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Page 1: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Continued fractions, Chen-Stein method and

extreme value theory

Parthanil Roy, Indian Statistical Institute

Joint work with Anish Ghosh and Maxim Kirsebom

April 25, 2019

Parthanil Roy CF and EVT April 25, 2019 1 / 30

Page 2: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24

=1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 3: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7

=1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 4: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 5: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 6: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 7: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 8: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 9: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Regular continued fractions

7

24=

1

24/7=

1

3 + 3

7

=1

3 + 1

7/3

=1

3 + 1

2+ 13

:= [3, 2, 3]

Note that 7 > 3 > 1.

Therefore by Euclidean Algorithm, any rational number

ω = p/q ∈ (0, 1)

(with gcd(p, q) = 1) will have a terminating (regular) continuedfraction expansion.

Parthanil Roy CF and EVT April 25, 2019 2 / 30

Page 10: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Conversely . . .

Whenever A1,A2,A3,A4 ∈ N,

[A1,A2,A3,A4] :=1

A1 + 1

A2+1

A3+1A4

∈ (0, 1)

is a rational number.

More generally, by induction on n,

ω = [A1,A2, . . .An]

(with A1,A2, . . .An ∈ N) is a rational number in (0, 1).

Parthanil Roy CF and EVT April 25, 2019 3 / 30

Page 11: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Conversely . . .

Whenever A1,A2,A3,A4 ∈ N,

[A1,A2,A3,A4] :=1

A1 + 1

A2+1

A3+1A4

∈ (0, 1)

is a rational number.

More generally, by induction on n,

ω = [A1,A2, . . .An]

(with A1,A2, . . .An ∈ N) is a rational number in (0, 1).

Parthanil Roy CF and EVT April 25, 2019 3 / 30

Page 12: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Non-terminating continued fraction expansion

TheoremA number ω ∈ (0, 1) has a unique non-terminating continued fractionexpansion

ω =1

A1 + 1

A2+1

A3+···

=: [A1,A2,A3, . . .]

(with each Ai ∈ N) if and only if ω /∈ Q.

Furthermore in this case,the nth truncate [A1,A2, . . .An]→ ω as n→∞.

Canonical rational approximation: ω ≈ [A1,A2, . . .An].

Examples: π ≈ 22

7and π ≈ 355

113.

Parthanil Roy CF and EVT April 25, 2019 4 / 30

Page 13: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Non-terminating continued fraction expansion

TheoremA number ω ∈ (0, 1) has a unique non-terminating continued fractionexpansion

ω =1

A1 + 1

A2+1

A3+···

=: [A1,A2,A3, . . .]

(with each Ai ∈ N) if and only if ω /∈ Q. Furthermore in this case,the nth truncate [A1,A2, . . .An]→ ω as n→∞.

Canonical rational approximation: ω ≈ [A1,A2, . . .An].

Examples: π ≈ 22

7and π ≈ 355

113.

Parthanil Roy CF and EVT April 25, 2019 4 / 30

Page 14: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Non-terminating continued fraction expansion

TheoremA number ω ∈ (0, 1) has a unique non-terminating continued fractionexpansion

ω =1

A1 + 1

A2+1

A3+···

=: [A1,A2,A3, . . .]

(with each Ai ∈ N) if and only if ω /∈ Q. Furthermore in this case,the nth truncate [A1,A2, . . .An]→ ω as n→∞.

Canonical rational approximation: ω ≈ [A1,A2, . . .An].

Examples: π ≈ 22

7and π ≈ 355

113.

Parthanil Roy CF and EVT April 25, 2019 4 / 30

Page 15: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Non-terminating continued fraction expansion

TheoremA number ω ∈ (0, 1) has a unique non-terminating continued fractionexpansion

ω =1

A1 + 1

A2+1

A3+···

=: [A1,A2,A3, . . .]

(with each Ai ∈ N) if and only if ω /∈ Q. Furthermore in this case,the nth truncate [A1,A2, . . .An]→ ω as n→∞.

Canonical rational approximation: ω ≈ [A1,A2, . . .An].

Examples: π ≈ 22

7

and π ≈ 355

113.

Parthanil Roy CF and EVT April 25, 2019 4 / 30

Page 16: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Non-terminating continued fraction expansion

TheoremA number ω ∈ (0, 1) has a unique non-terminating continued fractionexpansion

ω =1

A1 + 1

A2+1

A3+···

=: [A1,A2,A3, . . .]

(with each Ai ∈ N) if and only if ω /∈ Q. Furthermore in this case,the nth truncate [A1,A2, . . .An]→ ω as n→∞.

Canonical rational approximation: ω ≈ [A1,A2, . . .An].

Examples: π ≈ 22

7and π ≈ 355

113.

Parthanil Roy CF and EVT April 25, 2019 4 / 30

Page 17: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why continued fractions?

Continued fractions are important in algebra, analysis, combinatorics,ergodic theory, geometry, number theory, probability, etc..

