➑✉➐➀➓ ➔❸→ ➓ ➎➣➏⑦➐↔➑↕➔ → ➏ ➙ ➛ ➎➣➏⑦➐↔➑➜➐⑨➓ ➔◗→ ➓ ➎✇➏②➐➒➑➝➔ → ➑ ➙ ➞ ➎➣➏⑦➐↔➑➜➐⑨➓ ➔■➟ ➠
  • 1. Look for a solution in implicit form
➡ ➢➥➤r➦❾➧❝➦✴➨➫➩➯➭ ➲ . ➳ ➢♣➤r➦s➧❝➦❾➵➁➩➺➸ ➡ ➸ ➤ ➻ ➼ ➢➥➤r➦➽➧❝➦❾➵➁➩✰➸ ➡ ➸ ➧ ➾ ➚ ➢♣➤❣➦➽➧❝➦❾➵➁➩➺➸ ➡ ➸ ➵ ➭ ➲❸➪
  • 2. Consider the ordinary differential system
➶ ➤ ➳ ➭ ➶ ➧ ➼ ➭ ➾ ➶ ➵ ➚ ➪

The solution of two “independent” ordinary differential equations, e.g.,

➶ ➧ ➼ ➭ ➾ ➶ ➵ ➚

and

➶ ➤ ➳ ➭ ➶ ➧ ➼ ➦

leads to two families of integral curves,

➹ ➢✐➧➘➦➴➤r➦❾➵➁➩➃➭ ➚➬➷

and

➮ ➢✐➧❝➦➱➤❣➦➽➵④➩➃➭ ➚❙✃ ➪
  • 3. The generic solution of the PDE is provided by
➡ ➢♣➤r➦❾➧➘➦➽➵④➩➃➭ ❐❒➢ ➹ ➢✐➧➘➦➱➤r➦➽➵➁➩✴➦➒➮ ➢✐➧➘➦➱➤r➦➽➵➁➩➽➩✴➦

for arbitrary bivariate

❐ . Solving for ➵

in

➡ ➢♣➤r➦❾➧➘➦❾➵④➩❮➭ ➲

provides a relation

➵ ➭ ❰④Ï➯➢♣➤r➦❾➧❥➩ . General solution is ➨ ➢➥➤r➦❾➧t➩❧Ð❅➭ ❰ Ï ➢♣➤r➦➽➧❥➩✴➪

10

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SLIDE 11 Ñ➥Ò↕ÓÕÔ Ö Ò➝×◗Ø↕Ù Ø Ô Ú Ñ➴Û➁Ö Ò❝ÜÝ×❸Ø↕Ù Ø Ò Ú Ò↕Ó Ù Þ ß❃à

Consider

á Ò ÛâÖ Ò Ü Þ á Ô Ò Ó Ô Ö Ò Þ Ö árã Ò Ó ã à ä á Ò å árã

first integral by separation:

ã Ñ➴ÛâÖ Ò Ü ×➀æ➜ç➊è Ü Þ é ç à ä á Ò å á Ô variation of constant: Ô❘Ñ➴Û➁Ö Ò➌ÜÝ× ç➊è Ü Ú ê ë ì Ñ➴Û➁Ö ì Ü × Ó è Ü á ì Þ é➁í❺à

Bind the two integrals by arbitrary

î

&

ã ï Ù î Ù Ñ➊Û➁Ö Ò Ü × ç➴è Üñð Ô❥Ñ➊Û➁Ö Ò❝ÜÝ× ç➴è Ü Ú ê ë ì Ñ➊Û➁Ö ì Ü × Ó è Ü á ì Þ ß ð

Solve for

Ù , introducing arbitrary ò : Ù Ñ✇Ô ð Ò➝× Þ ó ÑôÒ↕× ò Ñ ó Ñ➥Ò➝×➊Ô Ú õ Ñ➥Ò➝×➒× ð õ ÑôÒ➝×❳ö Þ ê ë ì Ñ➴Û➁Ö ì Ü × Ó è Ü á ì ð

with

ó Ñ➥Ò➝×❳ö Þ Ñ➴Û➁Ö Ò Ü × ç➴è Ü .

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SLIDE 12

Initial conditions identify

÷ .

Theorem 1. Define the quantities

ø✾ù➥ú➝û ü ù➊ýâþ ú❝ÿÝû✁✄✂ ÿ✆☎ ✝ ùôú↕û ü ✞ ✟ ✠ ù➴ý➁þ ✠ ÿ û☛✡ ✂ ÿ ☎ ☞ ùôú➝û ü ✞ ✟ ✠✍✌ ù➴ýâþ ✠ ÿ û☛✎ ✂ ÿ ✏ ✠✒✑

(1) Then, the bivariate generating function of the probabilities is

✓ ù✕✔✖☎➒ú➝û ü ø✾ùôú↕û ÷ ù✕✔❣ø✾ù➥ú➝û✘✗ ✝ ù➥ú➝û↔û✙☎

(2) where

÷

is the function defined parametrically for

✚ ú ✚✜✛ ý by ÷ ù ✝ ùôú➝û➒û ü ☞✏ù➥ú➝û ✑

(3)

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Dominant singularities of

✢ ?

The diagram that summarizes

is

✣ ✤ ✥ ✦ ✧ ★✪✩✫✣✭✬ ✮ ✯✱✰ ✢ ✩✕✦✲✬✳✧ ✴✵✩✫✣✭✬✷✶

The radius of analyticity of

is

✸ ✧ ★✪✩✍✹✺✬✷✻ ★✪✩✼✣✭✬✵✽✾✧ ✿ ❀ ❁ ✩✍✹ ✯ ❁❃❂ ✬❃❄❆❅ ❂ ❇ ❁ ✻

Proof: There is local (analytic) invertibility of

❈❊❉●❋■❍ along ❉❑❏▼▲❖◆P❍ . Thus ◗

is analytic along

❉✫❏▼▲❘◆P❍ .

We have

◗❙❉❑❚❯❍❲❱ ❳ ❉✫❚❨▲❖❏❩❍ which has nonnegative coeffs

and is Pringsheim. We have

❈❊❉❘❬❭❍❫❪ ❴

while

❵❛❉❘❬❭❍❛❱ ❴

. Thus

◆ is a singularity.

