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Bounds on strong unicity for Chebyshev approximation with bounded - - PowerPoint PPT Presentation

Bounds on strong unicity for Chebyshev approximation with bounded coefficients Andrei Sipos , Technische Universit at Darmstadt Institute of Mathematics of the Romanian Academy August 15, 2019 Logic Colloquium 2019 Praha, Cesko Proof


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Bounds on strong unicity for Chebyshev approximation with bounded coefficients

Andrei Sipos

,

Technische Universit¨ at Darmstadt Institute of Mathematics of the Romanian Academy

August 15, 2019 Logic Colloquium 2019 Praha, ˇ Cesko

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SLIDE 2

Proof mining

Proof mining: an applied subfield of mathematical logic

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Proof mining

Proof mining: an applied subfield of mathematical logic goals: to find explicit and uniform witnesses or bounds and to remove superfluous premises from concrete mathematical statements by analyzing their proofs

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Proof mining

Proof mining: an applied subfield of mathematical logic goals: to find explicit and uniform witnesses or bounds and to remove superfluous premises from concrete mathematical statements by analyzing their proofs tools used: primarily proof interpretations (modified realizability, negative translation, functional interpretation)

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SLIDE 5

A brief history

Early efforts

David Hilbert: “¨ Uber das Unendliche” (1926) Grete Hermann: “The Question of Finitely Many Steps in Polynomial Ideal Theory” (1926)

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A brief history

Early efforts

David Hilbert: “¨ Uber das Unendliche” (1926) Grete Hermann: “The Question of Finitely Many Steps in Polynomial Ideal Theory” (1926)

Georg Kreisel’s program of “unwinding of proofs”

the shift of emphasis in the early 1950s Kreisel: Littlewood’s theorem, Hilbert’s 17th problem (1957) the publication of G¨

  • del’s Dialectica interpretation (1958)

Jean-Yves Girard: bounds on van der Waerden numbers by strategic cut elimination (1987) Horst Luckhardt: growth conditions on Herbrand terms and the number of solutions in Roth’s theorem (1989)

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SLIDE 7

A brief history

Early efforts

David Hilbert: “¨ Uber das Unendliche” (1926) Grete Hermann: “The Question of Finitely Many Steps in Polynomial Ideal Theory” (1926)

Georg Kreisel’s program of “unwinding of proofs”

the shift of emphasis in the early 1950s Kreisel: Littlewood’s theorem, Hilbert’s 17th problem (1957) the publication of G¨

  • del’s Dialectica interpretation (1958)

Jean-Yves Girard: bounds on van der Waerden numbers by strategic cut elimination (1987) Horst Luckhardt: growth conditions on Herbrand terms and the number of solutions in Roth’s theorem (1989)

Ulrich Kohlenbach: contemporary proof mining

uniqueness in approximation theory (since 1990) nonlinear analysis, convex optimization et al. (since 2001) ergodic theory, commutative algebra, differential algebra: work by Avigad, Towsner, Simmons (since 2007)

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SLIDE 8

A brief history

Early efforts

David Hilbert: “¨ Uber das Unendliche” (1926) Grete Hermann: “The Question of Finitely Many Steps in Polynomial Ideal Theory” (1926)

Georg Kreisel’s program of “unwinding of proofs”

the shift of emphasis in the early 1950s Kreisel: Littlewood’s theorem, Hilbert’s 17th problem (1957) the publication of G¨

  • del’s Dialectica interpretation (1958)

Jean-Yves Girard: bounds on van der Waerden numbers by strategic cut elimination (1987) Horst Luckhardt: growth conditions on Herbrand terms and the number of solutions in Roth’s theorem (1989)

Ulrich Kohlenbach: contemporary proof mining

uniqueness in approximation theory (since 1990) nonlinear analysis, convex optimization et al. (since 2001) ergodic theory, commutative algebra, differential algebra: work by Avigad, Towsner, Simmons (since 2007)

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Chebyshev approximation

We have the following classical Chebyshev approximation result. Theorem (de la Vall´ ee Poussin, Young – 1900s) For every n ∈ N and every continuous f : [0, 1] → R there is an unique p ∈ Pn (the set of real polynomials of degree at most n) such that f − p = min

q∈Pn f − q

(where · denotes the supremum norm).