See, for example, Khintchine (1964).

Parthanil Roy CF and EVT April 25, 2019 5 / 30

Page 18: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

For an irrational ω ∈ (0, 1)

ω =1

1/ω=

1

[1/ω] + 1/ω=:

1

A1(ω) + T (ω)

=1

A1(ω) + 1

A1(T (ω))+T 2(ω)

=:1

A1(ω) + 1

A2(ω)+T 2(ω)

= · · ·

Parthanil Roy CF and EVT April 25, 2019 6 / 30

Page 19: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

The Gauss map

Take Ω = (0, 1), A = B(0,1).

Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω]

for irrational ω ∈ Ω (and any way you like for rational ω ∈ Ω).

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω. Then for almost allω ∈ Ω (namely, for all ω ∈ Ω \Q),

ω = [A1(ω),A2(ω),A3(ω), . . .].

Quick Observation: T , A1 measurable ⇒ each An measurable.

Parthanil Roy CF and EVT April 25, 2019 7 / 30

Page 20: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

The Gauss map

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω]

for irrational ω ∈ Ω

(and any way you like for rational ω ∈ Ω).

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω. Then for almost allω ∈ Ω (namely, for all ω ∈ Ω \Q),

ω = [A1(ω),A2(ω),A3(ω), . . .].

Quick Observation: T , A1 measurable ⇒ each An measurable.

Parthanil Roy CF and EVT April 25, 2019 7 / 30

Page 21: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

The Gauss map

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω]

for irrational ω ∈ Ω (and any way you like for rational ω ∈ Ω).

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω. Then for almost allω ∈ Ω (namely, for all ω ∈ Ω \Q),

ω = [A1(ω),A2(ω),A3(ω), . . .].

Quick Observation: T , A1 measurable ⇒ each An measurable.

Parthanil Roy CF and EVT April 25, 2019 7 / 30

Page 22: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

The Gauss map

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω]

for irrational ω ∈ Ω (and any way you like for rational ω ∈ Ω).

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

Then for almost allω ∈ Ω (namely, for all ω ∈ Ω \Q),

ω = [A1(ω),A2(ω),A3(ω), . . .].

Quick Observation: T , A1 measurable ⇒ each An measurable.

Parthanil Roy CF and EVT April 25, 2019 7 / 30

Page 23: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

The Gauss map

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω]

for irrational ω ∈ Ω (and any way you like for rational ω ∈ Ω).

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω. Then for almost allω ∈ Ω (namely, for all ω ∈ Ω \Q),

ω = [A1(ω),A2(ω),A3(ω), . . .].

Quick Observation: T , A1 measurable ⇒ each An measurable.

Parthanil Roy CF and EVT April 25, 2019 7 / 30

Page 24: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

The Gauss map

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω]

for irrational ω ∈ Ω (and any way you like for rational ω ∈ Ω).

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω. Then for almost allω ∈ Ω (namely, for all ω ∈ Ω \Q),

ω = [A1(ω),A2(ω),A3(ω), . . .].

Quick Observation: T , A1 measurable ⇒ each An measurable.

Parthanil Roy CF and EVT April 25, 2019 7 / 30

Page 25: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Gauss dynamical system

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω].

Bad News: T does not preserve the Lebesgue measure on (0, 1).

Dene a probability measure P (Gauss measure) on (Ω,A) by

P(A) =

∫A

1

(1 + x) log 2dx .

Theorem (Gauss)

T preserves P , i.e., for all A ∈ A, P(A) = P(T−1(A)).

(Ω,A,P ,T ) = the Gauss dynamical system.

Parthanil Roy CF and EVT April 25, 2019 8 / 30

Page 26: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Gauss dynamical system

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω].

Bad News: T does not preserve the Lebesgue measure on (0, 1).

Dene a probability measure P (Gauss measure) on (Ω,A) by

P(A) =

∫A

1

(1 + x) log 2dx .

Theorem (Gauss)

T preserves P , i.e., for all A ∈ A, P(A) = P(T−1(A)).

(Ω,A,P ,T ) = the Gauss dynamical system.

Parthanil Roy CF and EVT April 25, 2019 8 / 30

Page 27: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Gauss dynamical system

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω].

Bad News: T does not preserve the Lebesgue measure on (0, 1).

Dene a probability measure P (Gauss measure) on (Ω,A) by

P(A) =

∫A

1

(1 + x) log 2dx .

Theorem (Gauss)

T preserves P , i.e., for all A ∈ A, P(A) = P(T−1(A)).

(Ω,A,P ,T ) = the Gauss dynamical system.

Parthanil Roy CF and EVT April 25, 2019 8 / 30

Page 28: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Gauss dynamical system

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω].

Bad News: T does not preserve the Lebesgue measure on (0, 1).

Dene a probability measure P (Gauss measure) on (Ω,A) by

P(A) =

∫A

1

(1 + x) log 2dx .