By Eulerian Beta integrals:

◆ ❜ ❈❊❉❘❬❭❍✘❱ ❬ ❝❡❞ ❉ ❬ ❝ ▲ ❬ ❢ ❍❛❱ ❬ ❝✵❣ ❉❘❬❭❤ ❢ ❍ ❣ ❉❘❬❭❤ ❝ ❍ ❣ ❉✐❬❭❤❦❥❧❍ ♠ ❱ ❬ ♠ ♥ ❏♦❥P❬✒♣✘❥P❬✷❏♦q ❢ ❥✺q ♥ q ♥ ♠ ◗sr☛t ◗✈✉❘✇ ①✐②④③ ♠ ❱ ❬ ♠ ♥ ❏♦❥P❬✒♣❛❥P❬✷❏♦q ❢ ❥✺q ♥ q⑥⑤ ▲

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SLIDE 14

Local expansions near

⑦ ⑧ ⑨ plus symmetries of the

problem are compatible with: Proposition 1. There are no singularities of

⑩ ❶✕❷✲❸
  • n
❹❺❷❡❹❻⑧ ❼ other than ❼ , ❼❨❽ , ❼❨❽❿❾ that are simple
  • poles. Precisely, let
➀ ❶✕❷✲❸➁⑧ ⑨ ❼ ➂ ❷ ➃ ⑨ ❼▼❽ ➂ ❷ ➃ ⑨ ❼❨❽ ❾ ➂ ❷ ⑧ ➄ ❷✜❾ ❼⑥➅➆➂ ❷❨➅❛➇

The function

⑩ ❶✕❷✲❸❫➂ ➀ ❶✕❷✲❸

is analytic in a disc

❹➈❷✱❹✜➉ ➊

for some

satisfying

➊ ➋ ❼ . (One can take ➊ ⑧ ➌❩❼ .)

Why singularities of

⑩ , BTW? ➍ ❶✕❷✖➎☛⑦✭❸➏⑧ ➐➑❶✫⑦✭❸❖⑩ ❶➒❷❨➐➑❶✫⑦✭❸ ➃ ➓ ❶✼⑦✪❸➔❸✷➎ ⑩ ❶ ➓ ❶✫⑦✭❸➔❸➁⑧ →➣❶✼⑦✪❸ ➇

Set

⑦ ⑧ ↔ and estimate ↕➙❷➜➛⑥➝➞⑩ ❶✕❷✲❸ : Get extremely

large deviations, all balls of one colour. Know approximately

↕➙❷ ➛ ➝ ➍ ❶➒❷➟➎➔⑦✪❸ = PGF of

distribution

LIMIT LAW. Set

to value

➡ ⑧ ⑨ and get LARGE DEVIATIONS.

And a good deal more. . .

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SLIDE 15

Part II

The

➢➥➤➧➦ model—elliptic structure

Recall: an elliptic function is a doubly periodic meromorphic function in

➨ .

Historically: Integration over a conic

➩ ➫ ➭✫➯❨➲✐➳✜➵ where ➳ ➸ ➺ ➭●➻➟➵ and ➼❨➽➚➾➪➺ ➸ ➶❦➲❃➹ , yields functions like ➘➷➴④➬➱➮❃➘❐✃ , ➘➷➴④➬✁❒④❮❰✃

and hyperbolic counterparts. Such functions satisfy

➘➷➴④➬❆➮✍➘❐✃Ï➭✫➯❯➵❛Ð ➸ ➘➷➴④➬➱➮❃➘❐✃■➭✫➯❯➵ÏÑ Ò❯Ó

so that inverses are simply periodic. This is a way to (re)build trigonometry from integrals over conics. Integration over a cubic or a quartic

➳ ➸ ➺ ➭●➻➟➵ with ➼❨➽➚➾➪➺ ➸ ÔP➲❘Õ , which are topologically “doughuts” leads

to double periodicity. Such things occur when rectifying the ellipse hence the name elliptic integrals and elliptic functions for inverses.

Ö ➶❭×P➭✫➯ÙØ Ú➪➵ÜÛ

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SLIDE 16

For a parameterized curve,

Ý Þ✫ß✪Þ✼à✪á➔áãâ ä➣Þ✼à✪á ,

examine all possible paths in the

à -plane, and the

corresponding determinations of

ß✪Þ✫à✭á . Reflect on Ý å æ çPè è â àêé

which defines

Ý Þ✼ëíìPî✵à✭á✳â à , that is, Ý Þ✕ï✲á✳â ð❧ñ .

Here:

Ý Þ✫ß✪Þ✼à✪á➔á➏â ä➣Þ✼à✭á ß✪Þ✫à✭á➁â ò å ó ô➷õ❆ô ö æø÷ ô❑ùøúüû❖ýþù é ß✪Þ✼à✪á➁â ò å ó ô❑ÿ❊õ❆ô ö æ➱÷ ô✫ù➔ú✁④ý➒ù ✂

The curve is

è☎✄✝✆ ✞✟✄ â ✠ and has genus 10.

Go step by step.

✡ The elementary triangle ✡ The fundamental triangle

16

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SLIDE 17

–2 –1 1 2 –3 –2 –1 1 2 3

The region

☛✌☞ (left) and a rendering of the six-sheeted

Riemann surface

  • f
✎✑✏✓✒✕✔✗✖ ✏✙✘✛✚ ✒✢✜✣✔✥✤✧✦★✜ for ✒

near 1 (right).

Because of double parameterization, taking

in a half-plane suffices.

17

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SLIDE 18

Lemma 1. The function

maps the interior of

✫✭✬ ✮✰✯ ✱ ✲ in a one-to-one manner on the interior of

the equilateral triangle

with vertices

✴✶✵✷✴✢✸✹✵✷✴✺✸✼✻ ,

where

✸ ✽✿✾ ❀❁✻☎❂❄❃✺❅❇❆ .
  • Proof. Folds angles in an appropriate way. . .