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Chebyshev approximation

We have the following classical Chebyshev approximation result. Theorem (de la Vall´ ee Poussin, Young – 1900s) For every n ∈ N and every continuous f : [0, 1] → R there is an unique p ∈ Pn (the set of real polynomials of degree at most n) such that f − p = min

q∈Pn f − q

(where · denotes the supremum norm). Kohlenbach extracted in 1990 a modulus of uniqueness – a function Ψ with the property that if p1 and p2 are such that f − p1, f − p2 ≤ min +Ψ(δ), then p1 − p2 ≤ δ.

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Chebyshev approximation

We have the following classical Chebyshev approximation result. Theorem (de la Vall´ ee Poussin, Young – 1900s) For every n ∈ N and every continuous f : [0, 1] → R there is an unique p ∈ Pn (the set of real polynomials of degree at most n) such that f − p = min

q∈Pn f − q

(where · denotes the supremum norm). Kohlenbach extracted in 1990 a modulus of uniqueness – a function Ψ with the property that if p1 and p2 are such that f − p1, f − p2 ≤ min +Ψ(δ), then p1 − p2 ≤ δ. He did this by analyzing the uniqueness proof and obtaining an approximate version of it. Let us see how the original proof flows.

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A sketch of de la Vall´ ee Poussin’s proof

Take p1 and p2 that attain the minimum distance E. Then also

p1+p2 2

attains the minimum and we denote it by p.

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A sketch of de la Vall´ ee Poussin’s proof

Take p1 and p2 that attain the minimum distance E. Then also

p1+p2 2

attains the minimum and we denote it by p. By a result called the alternation theorem, we have that there is a j ∈ {0, 1} and x1 < . . . < xn+1 in [0, 1] such that for every i ∈ {1, . . . , n + 1}, (p − f )(xi) = (−1)i+jE.

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SLIDE 14

A sketch of de la Vall´ ee Poussin’s proof

Take p1 and p2 that attain the minimum distance E. Then also

p1+p2 2

attains the minimum and we denote it by p. By a result called the alternation theorem, we have that there is a j ∈ {0, 1} and x1 < . . . < xn+1 in [0, 1] such that for every i ∈ {1, . . . , n + 1}, (p − f )(xi) = (−1)i+jE. Let i ∈ {1, . . . , n + 1} and assume wlog that i + j is even. Then (p − f )(xi) = E, so p1(xi) − f (xi) 2 + p2(xi) − f (xi) 2 = E.

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A sketch of de la Vall´ ee Poussin’s proof

Take p1 and p2 that attain the minimum distance E. Then also

p1+p2 2

attains the minimum and we denote it by p. By a result called the alternation theorem, we have that there is a j ∈ {0, 1} and x1 < . . . < xn+1 in [0, 1] such that for every i ∈ {1, . . . , n + 1}, (p − f )(xi) = (−1)i+jE. Let i ∈ {1, . . . , n + 1} and assume wlog that i + j is even. Then (p − f )(xi) = E, so p1(xi) − f (xi) 2 + p2(xi) − f (xi) 2 = E. Since p1 − f = E, p1(xi) − f (xi) ≤ E. Similarly, p2(xi) − f (xi) ≤ E. By the above, we have that both are actually equal to E and so p1(xi) = p2(xi).

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SLIDE 16

A sketch of de la Vall´ ee Poussin’s proof

Take p1 and p2 that attain the minimum distance E. Then also

p1+p2 2

attains the minimum and we denote it by p. By a result called the alternation theorem, we have that there is a j ∈ {0, 1} and x1 < . . . < xn+1 in [0, 1] such that for every i ∈ {1, . . . , n + 1}, (p − f )(xi) = (−1)i+jE. Let i ∈ {1, . . . , n + 1} and assume wlog that i + j is even. Then (p − f )(xi) = E, so p1(xi) − f (xi) 2 + p2(xi) − f (xi) 2 = E. Since p1 − f = E, p1(xi) − f (xi) ≤ E. Similarly, p2(xi) − f (xi) ≤ E. By the above, we have that both are actually equal to E and so p1(xi) = p2(xi). Since p1 and p2 coincide on at least n + 1 points, they must be equal.