Theorem (Gauss)

T preserves P ,

i.e., for all A ∈ A, P(A) = P(T−1(A)).

(Ω,A,P ,T ) = the Gauss dynamical system.

Parthanil Roy CF and EVT April 25, 2019 8 / 30

Page 29: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Gauss dynamical system

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω].

Bad News: T does not preserve the Lebesgue measure on (0, 1).

Dene a probability measure P (Gauss measure) on (Ω,A) by

P(A) =

∫A

1

(1 + x) log 2dx .

Theorem (Gauss)

T preserves P , i.e., for all A ∈ A, P(A) = P(T−1(A)).

(Ω,A,P ,T ) = the Gauss dynamical system.

Parthanil Roy CF and EVT April 25, 2019 8 / 30

Page 30: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Gauss dynamical system

Take Ω = (0, 1), A = B(0,1). Dene T : Ω→ Ω and A1 : Ω→ N by

T (ω) = 1/ω (Gauss map) and A1(ω) = [1/ω].

Bad News: T does not preserve the Lebesgue measure on (0, 1).

Dene a probability measure P (Gauss measure) on (Ω,A) by

P(A) =

∫A

1

(1 + x) log 2dx .

Theorem (Gauss)

T preserves P , i.e., for all A ∈ A, P(A) = P(T−1(A)).

(Ω,A,P ,T ) = the Gauss dynamical system.Parthanil Roy CF and EVT April 25, 2019 8 / 30

Page 31: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

A reformulation of Gauss's theorem

Exercise (in Probability Theory II): Suppose X is a randomvariable having probability density function

fX (x) =1

(1 + x) log 2, x ∈ (0, 1).

Then show that 1/X L= X .

Parthanil Roy CF and EVT April 25, 2019 9 / 30

Page 32: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx .

DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process. In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

Page 33: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx . DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process. In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

Page 34: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx . DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process. In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

Page 35: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx . DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process. In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

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A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx . DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process. In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

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A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx . DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process.

In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

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A stationary process

Take Ω = (0, 1), A = B(0,1), P(dx) = ((1 + x) log 2)−1 dx . DeneT : Ω→ Ω by T (ω) = 1/ω and A1 : Ω→ N by A1(ω) = [1/ω].

For all j ∈ N, set Aj+1(ω) := A1(T j(ω)), ω ∈ Ω.

This denes a sequence An : Ω→ Nn≥1 of positive integer-valuedrandom variables on the probability space (Ω,A,P).

An = nth digit in the regular continued fraction expansion of arandom number ω ∈ (0, 1) chosen according to the law P .

T preserves P ⇒ An is a strictly stationary process. In particular,A1,A2,A3, . . . are identically distributed.

Parthanil Roy CF and EVT April 25, 2019 10 / 30

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Two easy observations

Direct Computation: For all m ∈ N,

P(A1 ≥ m) =1

log 2log

(1 +

1

m

)

∼ 1

m log 2(as m→∞).

For all u > 0,

P

(A1 log 2

n> u

)= P

(A1 ≥

⌈un

log 2

⌉)∼ 1

un

as n→∞. In particular,

nP

(A1 log 2

n> u

)→ u−1

(A1 is regularly varying with index 1).

Parthanil Roy CF and EVT April 25, 2019 11 / 30

Page 40: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Two easy observations

Direct Computation: For all m ∈ N,

P(A1 ≥ m) =1

log 2log

(1 +

1

m

)∼ 1

m log 2(as m→∞).

For all u > 0,

P

(A1 log 2

n> u

)= P

(A1 ≥

⌈un

log 2

⌉)∼ 1

un

as n→∞. In particular,

nP

(A1 log 2

n> u

)→ u−1

(A1 is regularly varying with index 1).

Parthanil Roy CF and EVT April 25, 2019 11 / 30

Page 41: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Two easy observations

Direct Computation: For all m ∈ N,

P(A1 ≥ m) =1

log 2log

(1 +

1

m

)∼ 1

m log 2(as m→∞).

For all u > 0,

P

(A1 log 2

n> u

)= P

(A1 ≥

⌈un

log 2

⌉)∼ 1

un

as n→∞.

In particular,

nP

(A1 log 2

n> u

)→ u−1

(A1 is regularly varying with index 1).

Parthanil Roy CF and EVT April 25, 2019 11 / 30

Page 42: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Two easy observations

Direct Computation: For all m ∈ N,

P(A1 ≥ m) =1

log 2log

(1 +

1

m

)∼ 1

m log 2(as m→∞).

For all u > 0,

P

(A1 log 2

n> u

)= P

(A1 ≥

⌈un

log 2

⌉)∼ 1

un

as n→∞. In particular,

nP

(A1 log 2

n> u

)→ u−1

(A1 is regularly varying with index 1).

Parthanil Roy CF and EVT April 25, 2019 11 / 30

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If A1,A2,A3, . . . were independent

then

1(A1 log 2>un), 1(A2 log 2>un), 1(A3 log 2>un), . . .iid∼ Ber(pn),

where pn = P(A1 log 2 > un)

∼ 1

un.