Start with Elementary triangle.

❈ ❉ ❀ ✻✷❂❄❃✺❅❇❊ ❋ ✾❍● ■ ✫ ❋ ✲ ❈ ■ ✫ ❉ ✲ ✾ ✴ ■ ✫✧❏ ❀ ✻✷❂❄❃❑❅▼▲◆✻ ✲ ■ ✫ ❀ ✻✷❂❄❃✺❅❇❊ ✲ ✾ ✴✺✸

The “elementary triangle”

❖◗P (right) is the image of the basic

sector

❘❙P (left) via the mapping ❚ ❯❱ ❲❨❳❩❚✕❬ . ✾❍● ❈ ❉ ❭ ❭ ✻ ✴ ❪ ■ ✫ ❉ ✲ ✴✢✸ ❪ ■ ✫ ❭ ✲ ✴✢✸❫✻ ❪ ■ ✫ ❭ ✻ ✲

The “fundamental triangle”

(right) is the image of the slit upperhalf plane

❳❵❴✌P✛❛ ❜ ❬ (left) via the mapping ❚ ❯❱ ❲❨❳❩❚✕❬ .

18

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SLIDE 19

Three elementary triangles assemble to form a fundamental triangle

❝❍❞ ❡ ❢ ❣ ❣✕❤ ✐ ❥ ❦♠❧ ❢♦♥ ✐✢♣ ❥ ❦♠❧ ❣ ♥ ✐✢♣ ❤ ❥ ❦♠❧ ❣ ❤ ♥

Based on

❦♠❧ ❣rq ♥ ❝ ♣s❦♠❧ q ♥ , where ❣❙t ❝ ❢ , ♣✈✉ ❝ ❢ .

–1 –0.5 0.5 1 –0.5 0.5 1

Another view of the image of

✇❵①✌②④③ ⑤ ⑥ by ⑦❨✇❩⑧✕⑥ giving the

fundamental triangle

⑨ : a representation of the images of rays

emenating from 0 and of circles centred at 0

19

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SLIDE 20

Lemma 2. The function

is analytic (holomorphic) in the disk

❶❸❷❹❶✕❺ ❻❽❼ stripped of the points ❼❿❾☎❼✢➀✹❾✷❼✢➀➂➁ .

(The function admits these three points as simple poles, as asserted in Prop. 1.)

Rotated copies of the fundamental triangle around

➃❽➄➅➃➇➆④➄➅➃➇➆♠➈

shown against the circle of convergence of

➉➋➊➍➌➏➎ .
  • Proof. Laces around
➐ ➑ ➒ and changes of

variables:

➓♠➔→➒♦➣✌↔ ➓♠➔✙➐♠➣➙↕ ➛➝➜➟➞➡➠✢➔➟➒➢↔ ➐♠➣➤➜→➞❇➠ .

20

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SLIDE 21

The full story and the elliptic connection

A lattice

with generators

➦❑➧➩➨ ➫ ➭ : ➥✼➯➲➦❑➧✧➨➵➳④➸ ➺✑➻➽➼★➦✈➾ ➻➪➚✷➨ ➶ ➶ ➻❍➼➹➧✥➻❿➚➘➫ ➴✌➷✼➬

The Weierstraß zeta function relative to

is classically defined as

➮ ➯✃➱✢❐★➥❒➳✌❮❰➸ Ï ➱ ➾ ÐÒÑ➏Ó➵Ô✷Õ➩Ö❇× Ï ➱➘Ø Ù ➾ Ï Ù ➾ ➱ Ù ➚ ➬

Theorem 2. The

Ú -function of the Û ➚➡ÜÞÝ model intialized

with 2 balls of the first type (

ß Ö ➸ à Ö ➸ á ) is exactly Ú✼➯✃➱â➳④➸ Ï ã✕ä å Ø ➮ ➱➘Ø ã ã✕ä å ➾ ➮ Ø Ï ä å ➧ ã ❮❰➸ Ï æ ç ➯ ➼ Ý ➳ ç ➯ ➼ è ➳ ç ➯ ➼ ➚ ➳ ➧

(4) where

➮ ➯✁➱❽➳✌❮❰➸ ➮ ➯✃➱✢❐★➥êé✷ë✙ì♦➳ is the Weierstraß zeta function of

the hexagonal lattice:

➥ é✷ë✙ì ❮❰➸ í✟➻➽➼✷î➹ïñðâò è ➾ ➻➪➚➹î✑ó➝ïñðâò è ➶ ➶ ➻➽➼✣➧➩➻❿➚ô➫ ➴öõ ➬

21

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SLIDE 22

Proof.

÷ Follow all paths and examine ø♠ùûúêù✙üþý☎ý : any point ÿ

is reachable.

÷ There is a pole of ✂

at lattice points and residue is

✄ ☎ since determinations of ✆ ù✙ü♠ý in ø✞✝✠✟

are the same.

÷ By Liouville, ✂ ù ÿ ý and ✡ coincide (up to

normalization).

22

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SLIDE 23

O P ρ ρω ρω2

ζ2 1 ζ

A path in the

☛ -plane from ☞ to ✌

and the contour

above the

✎ -plane that realizes it via ✎ ✏✑ ☛✓✒ ✔✖✕ ✎✘✗ .

23

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SLIDE 24

Part III

Probabilistic consequences

Extract coeffs in simple fractions: Corollary 1. For the

✙✛✚✢✜✤✣ model, the probability

generating function

✥✧✦✩★✫✪✭✬✯✮ ✰✱★✲✪✞✳✯✴✧✬ admits an

exact formula valid for all

✵ ✶ ✷ , ✸✺✹✼✻✾✽✼✿❁❀ ❂✧❃ ✹❅❄❇❆❈✹❊❉●❋■❍ ❃ ❏ ✻❑✽✼✿✼▲ ▼✘◆ ❖ P ✻✾✽✛✿ ✻❑◗✩❘❚❙❱❯❳❲❅❨❬❩❭▲ ◗✧❪❱❙ ❍ ❯❳❲❅❨❬❩✠✿ ❍✺✹❫❍❴❘ ❵

where

❛ ★✫✪✭✬❝❜❞✮ ❡ ❢ ★✫✪✭✬ ❣ ❤ ✐ ❢ ★ ✐ ✬❦❥ ❧ ✐✢♠ ❢ ★✲✪✭✬♥✮ ★ ❡♣♦ ✪rq❊✬ ❣ts q❅✉

Note: when

✪ ✈ ❡ , this is like ❛ ★✫✪✭✬❱✇ ✦ ✇ ❣

.