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SLIDE 17

Approximating the proof

Let us now see how one approximates the proof on the previous

  • slide. First, for trivial reasons, the polynomials can be assumed to

be in the closed ball Z of radius 5

2f (which is compact, as it lies

inside the finite dimensional space Pn).

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SLIDE 18

Approximating the proof

Let us now see how one approximates the proof on the previous

  • slide. First, for trivial reasons, the polynomials can be assumed to

be in the closed ball Z of radius 5

2f (which is compact, as it lies

inside the finite dimensional space Pn).

1 for all p1, p2 ∈ Z and all ε > 0, if f − p1,

f − p2 ≤ E + Φ1(ε), then

  • f − p1+p2

2

  • ≤ E + ε.
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SLIDE 19

Approximating the proof

Let us now see how one approximates the proof on the previous

  • slide. First, for trivial reasons, the polynomials can be assumed to

be in the closed ball Z of radius 5

2f (which is compact, as it lies

inside the finite dimensional space Pn).

1 for all p1, p2 ∈ Z and all ε > 0, if f − p1,

f − p2 ≤ E + Φ1(ε), then

  • f − p1+p2

2

  • ≤ E + ε.

2 (the “ε-alternation theorem”) for all p ∈ Z and all ε > 0 with

f − p ≤ E + Φ2(ε) there is a j ∈ {0, 1} and x1 < . . . < xn+1 in [0, 1] such that for every i ∈ {1, . . . , n + 1}, |(p − f )(xi) − (−1)i+jE| ≤ ε.

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SLIDE 20

Last steps

I shall omit steps 3 and 4, as I am not going to focus on them.

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Last steps

I shall omit steps 3 and 4, as I am not going to focus on them.

5 for all p1, p2 ∈ Z and all δ, β > 0, x1 < . . . < xn+1 in [0, 1]

such that for all i ∈ {1, . . . , n}, xi+1 − xi ≥ β and for all i ∈ {1, . . . , n + 1}, |(p1 − p2)(xi)| ≤ Φ5(β, δ), we have that p1 − p2 ≤ δ.

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Last steps

I shall omit steps 3 and 4, as I am not going to focus on them.

5 for all p1, p2 ∈ Z and all δ, β > 0, x1 < . . . < xn+1 in [0, 1]

such that for all i ∈ {1, . . . , n}, xi+1 − xi ≥ β and for all i ∈ {1, . . . , n + 1}, |(p1 − p2)(xi)| ≤ Φ5(β, δ), we have that p1 − p2 ≤ δ. Kohlenbach has extracted moduli Φ1-Φ5 and by putting them together he obtained the modulus of uniqueness. This was possible, by the metatheorems of proof mining, because the uniqueness proof could be formalized in WE-PAω+WKL+QF-AC0,0.

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Directions to follow

Kohlenbach also suggested in his 1990 thesis to extend the techniques to the following results:

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Directions to follow

Kohlenbach also suggested in his 1990 thesis to extend the techniques to the following results: L1-best approximation: analyzed by K. and Paulo Oliva in the early 2000s

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Directions to follow

Kohlenbach also suggested in his 1990 thesis to extend the techniques to the following results: L1-best approximation: analyzed by K. and Paulo Oliva in the early 2000s Chebyshev approximation with bounded coefficients

a 1971 result of Roulier and Taylor

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Directions to follow

Kohlenbach also suggested in his 1990 thesis to extend the techniques to the following results: L1-best approximation: analyzed by K. and Paulo Oliva in the early 2000s Chebyshev approximation with bounded coefficients

a 1971 result of Roulier and Taylor its analysis stood for 30 years as an open problem in proof mining

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Directions to follow

Kohlenbach also suggested in his 1990 thesis to extend the techniques to the following results: L1-best approximation: analyzed by K. and Paulo Oliva in the early 2000s Chebyshev approximation with bounded coefficients

a 1971 result of Roulier and Taylor its analysis stood for 30 years as an open problem in proof mining

The last one is what we are going to focus on.