Therefore for all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un =n∑

j=1

1(Aj log 2>un)∼ Bin(n, pn)

L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 12 / 30

Page 44: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

If A1,A2,A3, . . . were independent

then

1(A1 log 2>un), 1(A2 log 2>un), 1(A3 log 2>un), . . .iid∼ Ber(pn),

where pn = P(A1 log 2 > un)∼ 1

un.

Therefore for all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un =n∑

j=1

1(Aj log 2>un)∼ Bin(n, pn)

L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 12 / 30

Page 45: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

If A1,A2,A3, . . . were independent

then

1(A1 log 2>un), 1(A2 log 2>un), 1(A3 log 2>un), . . .iid∼ Ber(pn),

where pn = P(A1 log 2 > un)∼ 1

un.

Therefore for all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un

=n∑

j=1

1(Aj log 2>un)∼ Bin(n, pn)

L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 12 / 30

Page 46: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

If A1,A2,A3, . . . were independent

then

1(A1 log 2>un), 1(A2 log 2>un), 1(A3 log 2>un), . . .iid∼ Ber(pn),

where pn = P(A1 log 2 > un)∼ 1

un.

Therefore for all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un =n∑

j=1

1(Aj log 2>un)

∼ Bin(n, pn)

L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 12 / 30

Page 47: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

If A1,A2,A3, . . . were independent

then

1(A1 log 2>un), 1(A2 log 2>un), 1(A3 log 2>un), . . .iid∼ Ber(pn),

where pn = P(A1 log 2 > un)∼ 1

un.

Therefore for all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un =n∑

j=1

1(Aj log 2>un)∼ Bin(n, pn)

L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 12 / 30

Page 48: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

If A1,A2,A3, . . . were independent

then

1(A1 log 2>un), 1(A2 log 2>un), 1(A3 log 2>un), . . .iid∼ Ber(pn),

where pn = P(A1 log 2 > un)∼ 1

un.

Therefore for all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un =n∑

j=1

1(Aj log 2>un)∼ Bin(n, pn)

L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 12 / 30

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Doeblin-Iosifescu asymptotics

Theorem (Doeblin (1940), Iosifescu (1977))

For all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Corollary (Main result of Galambos (1972))

Let M(1)n := maxAi log 2 : 1 ≤ 1 ≤ n, n ∈ N. Then for all u > 0,

P

(M

(1)n

n≤ u

)→ e−u

−1

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 13 / 30

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Doeblin-Iosifescu asymptotics

Theorem (Doeblin (1940), Iosifescu (1977))

For all u > 0,

Eun := #1 ≤ j ≤ n : Aj log 2 > un L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

Corollary (Main result of Galambos (1972))

Let M(1)n := maxAi log 2 : 1 ≤ 1 ≤ n, n ∈ N. Then for all u > 0,

P

(M

(1)n

n≤ u

)→ e−u

−1

as n→∞.

Parthanil Roy CF and EVT April 25, 2019 13 / 30

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The main question

Theorem (Doeblin (1940), Iosifescu (1977))

For all u > 0,

(DI ) Eun := #1 ≤ j ≤ n : Aj log 2 > un L−→ Eu∞ ∼ Poi(u−1)

as n→∞.

QuestionWhat is the rate of convergence in (DI )?

Parthanil Roy CF and EVT April 25, 2019 14 / 30

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Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 53: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972))

- signicantly improves a resultof Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 54: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 55: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N

(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 56: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 57: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process.

(Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 58: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

Page 59: Continued fractions, Chen-Stein method and extreme value ...math.iisc.ac.in/seminar-slides/2019/2019-03-01-ParthanilRoy.pdfContinued fractions, Chen-Stein method and extreme value

Why do we care?

Can estimate the rate of convergence of scaled maxima sequenceM

(1)n /n (as in Galambos (1972)) - signicantly improves a result

of Philipp (1976).

Rate of convergence for the scaled k th maxima for any k ∈ N(uniform over k).

A tiny detour of our proof recovers a result ofTyran-Kami«ska (2010) on the weak convergence of thecorresponding extremal point process. (Inspired by Chiarini,Cipriani and Hazra (2015).)

Rate of convergence of the scaled maxima for the geodesic owon the modular surface.

Parthanil Roy CF and EVT April 25, 2019 15 / 30

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The geodesic ow on the modular surface

The group SL2(Z) :=

(a bc d

): a, b, c , d ∈ Z, ad − bc = 1

acts isometrically on H := z ∈ C : Im(z) > 0 by rationaltransformations: (

a bc d

).z =

az + b

cz + d.

Series (1981, 1985): Connected the geodesic ow on M = H/SL2(Z)with Gauss dynamical system using a symbolic dynamics.

Pollicott (2009): Used this connection to nd the weak limit of thenormalized maxima of the geodesic ow on M .