24

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SLIDE 25

The Quasi-powers framework. Classics are: [Laplace] Given a random variable

, define its characteristic function aka Fourier transform as

②■③ ④⑥⑤⑧⑦❝⑨❶⑩ ❷❸④❺❹❼❻❾❽➀❿ ⑦ ⑩ ➁ ➂ ④➄➃ ⑩ ➅➆⑦❦❹❼❻❾❽ ➁ ⑩ ➇➈④➉❹❼❻❾❽➊⑦❱➋

If

➌✭➍ ⑩ ① ➎➐➏ ➑➒➑➓➑❊➏ ① ➍ with i.i.d. ① ➔ , then: ②✩→❅➣■④➀⑤❚⑦↔⑩ ④❺②r③ ④➀⑤❚⑦❚⑦ ➍ ➋

[L´ evy et al.] Fourier inversion is continuous: convergence of F .T.’s

↕❾➙➜➛ ➍➞➝ ➟ ② ❿ ➣ ④➀⑤❚⑦↔⑩ ②✭➠✓④➀⑤❚⑦

pointwise implies

➃ ➍ ➡ ➢

in distribution. [Berry-Esseen] Uniform distance on F .T. furthermore gives bounds on uniform distance on distribution functions.

25

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SLIDE 26

0.1 0.2 0.3 0.4 0.5 0.2 0.4 0.6 0.8 1

A Sedgewick plot of

➤➦➥➨➧❾➩➭➫ ➯ ➲➵➳➺➸ ➫❫➻❴➼ ➽●➾➪➚

for

➶ ➯ ➹❇➘➷➴t➴➺➬✢➮ (the

horizontal axis is normalized to

➶✃➱ ❐ ).

26

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SLIDE 27

Gaussian laws in analytic combinatorics

Classically

❒❰❮ Ï Ð Ñ✭Ò ÓÔÓÔÓÕÒ Ð ❮ , where Ð Ö have mean

and variance. Calculation shows that

×❳Ø❊Ù➷Ú ÛÝÜ●Þ❫ß à➀á ❒ ❮ â ã✼ä åræ ã ç â✺è ❮êé ë â áíì î ï

Hence Central Limit Theorem. A “good” uniform approximation

ð✺❮➪ñ❑ò✼ó➷ô õöñ✾ò✛órÓ✠÷ ñ✾ò✼ó ❮

for

ò ø ù (complex neighbourhood) is called QuasiPowers

approximation. From Bender, F .-Soria, Hwang (1995), one has: — Moments result from differentiation (complex an.) — Convergence to Gaussian distribution (erf) — Speed of convergence is

Ñ ú ❮ .

— Some large deviation estimates: probability of being far from mean at

û ã

for

û ü Ï ä

is exponentially small.

27

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SLIDE 28

Corollary 2 (Gaussian limit). For the

ý❴þ✠ÿ✁ model,

the random variable

✂ ✄

representing the number

  • f balls of the first type at time

is asymptotically Gaussian with speed of convergence to the limit

✆ ✝✟✞✡✠☞☛✍✌ þ✏✎ , ✑ ✂ ✒ ✓ ✔ ✝ ✂ ✒ ✎ ✕✖✂ ✒ ✗ ✘ ✙ ✚ ✛✢✜ ✣ ✤✦✥ ✧ ✤✩★✫✪✭✬✭✮✰✯✲✱✴✳ ✆ ✚ ✞ ✵
  • Proof. From lattice sum, in complex

neighbourhood

✶ ✷ ✚ : ✸ ✒✦✹ ✶✦✺ ✙ ✻ ✹ ✶✦✺ ✤ ✒ ✤☞✼ ✹ ✚ ✳ ✆ ✹ ✛ ✤ ✒ ✺✽✺ ✵

Note that

✾ ✿❁❀❃❂❅❄❇❆ plays the rˆ
  • le of a probability characteristic

function but it isn’t!

✾ ✿❁❀❃❂ ❄❇❆ ❈ ❉ ❊ ❈●❋■❍❑❏▼▲ ❊ ❈❖◆◗P✭❘ ❀❚❙ ▲ ❊ ❈ ❊◗❯❱❊ ❀❳❲✡❨ ❊ ❈ ❊❱❩◗❬ ❀✲❭ ▲ ❊ ❈ ❊ ◆◗◆ ❀✲❪ ▲ ❫✍❫✍❫❚❈

28

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SLIDE 29

The shape of moments. In the literature, only a few moments are computed via (unpleasant?) recurrence manipulations from probabilities and original rec. Here: everything is almost as though

❴❛❵❝❜❡❞❣❢✐❤ ❥ ❜❡❞❣❢❧❦ ❵ ❦♥♠ . ♦❇♣❱qsr✢t❛✉ ✈ r ✇ ① ♦③②④q⑤r⑥t⑦✉ ✈ r ⑧◗⑨ ✇ qs⑩◗❶❷r❹❸ ❺ ✇ t ① ♦❼❻④qsr✢t❛✉ ❽❿❾ ❽➁➀✽➂ ②➃♣➅➄ ❺✽➆ ✇ ⑧ r ② ❸ ❺❑➆ ⑨◗➇ r➅➈ ❺◗❺❑➉ ⑧◗⑨➋➊➍➌

Corollary 3 (Moments). For the

➎❇➏◗➐➒➑ model, exact

polynomial forms for moments of any order are available: the factorial moments satisfy

➓ ❜✽❜✟➔ ❵→❢✍➣ ❢✐❤ ↔ ➣ ❜✟↕ ➙ ➛➜❢◗➝ ↕ ➞ ➟➡➠✢➝

where the

↔ ➣ are polynomials generated by ➢④➤➦➥➍➧⑤➨➜➩➫❤ ➭ ➣✭➯✰➲ ➳ ➣ ➠③➵ ↔ ➣ ❜❡➸③❢

and

➺ ❜ ➳ ❢❹❤ ➻ ➼❁➽➚➾➪❥ ❜❿➛➶➙ ➳ ❢◗➹

Rota: polynomials of “binomial type” satisfying various convolution relations.