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The result

Theorem (Roulier and Taylor, 1971) Let n, m ∈ N be such that m ≤ n and (ki)m

i=1 ⊆ N be such that

0 < k1 < . . . < km ≤ n. In addition, let (ai)m

i=1 and (bi)m i=1 be

finite sequences in R ∪ {±∞} be such that for all i ∈ {1, . . . , m}, ai ≤ bi, ai = ∞ and bi = −∞. If one sets K :=

n

  • i=0

ciX i ∈ Pn | for all i ∈ {1, . . . , m}, ai ≤ cki ≤ bi

  • ,

then for any continuous f : [0, 1] → R there is a unique p ∈ K such that f − p = min

q∈K f − q.

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The result

Theorem (Roulier and Taylor, 1971) Let n, m ∈ N be such that m ≤ n and (ki)m

i=1 ⊆ N be such that

0 < k1 < . . . < km ≤ n. In addition, let (ai)m

i=1 and (bi)m i=1 be

finite sequences in R ∪ {±∞} be such that for all i ∈ {1, . . . , m}, ai ≤ bi, ai = ∞ and bi = −∞. If one sets K :=

n

  • i=0

ciX i ∈ Pn | for all i ∈ {1, . . . , m}, ai ≤ cki ≤ bi

  • ,

then for any continuous f : [0, 1] → R there is a unique p ∈ K such that f − p = min

q∈K f − q.

The proof resembles the one from before, so we shall focus on the part which is fundamentally different.

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The approximate form of the new proof

In the ε-alternation step one obtains (among others) an r ≤ n, a sequence of degrees n ≥ d1 > d2 > . . . > dr+1 = 0 and x1 < . . . < xr+1 in [0, 1].

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SLIDE 31

The approximate form of the new proof

In the ε-alternation step one obtains (among others) an r ≤ n, a sequence of degrees n ≥ d1 > d2 > . . . > dr+1 = 0 and x1 < . . . < xr+1 in [0, 1]. In the last step we deal with the difference p1 − p2 as before, only we split it as p1 − p2 = Q1 + Q2 where Q2 has only terms of degrees d1, . . . , dr+1.

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SLIDE 32

The approximate form of the new proof

In the ε-alternation step one obtains (among others) an r ≤ n, a sequence of degrees n ≥ d1 > d2 > . . . > dr+1 = 0 and x1 < . . . < xr+1 in [0, 1]. In the last step we deal with the difference p1 − p2 as before, only we split it as p1 − p2 = Q1 + Q2 where Q2 has only terms of degrees d1, . . . , dr+1. It is thus enough to show that for each i, Qi ≤ δ

2.

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SLIDE 33

The approximate form of the new proof

In the ε-alternation step one obtains (among others) an r ≤ n, a sequence of degrees n ≥ d1 > d2 > . . . > dr+1 = 0 and x1 < . . . < xr+1 in [0, 1]. In the last step we deal with the difference p1 − p2 as before, only we split it as p1 − p2 = Q1 + Q2 where Q2 has only terms of degrees d1, . . . , dr+1. It is thus enough to show that for each i, Qi ≤ δ

2.

Q1 is easily bounded by classical methods (using the way the di’s were chosen).

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SLIDE 34

The approximate form of the new proof

In the ε-alternation step one obtains (among others) an r ≤ n, a sequence of degrees n ≥ d1 > d2 > . . . > dr+1 = 0 and x1 < . . . < xr+1 in [0, 1]. In the last step we deal with the difference p1 − p2 as before, only we split it as p1 − p2 = Q1 + Q2 where Q2 has only terms of degrees d1, . . . , dr+1. It is thus enough to show that for each i, Qi ≤ δ

2.

Q1 is easily bounded by classical methods (using the way the di’s were chosen). For Q2, one must generalize the proof of the original step 5.