Our work yields the rate of convergence in Pollicott's result.

Parthanil Roy CF and EVT April 25, 2019 16 / 30

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The geodesic ow on the modular surface

The group SL2(Z) :=

(a bc d

): a, b, c , d ∈ Z, ad − bc = 1

acts isometrically on H := z ∈ C : Im(z) > 0 by rationaltransformations: (

a bc d

).z =

az + b

cz + d.

Series (1981, 1985): Connected the geodesic ow on M = H/SL2(Z)with Gauss dynamical system using a symbolic dynamics.

Pollicott (2009): Used this connection to nd the weak limit of thenormalized maxima of the geodesic ow on M .

Our work yields the rate of convergence in Pollicott's result.

Parthanil Roy CF and EVT April 25, 2019 16 / 30

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The geodesic ow on the modular surface

The group SL2(Z) :=

(a bc d

): a, b, c , d ∈ Z, ad − bc = 1

acts isometrically on H := z ∈ C : Im(z) > 0 by rationaltransformations: (

a bc d

).z =

az + b

cz + d.

Series (1981, 1985): Connected the geodesic ow on M = H/SL2(Z)with Gauss dynamical system using a symbolic dynamics.

Pollicott (2009): Used this connection to nd the weak limit of thenormalized maxima of the geodesic ow on M .

Our work yields the rate of convergence in Pollicott's result.

Parthanil Roy CF and EVT April 25, 2019 16 / 30

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The geodesic ow on the modular surface

The group SL2(Z) :=

(a bc d

): a, b, c , d ∈ Z, ad − bc = 1

acts isometrically on H := z ∈ C : Im(z) > 0 by rationaltransformations: (

a bc d

).z =

az + b

cz + d.

Series (1981, 1985): Connected the geodesic ow on M = H/SL2(Z)with Gauss dynamical system using a symbolic dynamics.

Pollicott (2009): Used this connection to nd the weak limit of thenormalized maxima of the geodesic ow on M .

Our work yields the rate of convergence in Pollicott's result.

Parthanil Roy CF and EVT April 25, 2019 16 / 30

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The main result

Theorem (Ghosh, Kirsebom, R. (2019))

There exists κ > 0 and a sequence 1 `n nε (for all ε > 0) suchthat for all u > 0 and for all n ∈ N,

dTV (Eun , Eu∞) := supA⊆N∪0

∣∣P(Eun ∈ A)−P(Eu∞ ∈ A)∣∣ ≤ κ

min u, u2`nn.

Corollary

Suppose M(k)n := k th maximum of Ai log 2 : 1 ≤ i ≤ n. For all

u > 0 and for all k , n ∈ N,

supk∈N

∣∣∣∣∣P(M

(k)n

n≤ u

)− e−u

−1k−1∑i=0

u−i

i !

∣∣∣∣∣ ≤ κ

min u, u2`nn.

Parthanil Roy CF and EVT April 25, 2019 17 / 30

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The main result

Theorem (Ghosh, Kirsebom, R. (2019))

There exists κ > 0 and a sequence 1 `n nε (for all ε > 0) suchthat for all u > 0 and for all n ∈ N,

dTV (Eun , Eu∞) := supA⊆N∪0

∣∣P(Eun ∈ A)−P(Eu∞ ∈ A)∣∣ ≤ κ

min u, u2`nn.

Corollary

Suppose M(k)n := k th maximum of Ai log 2 : 1 ≤ i ≤ n. For all

u > 0 and for all k , n ∈ N,

supk∈N

∣∣∣∣∣P(M

(k)n

n≤ u

)− e−u

−1k−1∑i=0

u−i

i !

∣∣∣∣∣ ≤ κ

min u, u2`nn.

Parthanil Roy CF and EVT April 25, 2019 17 / 30

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Comparison with existing results

Resnick and de Haan (1989): If A1,A2, . . . were independent,then ∣∣∣P (M (1)

n /n ≤ u)− e−u

−1∣∣∣≤ O(1/n).

Our upper bound = O(`n/n) = o(n−1+ε

)for all ε > 0.

Philipp (1976): For Gauss dynamical system∣∣∣P (M (1)n /n ≤ u

)− e−u

−1∣∣∣ ≤ O(`n/n)O

(exp−(log n)δ

)for all δ ∈ (0, 1).

Parthanil Roy CF and EVT April 25, 2019 18 / 30

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Comparison with existing results

Resnick and de Haan (1989): If A1,A2, . . . were independent,then ∣∣∣P (M (1)

n /n ≤ u)− e−u

−1∣∣∣≤ O(1/n).

Our upper bound = O(`n/n) = o(n−1+ε

)for all ε > 0.

Philipp (1976): For Gauss dynamical system∣∣∣P (M (1)n /n ≤ u

)− e−u

−1∣∣∣ ≤ O(`n/n)O

(exp−(log n)δ

)for all δ ∈ (0, 1).