29

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SLIDE 30

Large deviations. From dominant poles of

➘ , corresponding to ➴ ➷ ➬ :

Corollary 4 (Extreme large deviations). The probability that, in the

➮❛➱✫✃✁❐ model, all balls are of

the first colour satisfies

❒●❮ ❐Ï❰➚ÐÑ➱➋Ò ➘ Ó ❮ÕÔ❹Ö ×⑥Ø❛Ù ❐ÏÚ Ù ❐ÜÛ✽Ý➶Þ ß Óáà Ù Ú Ô✍â❹ã

for any

à ä å .

Moreover: Corollary 5 (Large deviations). Let

æ

be a number of the open interval

Óá➬ ã❃ç è❃Ô . One has é❁ê⑤ë Ú✲ì í Ý î éðïòñôó Ó➁õ Ú ö æ ÷ î Ô ➷ ø Ø Óáæ Ô◗ã

(5) where the rate function

Ø is determined by Ø Óùæ Ô ➷ éðïòñ Óûú❇ü ý❇þ Óÿú ý Ô✽Ô→ã

(6) and

ú ý depending on æ

is the implicitly defined root

  • Óù➬
ã Ý Ô of ➴ þ ✁ Ó✟➴ Ô þ Ó✟➴ Ô Þ æ ➷ ➬✄✂

(7)

30

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SLIDE 31

Proof is standard for probabilists. Assume

☎✝✆✟✞✡✠☞☛✍✌ ✎ ✞✏✠✑☛ ✆

, where

✎ ✞✏✠✑☛ increases from ✒✔✓ to 1 as ✠ ✕ ✞✗✖✄✘✚✙✛☛ .

One has Cauchy aka saddle-point bounds:

✜ ✠✑✢✤✣✥☎ ✆ ✞✡✠✑☛✧✦ ☎✝✆✟✞✡✠ ✓ ☛ ✠ ✢ ✓ ✌ ✎ ✞✡✠ ✓ ☛ ✆ ✠ ✢ ✓ ★

Adopt the best

✠ ✓ (which must exist by some

convexity prop.) and get an exponentially small

  • upperbound. Cram ´

er aka “shifting the mean”: apply a form of CLT near

✠ ✓ to conclude that the

upperbound is also a lowerbound.

31

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SLIDE 32

0.05 0.1 0.15 0.2 0.25 0.3 0.2 0.4 0.6 0.8 1 0.05 0.1 0.15 0.2 0.25 0.3 0.1 0.2 0.3 0.4 0.5

Left: a Sedgewick plot of

✩✫✪ ✬ ✭✯✮✱✰✳✲✵✴✷✶✹✸ ✭ ✺ ✻✽✼✿✾ ✭✽❀ ✬ ❁❃❂❅❄

for

❆ ✺ ❇❃❈❊❉❋❉❍●✳■ (the horizontal axis is normalized to ❆❑❏ ▲ ); right: a

comparison against the large deviation rate (thick line).

32

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SLIDE 33

Related work

Gaussian law by moments: [Bagchi & Pal 1985]. Here global expression for moment polynomials +speed of convergence Elliptic connection related to [Panholzer & Prodinger 1998] via specific approach

▼❖◆P◆◗◆❙❘ ❚❯▼❱◆✱❲❨❳ ❚ . Here: much

more general, for whole class. Large deviations seem to be new. Local limit laws? Probably true. Want to apply saddle point, need bounding technique.

33

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SLIDE 34

Part IV

General case

Matrix drawn added

❩ ❬ ❭ ❬ ❪ ❫ ❭ ❴ ❵❜❛ ❪ ❝ ❫ ❞ ❴ ❝ ❵ ❞ ❡

Consider general case of urns with replacement, i.e.,

❪ ❢ ❣ , ❫ ❢ ❣ . ❤ ✐ ✐ ❝ ❡ ❥❦❝ ❡ ❤ ❥

A 3–parameter family Plus initially

✐♠❧ black; ❥ ❧ white.

34

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SLIDE 35

Ideas:

♥ Look at the enumerative version. ♥ Set up PDE for bivariate generating function via
  • perator
♦q♣sr . ♥ Get a t –function parameterized by Abelian

integrals over Fermat curve

✉✑✈ ✇ ①②✈ ③ ④ . ♥ Determine singularities by looking at geometry
  • f conformal maps of basic domains.
♥ Generally, non-elliptic solutions, but:

— Gaussian limit with speed of convergence; — Extreme large deviations; — Large deviation rate Recycles most of

⑤⑦⑥⑨⑧❶⑩ case but without double

periodicity at this level of generality.

35

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SLIDE 36

The operator approach Number balls in order of appearance

❷❹❸❻❺❙❸❻❼✄❸❾❽✚❽❾❽

choose 2

❿ ➀➂➁ ➃ ➄⑨➅✤➆❋➇✛➅ ➆

choose 5

❿ ➀➂➁ ➃ ➈✽➅❋➅❾➆❯➉➊➅❋➅✚➆➌➋✛➅❋➅❾➆

choose 8

❿ ➀➂➁ ➃ ➍✽➅✚➆➏➎q➅✚➆❋➐✽➅✤➆❋➑✽➅✚➆

choose 9

❿ ➀➂➁ ➃ ➎q➅✤➆❋➑✽➅✤➆➒➄➔➓→➅❋➅❾➆s➄✛➄⑨➅❋➅✚➆➒➄⑨➇✛➅❋➅❾➆ ➣ ↔ ↕ ➙ ➛ ➜ ; at time ➝ , after action, size is ➞➌➟ ; ➞❋➠ ↕ ➙ ➠ ➛ ➜ ➠ is given; ➞ ➟ ↕ ➞ ➠ ➛ ↔ ➝➡❽

Thus

➢ ➟ ↕ ➞❋➠➥➤➦➞➌➠ ➛ ↔✽➧☞➨❾➨❾➨ ➤➩➞❋➠ ➛ ➝ ↔→➧ ❽

Let

➢ ➟➭➫➲➯ be number of histories of length ➝

leading to

➳ Black (Type I) balls and ➢ ➤✗➵❅❸➏➸ ➧✧➺➻↕ ➟➭➫◗➯ ➢ ➟➭➫➲➯ ➸ ➯ ➵ ➟ ➝➡➼ ❽

36

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SLIDE 37

Combinatorial marking

differentiation Represent a particular history

with

➚ black balls

and

➪ white balls as ➶✑➹✛➘❖➴ .