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SLIDE 35

Proof of the original step 5

Set p := p1 − p2. By the classical Lagrangian interpolation formula, we have that: p =

n+1

  • j=1

 

i=j

X − xi xj − xi

  · p(xj).

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SLIDE 36

Proof of the original step 5

Set p := p1 − p2. By the classical Lagrangian interpolation formula, we have that: p =

n+1

  • j=1

 

i=j

X − xi xj − xi

  · p(xj).

Since we have, for all x ∈ [0, 1],

  • i=j

X − xi xj − xi

1

  • i=j β|i − j| ≤ 1

βn ,

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SLIDE 37

Proof of the original step 5

Set p := p1 − p2. By the classical Lagrangian interpolation formula, we have that: p =

n+1

  • j=1

 

i=j

X − xi xj − xi

  · p(xj).

Since we have, for all x ∈ [0, 1],

  • i=j

X − xi xj − xi

1

  • i=j β|i − j| ≤ 1

βn , we get, for all x ∈ [0, 1], |p(x)| ≤

n+1

  • j=1
  • i=j

X − xi xj − xi

  • · |p(xj)| ≤ (n + 1) · 1

βn · Φ5(β, δ).

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SLIDE 38

Proof of the original step 5

Set p := p1 − p2. By the classical Lagrangian interpolation formula, we have that: p =

n+1

  • j=1

 

i=j

X − xi xj − xi

  · p(xj).

Since we have, for all x ∈ [0, 1],

  • i=j

X − xi xj − xi

1

  • i=j β|i − j| ≤ 1

βn , we get, for all x ∈ [0, 1], |p(x)| ≤

n+1

  • j=1
  • i=j

X − xi xj − xi

  • · |p(xj)| ≤ (n + 1) · 1

βn · Φ5(β, δ). Since we want the right hand side to be smaller or equal to δ, one may take Φ5(β, δ) :=

βn n+1 · δ.

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SLIDE 39

The lemma

Our new step 5 takes the form of the following lemma. Lemma Let n, r ∈ N with r ≤ n and (di)r+1

i=1 ⊆ N with

n ≥ d1 > d2 > . . . > dr+1 = 0. Let β, δ > 0 and (xj)r+1

j=1 ⊆ [0, 1]

such that for all j ∈ {1, . . . , r}, xj+1 − xj ≥ β. Suppose that we have a polynomial p =

r+1

  • i=1

ηiX di such that for all j ∈ {1, . . . , r + 1}, |p(xj)| ≤ Φ5(β, δ). Then p ≤ δ.

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SLIDE 40

The lemma

Our new step 5 takes the form of the following lemma. Lemma Let n, r ∈ N with r ≤ n and (di)r+1

i=1 ⊆ N with

n ≥ d1 > d2 > . . . > dr+1 = 0. Let β, δ > 0 and (xj)r+1

j=1 ⊆ [0, 1]

such that for all j ∈ {1, . . . , r}, xj+1 − xj ≥ β. Suppose that we have a polynomial p =

r+1

  • i=1

ηiX di such that for all j ∈ {1, . . . , r + 1}, |p(xj)| ≤ Φ5(β, δ). Then p ≤ δ. To obtain Φ5, we need to generalize the Lagrangian formula.

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SLIDE 41

Towards the new formula

Using the form of p in the lemma, we get that for all j ∈ {1, . . . , r + 1}, p(xj) =

r+1

  • i=1

ηixdi

j .

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SLIDE 42

Towards the new formula

Using the form of p in the lemma, we get that for all j ∈ {1, . . . , r + 1}, p(xj) =

r+1

  • i=1

ηixdi

j .

Therefore, we have

     

p p(x1) . . . p(xr+1)

     

=

r+1

  • i=1

ηi

     

X di xdi

1

. . . xdi

r+1

     

,

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SLIDE 43

Towards the new formula

Using the form of p in the lemma, we get that for all j ∈ {1, . . . , r + 1}, p(xj) =

r+1

  • i=1

ηixdi

j .