Parthanil Roy CF and EVT April 25, 2019 18 / 30

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Comparison with existing results

Resnick and de Haan (1989): If A1,A2, . . . were independent,then ∣∣∣P (M (1)

n /n ≤ u)− e−u

−1∣∣∣≤ O(1/n).

Our upper bound = O(`n/n) = o(n−1+ε

)for all ε > 0.

Philipp (1976): For Gauss dynamical system∣∣∣P (M (1)n /n ≤ u

)− e−u

−1∣∣∣ ≤ O(`n/n)O

(exp−(log n)δ

)for all δ ∈ (0, 1).

Parthanil Roy CF and EVT April 25, 2019 18 / 30

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Comparison with existing results

Resnick and de Haan (1989): If A1,A2, . . . were independent,then ∣∣∣P (M (1)

n /n ≤ u)− e−u

−1∣∣∣≤ O(1/n).

Our upper bound = O(`n/n) = o(n−1+ε

)for all ε > 0.

Philipp (1976): For Gauss dynamical system∣∣∣P (M (1)n /n ≤ u

)− e−u

−1∣∣∣ ≤ O(`n/n)O

(exp−(log n)δ

)for all δ ∈ (0, 1).

Parthanil Roy CF and EVT April 25, 2019 19 / 30

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Sketch of proof

Recall Eun =∑n

j=11(Aj log 2>un)

approx∼ Bin(n, pn = P(A1 log 2 > un)

).

Dene an intermediate random variable Eun ∼ Poi(npn).

On the other hand, Eu∞ ∼ Poi(u−1).

• Use triangle inequality

dTV (Eun , Eu∞) ≤ dTV (Eun , Eun ) + dTV (Eun , Eu∞).

• Bound dTV (Eun , Eun ) using Chen-Stein method (Arratia, Goldsteinand Gordon (1989)) + exponential mixing (Philipp (1970)).

• Estimate dTV (Eun , Eu∞) using second order regular variation.

Parthanil Roy CF and EVT April 25, 2019 20 / 30

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Sketch of proof

Recall Eun =∑n

j=11(Aj log 2>un)

approx∼ Bin(n, pn = P(A1 log 2 > un)

).

Dene an intermediate random variable Eun ∼ Poi(npn).

On the other hand, Eu∞ ∼ Poi(u−1).

• Use triangle inequality

dTV (Eun , Eu∞) ≤ dTV (Eun , Eun ) + dTV (Eun , Eu∞).

• Bound dTV (Eun , Eun ) using Chen-Stein method (Arratia, Goldsteinand Gordon (1989)) + exponential mixing (Philipp (1970)).

• Estimate dTV (Eun , Eu∞) using second order regular variation.

Parthanil Roy CF and EVT April 25, 2019 21 / 30

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Sketch of proof

Recall Eun =∑n

j=11(Aj log 2>un)

approx∼ Bin(n, pn = P(A1 log 2 > un)

).

Dene an intermediate random variable Eun ∼ Poi(npn).

On the other hand, Eu∞ ∼ Poi(u−1).

• Use triangle inequality

dTV (Eun , Eu∞) ≤ dTV (Eun , Eun ) + dTV (Eun , Eu∞).

• Bound dTV (Eun , Eun ) using Chen-Stein method (Arratia, Goldsteinand Gordon (1989)) + exponential mixing (Philipp (1970)).

• Estimate dTV (Eun , Eu∞) using second order regular variation.

Parthanil Roy CF and EVT April 25, 2019 22 / 30

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Sketch of proof

Recall Eun =∑n

j=11(Aj log 2>un)

approx∼ Bin(n, pn = P(A1 log 2 > un)

).

Dene an intermediate random variable Eun ∼ Poi(npn).

On the other hand, Eu∞ ∼ Poi(u−1).

• Use triangle inequality

dTV (Eun , Eu∞) ≤ dTV (Eun , Eun ) + dTV (Eun , Eu∞).

• Bound dTV (Eun , Eun ) using Chen-Stein method (Arratia, Goldsteinand Gordon (1989)) + exponential mixing (Philipp (1970)).

• Estimate dTV (Eun , Eu∞) using second order regular variation.

Parthanil Roy CF and EVT April 25, 2019 23 / 30

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Sketch of proof

Recall Eun =∑n

j=11(Aj log 2>un)

approx∼ Bin(n, pn = P(A1 log 2 > un)

).

Dene an intermediate random variable Eun ∼ Poi(npn).

On the other hand, Eu∞ ∼ Poi(u−1).

• Use triangle inequality

dTV (Eun , Eu∞) ≤ dTV (Eun , Eun ) + dTV (Eun , Eu∞).

• Bound dTV (Eun , Eun ) using Chen-Stein method (Arratia, Goldsteinand Gordon (1989)) + exponential mixing (Philipp (1970)).

• Estimate dTV (Eun , Eu∞) using second order regular variation.

Parthanil Roy CF and EVT April 25, 2019 24 / 30

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How to estimate dTV (Eun , Eu∞)?