Evolution chooses a black ball and acts; e.g., for

➷❅➬⑨➮❶➱ : ➶ ➹ ➘ ➴✑✃✟❐ ❒→❮✔❰ ➚♠➶ ➹ ➘ ➴ ✃✟❐ ❒ÐÏ❹ÑÓÒ➔Ô ➚♠➶ ➹✽Õ ➬ ➘ ➴✿Ö ➱❱×

Similarly for white balls. Cleverly introduce:

Ø Ù ✃ ➶ Õ❨Ú ➘ ➱ Û Û ➶ Ü ➶ÞÝß➘ Õ ➬ Û Û ➘ ×

Then

Ø ➶ ➹ ➘ ➴ describes all the successors of ➾ à ✃ ➶ ➹ ➘ ➴ .

All evolutions of length

á

are generated by

Øãâ ➶åä⑨æ✳➘❙ç❍æ , and a trivariate version of è

is

é è ê✗ë❅ì➏➶íì➏➘✄î Ù ✃ ïqðsñ ò ➶ ä⑨æ ➘ ç❍æ ×

37

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SLIDE 38

The basic PDE

ó By general principles: ô♠õ öø÷ õ➒ù❅úüû ý þ ÷ õsù❅ú ÿ ô♠õ ✁ ✂ ý þ ✄ ✁ ✂ ☎ ó By homogeneity, any term ✆ ý ✝✟✞✡✠☞☛✍✌✏✎

has

✑ ✒ ✓ ý ✔✖✕ ✒ ✗✙✘ : ✚✜✛✣✢ ✒ ✛✥✤ ✦ ✔ ✛ õ✣✧ ✆ ý ✗★✘ ✆ ÿ

where

✛ ✢ ✩ ✝ ô ✢ .

In summary, system of PDEs:

✪ ✫✭✬ ô♠õ ✁ ✂ ý þ ✄ ✁ ✂ ✚✮✛ ✢ ✒ ✛ ✤ ✦ ✔ ✛ õ ✧ ✁ ✂ ý ✗ ✘ ✁ ✂ ☎

Eliminate

ô ✤ and get ô♠õ ✁ ✂ ý ✝✰✯✲✱✳✠✵✴✷✶✸✱ ✛✥✢ ✁ ✂ ✒ ✝✰✴✷✶✺✹★✠✻✴✼✯✽✹✿✾✣✔ ✛ õ ✁ ✂ ✦ ✛✣✢ ✁ ✂ ✦ ✗✙✘ ✁ ✂ ❀ ☎

One can set

✠ ❁ ❂

and get

✂ ✚ ✌❅ÿ❃✝ ✧ ❁ ✂ ✚ ✌✡❄❃✝íÿ❃✠ ❅❆ ❂ ✧ : ❇❉❈❋❊❍● ■❑❏▼▲✻◆✮❖✵P❘◗❚❙❱❯❳❲ ❈❨▲✡◆✮❖✵P❩❖❭❬❪● ▲❭❬❴❫❛❵❜◗❩❙❞❝
  • ❡❩❢❣▲✡◆✮❖✵P✷❤❜✐✥❥❧❦
❈♠❏✏♥❚▲✵◗✺♦ ♣rq

38

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SLIDE 39

Apply general technology for first-order PDEs. Theorem 3. The probability of the urn defined by

matrix:

s✉t t✇✈ ① ② ✈ ① s ②

, initial cond

③ t❱④▼⑤❚⑥❚④ ③⑧⑦ t❞④❪✈ ② ④▼⑤

assuming it is tenable, is

⑨❶⑩✽❷❹❸✲❺❼❻ ❽ ❷❹❾ ❿ ➀✣❺ ❽ ➁❧➂❉➃ ➄❳➅ ➆ ⑩ ❽ ➁ ❾ ❿ ➂ ➃ ➄ ➅ ➇➉➈ ⑩➋➊❨➌ ❷ ➈✡➍ ❸✽❺➏➎

There

➌ ❷ ➈✡➍ ❸✽❺ is given by ➌ ❷ ➈✡➍ ❸✽❺➐❻ ➑❛❷❉❸✽❺ ➂♠➃❑➒ ❷ ➈ ➑❛❷❹❸✲❺ ➄ ❿ ➓✲❷❹❸✽❺❃❺ ➍

where

➔ ❻ ➆→❿ ➣ ❿ ↔ , ➑❛❷❉❸✽❺➙↕➛❻ ❷✷➀➝➜ ❸✽➞☞❺➠➟★➡➠➞ ➍ ➓✲❷❹❸✲❺➙↕➢❻ ➤ ➥ ➦✙➧✣➨ ➟ ➑❛❷ ➦ ❺ ➧➫➩✺➭ ➯ ➦

and the function

is defined implicitly by

➒ ❷❉➓✲❷❹❸✽❺❃❺➐❻ ❸ ➧ ➃ ➑❛❷❉❸✽❺ ➂ ➃ ➎

39

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SLIDE 40

Analytic aspects. Abelian integrals over Fermat curve

➲✲➳ ➵ ➸❛➳ ➺ ➻r➼

In general, global structure is not “clear”, but dominant singularities are OKay.

Consider the complex plane with

rays emanating from 0 and having directions given by all the

➽ th roots of

unity.