Therefore, we have

     

p p(x1) . . . p(xr+1)

     

=

r+1

  • i=1

ηi

     

X di xdi

1

. . . xdi

r+1

     

, so

  • p

X d1 · · · X dr+1 p(x1) xd1

1

· · · xdr+1

1

. . . . . . ... . . . p(xr+1) xd1

r+1

· · · xdr+1

r+1

  • = 0.
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SLIDE 44

Towards the new formula

Using the form of p in the lemma, we get that for all j ∈ {1, . . . , r + 1}, p(xj) =

r+1

  • i=1

ηixdi

j .

Therefore, we have

     

p p(x1) . . . p(xr+1)

     

=

r+1

  • i=1

ηi

     

X di xdi

1

. . . xdi

r+1

     

, so

  • p

X d1 · · · X dr+1 p(x1) xd1

1

· · · xdr+1

1

. . . . . . ... . . . p(xr+1) xd1

r+1

· · · xdr+1

r+1

  • = 0.

We are thus led to use Vandermonde determinants.

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SLIDE 45

Generalizing Vandermonde

Remember the ordinary Vandermonde determinant: V (y1, . . . , yr+1) :=

  • yr

1

yr−1

1

· · · 1 yr

2

yr−1

2

· · · 1 . . . . . . ... . . . yr

r+1

yr−1

r+1

· · · 1

  • =
  • 1≤i<j≤r+1

(yi − yj).

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SLIDE 46

Generalizing Vandermonde

Remember the ordinary Vandermonde determinant: V (y1, . . . , yr+1) :=

  • yr

1

yr−1

1

· · · 1 yr

2

yr−1

2

· · · 1 . . . . . . ... . . . yr

r+1

yr−1

r+1

· · · 1

  • =
  • 1≤i<j≤r+1

(yi − yj). Now define the following generalization (where h1 > . . . > hr+1): V (h1, . . . , hr+1; y1, . . . , yr+1) :=

  • yh1

1

yh2

1

· · · yhr+1

1

yh1

2

yh2

2

· · · yhr+1

2

. . . . . . ... . . . yh1

r+1

yh2

r+1

· · · yhr+1

r+1

  • .
slide-47
SLIDE 47

Generalizing Vandermonde

Remember the ordinary Vandermonde determinant: V (y1, . . . , yr+1) :=

  • yr

1

yr−1

1

· · · 1 yr

2

yr−1

2

· · · 1 . . . . . . ... . . . yr

r+1

yr−1

r+1

· · · 1

  • =
  • 1≤i<j≤r+1

(yi − yj). Now define the following generalization (where h1 > . . . > hr+1): V (h1, . . . , hr+1; y1, . . . , yr+1) :=

  • yh1

1

yh2

1

· · · yhr+1

1

yh1

2

yh2

2

· · · yhr+1

2

. . . . . . ... . . . yh1

r+1

yh2

r+1

· · · yhr+1

r+1

  • .

Armed with these notations, by expanding the determinant on the previous slide along its first column, we get that p =

r+1

  • j=1

(−1)j−1 V (d1, . . . , dr+1; X, x1, . . . , xj, . . . , xr+1) V (d1, . . . , dr+1; x1, . . . , xr+1) · p(xj).

slide-48
SLIDE 48

Young tableaux

We shall need some definitions from algebraic combinatorics to help us in dealing with those determinants. partition: a finite sequence (λi)r+1

i=1 ⊆ N with λ1 ≥ . . . ≥ λr+1

slide-49
SLIDE 49

Young tableaux

We shall need some definitions from algebraic combinatorics to help us in dealing with those determinants. partition: a finite sequence (λi)r+1

i=1 ⊆ N with λ1 ≥ . . . ≥ λr+1

we can move bijectively between strictly decreasing sequences h and partitions λ by the formula λh

i := hi + i − r − 1

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SLIDE 50

Young tableaux

We shall need some definitions from algebraic combinatorics to help us in dealing with those determinants. partition: a finite sequence (λi)r+1

i=1 ⊆ N with λ1 ≥ . . . ≥ λr+1

we can move bijectively between strictly decreasing sequences h and partitions λ by the formula λh

i := hi + i − r − 1

if r ∈ N and λ is a partition of length r + 1, then a semistandard Young tableau of weight λ is a jagged array with r + 1 rows where for any i ∈ {1, . . . , r + 1}, the i’th line has λi entries which are elements of the set {1, . . . , r + 1}, such that the entries on each row are (weakly) increasing and the entries on each column are strictly increasing 1 1 2 7 8 2 3 3 4 4 5 6 6