Recall Eun ∼ Poi(npn) and Eu∞ ∼ Poi(u−1).

Lemma (8) of Freedman (1974):

dTV (Eun , Eu∞) ≤∣∣npn − u−1

∣∣ (soft bound)

=∣∣nP(A1 log 2 > un)− u−1

∣∣≤ 3 log 2

2u21

n(second order regular variation)

`nn.

Parthanil Roy CF and EVT April 25, 2019 25 / 30

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How to estimate dTV (Eun , Eu∞)?

Recall Eun ∼ Poi(npn) and Eu∞ ∼ Poi(u−1).

Lemma (8) of Freedman (1974):

dTV (Eun , Eu∞) ≤∣∣npn − u−1

∣∣ (soft bound)

=∣∣nP(A1 log 2 > un)− u−1

∣∣

≤ 3 log 2

2u21

n(second order regular variation)

`nn.

Parthanil Roy CF and EVT April 25, 2019 25 / 30

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How to estimate dTV (Eun , Eu∞)?

Recall Eun ∼ Poi(npn) and Eu∞ ∼ Poi(u−1).

Lemma (8) of Freedman (1974):

dTV (Eun , Eu∞) ≤∣∣npn − u−1

∣∣ (soft bound)

=∣∣nP(A1 log 2 > un)− u−1

∣∣≤ 3 log 2

2u21

n(second order regular variation)

`nn.

Parthanil Roy CF and EVT April 25, 2019 25 / 30

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How to estimate dTV (Eun , Eu∞)?

Recall Eun ∼ Poi(npn) and Eu∞ ∼ Poi(u−1).

Lemma (8) of Freedman (1974):

dTV (Eun , Eu∞) ≤∣∣npn − u−1

∣∣ (soft bound)

=∣∣nP(A1 log 2 > un)− u−1

∣∣≤ 3 log 2

2u21

n(second order regular variation)

`nn.

Parthanil Roy CF and EVT April 25, 2019 25 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n. Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).Note that Eun =

∑i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn). Therefore Eun

L=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n.

Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).Note that Eun =

∑i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn). Therefore Eun

L=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n. Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).

Note that Eun =∑

i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn). Therefore Eun

L=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n. Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).Note that Eun =

∑i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn). Therefore Eun

L=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n. Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).Note that Eun =

∑i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn).

Therefore EunL=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n. Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).Note that Eun =

∑i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn). Therefore Eun

L=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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How to bound dTV (Eun , Eun )?

Recall Eun =∑n

i=11(Ai log 2>un) and Eun ∼ Poi(npn).

I := 1, 2, . . . , n. Xi := 1(Ai log 2>un) ∼ Ber(pn)i∈I (dependent).Note that Eun =

∑i∈I Xi .

Take Y1,Y2, . . . ,Yniid∼ Poi(pn). Therefore Eun

L=∑

i∈I Yi .

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ ??

Parthanil Roy CF and EVT April 25, 2019 26 / 30

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Arratia, Goldstein and Gordon (1989)

Xi ∼ Ber(πi)i∈I (possibly dependent).

Yi ∼ Poi(πi)i∈I (independent).

For each i ∈ I, there exists a subset Bi ⊆ I such that i ∈ Bi andXi is nearly independent of Xj : j ∈ I \ Bi.

b1 :=∑i∈I

∑j∈Bi

πiπj , b2 :=∑i∈I

∑j∈Bi\i

E (XiXj),

b3 :=∑i∈I

E[∣∣E (Xi − πi

∣∣ Xj : j ∈ I \ Bj)∣∣].

dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ 4b1 + 4b2 + 2b3

Parthanil Roy CF and EVT April 25, 2019 27 / 30

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Arratia, Goldstein and Gordon (1989)

Xi ∼ Ber(πi)i∈I (possibly dependent).

Yi ∼ Poi(πi)i∈I (independent).

For each i ∈ I, there exists a subset Bi ⊆ I such that i ∈ Bi andXi is nearly independent of Xj : j ∈ I \ Bi.

b1 :=∑i∈I

∑j∈Bi

πiπj , b2 :=∑i∈I

∑j∈Bi\i

E (XiXj),

b3 :=∑i∈I

E[∣∣E (Xi − πi

∣∣ Xj : j ∈ I \ Bj)∣∣].

dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ 4b1 + 4b2 + 2b3

Parthanil Roy CF and EVT April 25, 2019 27 / 30

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Arratia, Goldstein and Gordon (1989)

Xi ∼ Ber(πi)i∈I (possibly dependent).

Yi ∼ Poi(πi)i∈I (independent).

For each i ∈ I, there exists a subset Bi ⊆ I such that i ∈ Bi andXi is nearly independent of Xj : j ∈ I \ Bi.

b1 :=∑i∈I

∑j∈Bi

πiπj , b2 :=∑i∈I

∑j∈Bi\i

E (XiXj),

b3 :=∑i∈I

E[∣∣E (Xi − πi

∣∣ Xj : j ∈ I \ Bj)∣∣].

dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ 4b1 + 4b2 + 2b3

Parthanil Roy CF and EVT April 25, 2019 27 / 30

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Arratia, Goldstein and Gordon (1989)

Xi ∼ Ber(πi)i∈I (possibly dependent).