➾➋➚➝➪➹➶ ➘✏➴ ➘ ➶ ➷➮➬❑➱❐✃✳➴✺❒ ❮ ➷ ❮ ❰ ➴ Ï➠Ð✳Ñ ➽ ❮ Ò ❮ ÏrÓÔÐ➙Õ ÖØ×✮Ñ ➽ Ù

The image of

➾✍Ú by Û Ó❨Ü✻× is a quadrilateral, the

elementary kite with vertices at the points

❒r➴ Û Ó❚ÖØ× ➴ Û Ó✜Õ ❰ × ➴ Û Ó ➬➏ÝÞ➱àß❱á★â × Ù ã Û Ó ❒ × ãåä ➶ Û Ó❋ÖØ× ã Û Ó ➬ ÝÞ➱àß❱á★â × æ æ æ ç ç ç ã Û Ó✜Õ ❰ × è Ý❴é❃ß❱á★â è Ý❴ê❉ß❞á✙â èìë ß❱á★â èìë ß❱á★â

The elementary kite.

40

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SLIDE 41

Definition 1. The fundamental polygon of an urn model is the (closure of) the union of

í

regularly rotated versions of the elementary kite about the

  • rigin.

The elementary kite and the fundamental polygon of the urn

î ï ð ð î ï í ñ ò , ó ñ ô õ öø÷☞ù❼ú ö❉û î ÷➋ù➠üþý✷ÿ✁✄✂

41

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SLIDE 42

Theorem 4. The

function is analytic beyond its disc of convergence whose radius is

✆ ✝ ✞ ✟✡✠ ☛✌☞ ✟✎✍✑✏ ✟✓✒ ✝ ✞ ✟ ✔ ☛✖✕ ✗ ✒ ✔ ☛✙✘ ✗ ✒ ✔ ☛✚✕✜✛✢✘ ✗ ✒ ✣

It has an algebraic branch point at

✤ ✝ ✆ , where ☎ ☛ ✆ ✥ ✦ ✒★✧ ☛ ✆ ✥ ✦ ✒✪✩ ✕✬✫✪✘ ✣

(8) It is continuable beyond its circle of convergenc in a star-like domain.

  • Proof. Uses symmetries about origin, then

rotations around vertices.

Suffices to apply singularity analysis.

42

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SLIDE 43

Probabilisitic consequences Corollary 6. A quasipowers approximation holds but with weaker error terms than

✭✯✮✱✰✳✲ .

The limit law is Gaussian with speed of convergence

✴ ✵ ✶ ✷ ✸✺✹ .

Corollary 7. The large deviation rate exists and is expressible in terms of integrals over the Fermat curve. Corollary 8. The extreme large deviation rate is given explicitly in terms of Gamma function values at rational points.

43

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SLIDE 44

Part V

Special cases and explicitly solvable models

The urns

✻ ✻ ✻ ✻ ✼ ✽ ✾ ✻ ✻ ✽ ✾ ✼ ✽ ✾ ✾ ✻ ✻

correspond to: sampling with replacement or without replacement, and Coupon Collector. Solutions agree with basic combinatorics!

✿ ❀❂❁ ✼❄❃❆❅❈❇ ❃❊❉✱❋✬●■❍❏❉✱❋▲❑◆▼❖❋▲P❘◗ ✿ ❀❂❁ ✼❄❃❆❅❈❇ ❀❂❁ ❙ ❃❆❅ ❉ ❋ ❀❚❁ ❙ ✾ ❅ ▼ ❋✄❯ ✿ ❀❚❁ ✼❱❃❆❅❈❇ ❀
✽ ✾ ❙ ❃❆❅ ❉ ❋❲❯

44

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SLIDE 45

The Ehrenfest Urn

❳ Initially: 2 urns with balls moving

between them.

❳ A celebrated controversy: irreversibility versus

ergodicity.

❨ ❩ ❩ ❩ ❨ ❩

Balance is

❬ ❭ ❪ . One has ❫ ❭ ❴❵❭ ❩ , hence ❛ ❭ ❜ .

Start with

❫❞❝ ❭ ❡

.

One has

❢❤❣❥✐✯❦♠❧ ❣♦♥❈♣ ✐rqs❦✉t❖✈✇q , hence genus 0. ① ❣❥✐✯❦♠❧ ② ③ ④⑥⑤ ♥❈♣ ⑤ q ❧ ♥ ⑦⑨⑧❶⑩❸❷ ♥❺❹ ✐ ♥❈♣ ✐ ❧ ❻✬❼❽❻✚❾➀❿➁❣❥✐➂❦❄➃

The function

is defined implicitly by

➄➅❣➆❻✬❼❽❻✚❾➀❿✯❣➇✐➂❦♦❦✢❧ ✐ ➈ ♥❈♣ ✐ q ➉ ➊

which is equivalent to

➄➅❣➇➋➌❦◆❧ ➍✇➎➏❾➐❿ ➉ ➋ . ➑ ❣❘➒ ➊ ✐➂❦◆❧ ❣➓♥➔♣→✐ q ❦ ➉ ✈✇q ➍✇➎➏❾➀❿ ➉ ❣❘➒❲❹➣❻✬❼❽❻✚❾➀❿↔✐➂❦◆❧ ❣➇➍✇➎➏❾➀❿→➒✄❹✡✐➙↕ ⑩ ➍✇❿★➒❲❦ ➉ ➃ ➛

Combinatorics!

45

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SLIDE 46

Elliptic cases

➜ ➝ ➞✡➟ ➠ ➡ ➞➢➠ ➤ ➥ ➝ ➞✎➦ ➟ ➠ ➞➙➟ ➤ ➧ ➝ ➞✎➦ ➟ ➟ ➞✎➦ ➨

Corollary 9. The three urn models

➩ ➫✁➭ ➫➲➯
  • f

balance

➳ have solutions expressible in terms of

elliptic functions. The corresponding lattices are the equilateral triangular lattice (cases

➩ ➫➲➯ ) and

the square lattice tilted by

➵➺➸➼➻ (case ➭ ).