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SLIDE 51

Schur functions

Now, if T is such a semistandard Young tableau in which for each i ∈ {1, . . . , r + 1}, i appears ti times in T, one denotes by yT the monomial yt1

1 . . . ytr+1 r+1. Then the Schur function associated to a

partition λ is defined by sλ :=

  • T

yT, where T ranges over all semistandard Young tableaux of weight λ.

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SLIDE 52

Schur functions

Now, if T is such a semistandard Young tableau in which for each i ∈ {1, . . . , r + 1}, i appears ti times in T, one denotes by yT the monomial yt1

1 . . . ytr+1 r+1. Then the Schur function associated to a

partition λ is defined by sλ :=

  • T

yT, where T ranges over all semistandard Young tableaux of weight λ. The result which is relevant to our ends states that for any r and any strictly decreasing h of length r + 1, V (h1, . . . , hr+1; y1, . . . , yr+1) = V (y1, . . . , yr+1) · sλh(y1, . . . , yr+1).

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SLIDE 53

Schur functions

Now, if T is such a semistandard Young tableau in which for each i ∈ {1, . . . , r + 1}, i appears ti times in T, one denotes by yT the monomial yt1

1 . . . ytr+1 r+1. Then the Schur function associated to a

partition λ is defined by sλ :=

  • T

yT, where T ranges over all semistandard Young tableaux of weight λ. The result which is relevant to our ends states that for any r and any strictly decreasing h of length r + 1, V (h1, . . . , hr+1; y1, . . . , yr+1) = V (y1, . . . , yr+1) · sλh(y1, . . . , yr+1). A simple proof may be found in:

  • R. A. Proctor, Equivalence of the combinatorial and the classical

definitions of Schur functions. J. Combin. Theory Ser. A 51, no. 1, 135–137, 1989.

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SLIDE 54

Back to the formula

The formula for p now becomes p =

n+1

  • j=1

 

i=j

X − xi xj − xi

  · p(xj) · sλd(X, x1, . . . ,

xj, . . . , xr+1) sλd(x1, . . . , xr+1) . This formula differs from the Lagrangian one only by the additional Schur factors, so we only need to bound those in order to get Φ5.

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SLIDE 55

The upper bound

For any partition λ of length r + 1, the number of semistandard Young tableaux of weight λ can be shown to be Nλ :=

  • 1≤i<j≤r+1

λi − λj + j − i j − i .

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SLIDE 56

The upper bound

For any partition λ of length r + 1, the number of semistandard Young tableaux of weight λ can be shown to be Nλ :=

  • 1≤i<j≤r+1

λi − λj + j − i j − i . Moreover, for any n there is a finite number of strictly decreasing h’s with length smaller or equal to n + 1 and with h1 ≤ n. If we set, for any n, Nn to be the maximum of all the Nλh’s for all these h’s, this number is easily seen to be computable.

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SLIDE 57

The upper bound

For any partition λ of length r + 1, the number of semistandard Young tableaux of weight λ can be shown to be Nλ :=

  • 1≤i<j≤r+1

λi − λj + j − i j − i . Moreover, for any n there is a finite number of strictly decreasing h’s with length smaller or equal to n + 1 and with h1 ≤ n. If we set, for any n, Nn to be the maximum of all the Nλh’s for all these h’s, this number is easily seen to be computable. Proposition For all n, r ∈ N with r ≤ n, any strictly decreasing h of length r + 1 and with h1 ≤ n, and any y1, . . . , yr+1 ∈ [0, 1], 0 ≤ sλh(y1, . . . , yr+1) ≤ Nn.

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SLIDE 58

The lower bound

First, for all j ∈ {2, . . . , n}, we have that 1 ≥ xk ≥ x2 ≥ x2 − x1 ≥ β.