Yi ∼ Poi(πi)i∈I (independent).

For each i ∈ I, there exists a subset Bi ⊆ I such that i ∈ Bi andXi is nearly independent of Xj : j ∈ I \ Bi.

b1 :=∑i∈I

∑j∈Bi

πiπj , b2 :=∑i∈I

∑j∈Bi\i

E (XiXj),

b3 :=∑i∈I

E[∣∣E (Xi − πi

∣∣ Xj : j ∈ I \ Bj)∣∣].

dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ 4b1 + 4b2 + 2b3

Parthanil Roy CF and EVT April 25, 2019 27 / 30

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Arratia, Goldstein and Gordon (1989)

Xi ∼ Ber(πi)i∈I (possibly dependent).

Yi ∼ Poi(πi)i∈I (independent).

For each i ∈ I, there exists a subset Bi ⊆ I such that i ∈ Bi andXi is nearly independent of Xj : j ∈ I \ Bi.

b1 :=∑i∈I

∑j∈Bi

πiπj , b2 :=∑i∈I

∑j∈Bi\i

E (XiXj),

b3 :=∑i∈I

E[∣∣E (Xi − πi

∣∣ Xj : j ∈ I \ Bj)∣∣].

dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ 4b1 + 4b2 + 2b3

Parthanil Roy CF and EVT April 25, 2019 27 / 30

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Arratia, Goldstein and Gordon (1989)

Xi ∼ Ber(πi)i∈I (possibly dependent).

Yi ∼ Poi(πi)i∈I (independent).

For each i ∈ I, there exists a subset Bi ⊆ I such that i ∈ Bi andXi is nearly independent of Xj : j ∈ I \ Bi.

b1 :=∑i∈I

∑j∈Bi

πiπj , b2 :=∑i∈I

∑j∈Bi\i

E (XiXj),

b3 :=∑i∈I

E[∣∣E (Xi − πi

∣∣ Xj : j ∈ I \ Bj)∣∣].

dTV (Eun , Eun ) = dTV

(∑i∈I

Xi ,∑i∈I

Yi

)≤ 4b1 + 4b2 + 2b3

Parthanil Roy CF and EVT April 25, 2019 28 / 30

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How to bound b1, b2, b3?

After carefully choosing the Bi 's . . .

b1 can be bounded easily, and

the bounds on b2 and b3 need the following exponential mixingproperty of Ai 's:

Theorem (Philipp (1970))

There exists C > 0 and θ > 1 such that for all m, n ∈ N, for allF ∈ σ(A1,A2, . . . ,Am), and for all H ∈ σ(Am+n,Am+n+1, . . .),

|P(F ∩ H)− P(F )P(H)| ≤ Cθ−n P(F )P(H).

Parthanil Roy CF and EVT April 25, 2019 29 / 30

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How to bound b1, b2, b3?

After carefully choosing the Bi 's . . .

b1 can be bounded easily, and

the bounds on b2 and b3 need the following exponential mixingproperty of Ai 's:

Theorem (Philipp (1970))

There exists C > 0 and θ > 1 such that for all m, n ∈ N, for allF ∈ σ(A1,A2, . . . ,Am), and for all H ∈ σ(Am+n,Am+n+1, . . .),

|P(F ∩ H)− P(F )P(H)| ≤ Cθ−n P(F )P(H).

Parthanil Roy CF and EVT April 25, 2019 29 / 30

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How to bound b1, b2, b3?

After carefully choosing the Bi 's . . .

b1 can be bounded easily, and

the bounds on b2 and b3 need the following exponential mixingproperty of Ai 's:

Theorem (Philipp (1970))

There exists C > 0 and θ > 1 such that for all m, n ∈ N, for allF ∈ σ(A1,A2, . . . ,Am), and for all H ∈ σ(Am+n,Am+n+1, . . .),

|P(F ∩ H)− P(F )P(H)| ≤ Cθ−n P(F )P(H).

Parthanil Roy CF and EVT April 25, 2019 29 / 30

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How to bound b1, b2, b3?

After carefully choosing the Bi 's . . .

b1 can be bounded easily, and

the bounds on b2 and b3 need the following exponential mixingproperty of Ai 's:

Theorem (Philipp (1970))

There exists C > 0 and θ > 1 such that for all m, n ∈ N, for allF ∈ σ(A1,A2, . . . ,Am), and for all H ∈ σ(Am+n,Am+n+1, . . .),

|P(F ∩ H)− P(F )P(H)| ≤ Cθ−n P(F )P(H).

Parthanil Roy CF and EVT April 25, 2019 29 / 30

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Thank You Very Much

Parthanil Roy CF and EVT April 25, 2019 30 / 30