Like for

➽r➾✱➚✳➪ : TILINGS. ➶ ➹ ➘ ➳ ➴ ➴ ➘ ➳ ➷

Corollary 10. The urn model

admits an elliptic function solution of the lemniscatic type.

46

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SLIDE 47

Urns without replacement = the original models!

  • lya–Eggenberger’s contagion urn.
➮ ➱ ➱ ➮ ✃ ❐ ❒❚❮Ï❰❱Ð❆Ñ❈Ò Ð❊Ó✱Ô ❒ÖÕ⑨× ➮ ❮ØÑ❄Ù Ô▲Ú✁Ó ❒ÖÕ❵× ➮ Ð Ó ❮ÛÑ Ó✱ÔÜÚ✁Ó ❰

With

➮ Ò Õ and ➮❞Ý Ò Þ Ý Ò Õ , the PGF of at time ß

is

Ð ß à Õ ❒ÖÕ à Ð à á✬á✬á❸à Ð✑ârÑs❰
  • Cf. also M. Durand. In general:
ã❈❒ White â Ò ➮ Ý à➣ä ➮ Ñ★Ò å ❮ â ÐÏæ✱çè❒ÖÕ❵× ❮ÛÑ➲é Ù Ô ÚÜÓ ❒❽Õ⑨× Ð❊❮ØÑ✪é Ó Ô ÚÜÓ å ❮ â çè❒ÖÕ❵× ❮ÛÑ éëê Ô Ú✁Ó ✃

47

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SLIDE 48

The altruistic model.

ì í î ï ï î ð

Friedman 1947: “Every time an accident occurs, the safety campaign is pushed harder. Whenever no accident occurs, the safety capaign slackens and the probability of an accident increases.”

ñ ò❚óÏô❱õ❆ö í õ✑÷✱ø✬ù➔÷✱ø✁ú⑥û❘ü✁ý✑þ❲ÿ✁ ò✄✂✆☎ õ ÷ ö✞✝ ø✠✟ ÷ ò✡✂☛☎ õ ù ÷ ú⑥û❘ü▲ý❊þ ÿ
  • ö
✝ ø☞✟ ÷ ô

Smythe

ï í ✂ : stemma construction in philology as

well as with recursive trees. Eulerian numbers and leaves in “recursive trees”.

48

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SLIDE 49

The KMR urn: Kotz–Mahmoud–Robert!

✌ ✍ ✎ ✏ ✎ ✌ ✑

Bagchi and Pal [1985]: “present some curious technical problems”. Bivariate algebraic solution, genus

✏ : ✒✔✓✖✕ ✗✙✘ ✗✙✘ ✒✛✚ ✜ ✗✙✘ ✜✣✢✥✤ ✗✧✦★✒ ✚☞✩✫✪✡✬ ✦ ✚✮✭✠✯✰✚☞✩✱✪✳✲ ✯✰✚ ✕✁✴✵✓✖✕ ✲✶✭✡✚✸✷ ✗✹✘ ✜✺✢✥✤ ✗✧✦★✒ ✚☞✩✱✪ ✬✼✻ ✴✵✓✖✕

Mean and variance at time

(

✌ ✾ ✿ ): ❀ ✽ ✍ ✎☛❁ ✎ ❂❄❃❆❅✫❇✮❈❊❉ ❃ ❋
✽ ❁ ❍ ■ ❏▲❑ ✿◆▼ ❀P❖ ✽ ❇✮❈❊❉ ✍ ✎◗✍ ❘ ❑ ✽ ❅❚❙✡❈❯❉ ❖❲❱ ■ ✿ ❳ ■ ❁ ✿ ❍ ❏▲❑ ✿◆▼ ❀P❖❩❨ ✽ ❇❬❈ ❨ ❁ ✿ ❍ ■ ❏▲❑ ✿❭▼ ❀P❖ ✽ ❇✮❈❊❉ ✍ ❘ ❑ ✽ ❖✁❱

Distribution: prototype is

❪ ❫ ❑❵❴ ✑❯❛ ❖ ✾ ❜❝✎☛❁ ❛ ❑ ✎☛❁ ❑ ✎❞❁ ❴ ❖✄❡ ❈❣❢ ❡✐❤ ❙✞❥ ❖✄❦ ❅❚❙✄❈ ❡

Singular exponent is discontinuous at

❛ ✾ ✎ .

49

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SLIDE 50

Banderier, F ., Schaeffer, Soria: within analytic combinatorics such changes are associated to stable laws. (Modify singularity analysis techniques.) — e.g., cores of random maps.

Corollary 11. Model with matrix (

❧✥♠ ♥♣♦✞q❝♦❬♥♣♦✄❧ ) and rts✸✉ ♥♣♦✡❧ s✸✉ q : ✈ ✇ ① ②④③✮⑤⑦⑥✰③☞⑧✫⑨❄⑩ ✉ ❶ ❷ ♥ ②✱③✮⑤⑦⑥✰③☞⑧✱⑨✳⑩✛❸❺❹ ♥✧❻ ❹ ❧▲♠ ♥✧❼❽❼ ❸❺❹ ♥✧❻❾❧❿❼ ❶➀⑨t⑤✄③✧➁➂⑨✠➃ ❶➅➄ ❧ ❧▲♠ ♥ ♦ ➃ ❹ ❶➅➄❩➆ ❼ ✉ ➇ ♥ ➈ ➉☞➊ ⑨ ❹ ➇✹❶ ❼ ➉ ➋❭➌ ❸❺❹ ♥❚♠ ➆➎➍ ❼➐➏✞➑➓➒ ❹ ➍ ➈ ➆ ❼❊♦

the quantity

❶ ➁➂⑨ ➃ ❹ ❶ ➁→➔ ➄❩➆ ❼ is exactly the density of a

stable law of index

when

q ➣ ➆ ➣ ♥ .

Supplements martingale arguments of Gouet [1993] = nonconstructive.

50

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SLIDE 51

Conclusions

A unified analytic framework All

↔ ↕ ↔ urns with constant balance admit of

analytic model. Some interesting special function solutions: algebraic, elliptic, etc. Some new probability laws. Work still in progress!

51