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SLIDE 59

The lower bound

First, for all j ∈ {2, . . . , n}, we have that 1 ≥ xk ≥ x2 ≥ x2 − x1 ≥ β. Since dr+1 = 0, λd

r+1 = 0, so using the following semistandard

Young tableau of weight λd: 2 2

. . .

2 2 3 3

. . . r+1

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SLIDE 60

The lower bound

First, for all j ∈ {2, . . . , n}, we have that 1 ≥ xk ≥ x2 ≥ x2 − x1 ≥ β. Since dr+1 = 0, λd

r+1 = 0, so using the following semistandard

Young tableau of weight λd: 2 2

. . .

2 2 3 3

. . . r+1

we get that sλd(x1, . . . , xr+1) ≥ x

λd

1

2 . . . xλd

r

r+1 ≥ β

r

i=1 λd i

≥ βr·λd

1 = βr(d1−r) ≥ βr(n−r) ≥ β n2 4 .

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SLIDE 61

Wrapping up

We may take then

  • Φ5(β, δ) :=

βn+ n2

4

Nn(n + 1) · δ.

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SLIDE 62

Wrapping up

We may take then

  • Φ5(β, δ) :=

βn+ n2

4

Nn(n + 1) · δ. The lower bound also shows that the “Lagrange-Schur” formula for p is well-defined, i.e. that the denominator is nonzero.

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SLIDE 63

Wrapping up

We may take then

  • Φ5(β, δ) :=

βn+ n2

4

Nn(n + 1) · δ. The lower bound also shows that the “Lagrange-Schur” formula for p is well-defined, i.e. that the denominator is nonzero. In addition, like with the original Lagrange formula, we may also show the existence of an interpolation polynomial with prescribed degrees, by reversing the above argument (there is a catch, but it is easily taken care of).

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SLIDE 64

The final modulus

Of course, there is much more to the extraction of the modulus. For example, the Schur formula also plays a role in the corresponding ε-alternation result.

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SLIDE 65

The final modulus

Of course, there is much more to the extraction of the modulus. For example, the Schur formula also plays a role in the corresponding ε-alternation result. In the end, we get the modulus

  • f uniqueness

Ψ(δ) :=

  • χω,n,M( L

2)

2

n2

2 +2n

10 · N2

n(n + 1)(nFn + 1) · δ,

which depends (in addition to δ) on the norm of a polynomial p0 in K; the degree n; a lower bound L on E; a modulus of uniform continuity ω for f ; the norm of f .

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SLIDE 66

Some remarks

The modulus does not depend on the bounds on the coefficients, except via p0, which is in line with what Kohlenbach’s metatheorems predict.

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SLIDE 67

Some remarks

The modulus does not depend on the bounds on the coefficients, except via p0, which is in line with what Kohlenbach’s metatheorems predict. The dependence on the norm of f may be removed at virtually no cost, by a shifting trick.

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SLIDE 68

Some remarks

The modulus does not depend on the bounds on the coefficients, except via p0, which is in line with what Kohlenbach’s metatheorems predict. The dependence on the norm of f may be removed at virtually no cost, by a shifting trick. The fact that the modulus is linear in δ corresponds to its coefficient being what approximation theorists call a constant

  • f strong unicity, the existence of which having been shown

before in this setting only nonconstructively.

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SLIDE 69

Some remarks

The modulus does not depend on the bounds on the coefficients, except via p0, which is in line with what Kohlenbach’s metatheorems predict. The dependence on the norm of f may be removed at virtually no cost, by a shifting trick. The fact that the modulus is linear in δ corresponds to its coefficient being what approximation theorists call a constant

  • f strong unicity, the existence of which having been shown

before in this setting only nonconstructively. One may even remove the dependence on L, though at the expense of linearity.

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SLIDE 70

All this can be found in:

  • A. Sipos

¸, Bounds on strong unicity for Chebyshev approximation with bounded coefficients. arXiv:1904.10284 [math.CA], 2019.

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SLIDE 71

Thank you for your attention.