FLATNESS OF CONJUGATE RECIPROCAL UNIMODULAR POLYNOMIALS. June 24, 2015

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1 FLATNESS OF CONJUGATE RECIPROCAL UNIMODULAR POLYNOMIALS Tamás Erdélyi June 24, 2015 Abstract. A polynomial is called unimodular if each of its coefficients is a complex number of modulus 1. A polynomial P of the form P(z) = n j=0 a jz j is called conjugate reciprocal if a n j = a j, a j C for each j = 0,1,...,n. Let D be the unit circle of the complex plane. We prove that there is an absolute constant ε > 0 such that max f(z) (1+ε) 4/3m 1/2, z D for every conjugate reciprocal unimodular polynomial of degree m. We also prove that there is an absolute constant ε > 0 such that M q (f ) exp(ε(q 2)/q) 1/3m 3/2, 1 q < 2, and M q (f ) exp(ε(q 2)/q) 1/3m 3/2, 2 < q, for every conjugate reciprocal unimodular polynomial of degree m, where M q (g) = ( 1 2π 2π 0 g(e it ) q dt) 1/q, q > Introduction LetT n bethesetofallreal trigonometricpolynomialsofdegreeatmost n. Let Pn c bethe set of all algebraic polynomials of degree at most n with complex coefficients. Throughout this paper it will be comfortable for us to denote an appropriate period [a,a+2π) by. Let n A n := Q : Q(t) = cos(jt+γ j ), γ j R j=1 ey words and phrases. Littlewood polynomials; unimodular polynomials; conjugate reciprocal polynomials; flatness properties Mathematics Subject Classifications. 11C08, 41A17 1 Typeset by AMS-TEX

2 and n B n+1/2 := Q : Q(t) = ( ) 2j +1 cos t+γ j, γ j R 2. j=0 We use the notation Q p := ( ) 1/p 1 Q(t) p, p > 0, 2π and Q := max t Q(t). The Bernstein Szegő inequality (see p. 232 in [7], for instance) gives that Q (t) 2 +n 2 Q(t) 2 n 2 Q 2, Q T n, t R. Integrating the left hand side on the period and using Parseval s formula we obtain n(n+1)(2n+1) 12 + n3 2 n2 Q 2, Q A n, and hence (1.1) Q 4/3 n/2, Q A n. One of the highlights of this paper is to improve (1.1) by showing that there is an absolute constant ε > 0 such that Q (1+ε) 4/3 n/2, Q A n. Let n m := P : P(z) = a j z j, a j C, a j = 1, j = 0,1,...,m j=0 be the set of all unimodular polynomials of degree m. Associated with an algebraic polynomial P of the form P(z) = m a j z j, a j C, a m 0, j=0 let m P(z) := a j z j and P (z) := z m P(1/z). j=0 2

3 The polynomial P of degree m is called conjugate reciprocal if P = P. The classes A n, B n+1/2, and m and flatness properties of their elements were studied by many authors, see [1 40], for instance. Let and M q (f) := f(e it ) q = ( 1/q 1 f(e it ) dt) q, q (0, ), 2π M (f) := sup f(e it ). t There is a beautiful short argument to see that (1.2) M (f) 4/3m 1/2 for every conjugate reciprocal unimodular polynomial f m. Namely, Parseval s formula gives ( ) 1/2 m(m+1)(2m+1) M (f ) M 2 (f ) =, f m. 3 Combining this with Lax s Bernstein-type inequality M (f ) m 2 M (f) valid for all conjugate reciprocal algebraic polynomials f Pn c instance), we obtain (see p. 438 in [7], for ( ) 1/2 m(m+1)(2m+1) 4/3m 1/2 M (f) 2 m 3 for all conjugate reciprocal unimodular polynomials f m. One of the highlights of this paper is to improve (1.2) by showing that there is an absolute constant ε > 0 such that M (f) (1+ε) 4/3m 1/2, for every conjugate reciprocal unimodular polynomial f m. We also prove that there is an absolute constant ε > 0 such that M q (f ) exp(ε(q 2)/q) 1/3m 3/2, 1 q < 2, and M q (f ) exp(ε(q 2)/q) 1/3m 3/2, 2 < q, for every conjugate reciprocal unimodular polynomial of degree m. See Theorem

4 2. New Results Theorem 2.1. Let Q A n and P = (Q ) 2 +n 2 Q 2. There is an absolute constant δ > 0 such that P 1/2 (1 δ) P 1. Theorem 2.1*. Let Q B n+1/2 and P = (Q ) 2 + (n + 1/2) 2 Q 2. There is an absolute constant δ > 0 such that P 1/2 (1 δ) P 1. Theorem 2.2. Let Q A n and P = (Q ) 2 +n 2 Q 2. There is an absolute constant δ > 0 such that P (1+δ) P 1. Theorem 2.2*. Let Q B n+1/2 and P = (Q ) 2 + (n + 1/2) 2 Q 2. There is an absolute constant δ > 0 such that P (1+δ) P 1. Theorem 2.3. There is an absolute constant δ > 0 such that for every Q A n. Q (1+δ) 4/3 n/2 Theorem 2.3*. There is an absolute constant δ > 0 such that for every Q B n+1/2. Q (1+δ) 4/3 n/2 Let D be the unit circle of the complex plane. Let f be a continuous function on D and let I q (f) := M q (f) q = 1 f(e it ) q dt 2π and M (f) := max z D f(z). Theorem 2.4. There is an absolute constant ε > 0 such that M 1 (f ) (1 ε) 1/3m 3/2 for every conjugate reciprocal unimodular polynomial f m. Theorem 2.5. There is an absolute constant ε > 0 such that M (f ) (1+ε) 1/3m 3/2 for every conjugate reciprocal unimodular polynomial f m. 4

5 Theorem 2.6. There is an absolute constant ε > 0 such that M (f) (1+ε) 4/3m 1/2 for every conjugate reciprocal unimodular polynomial f m. Theorem 2.7. There is an absolute constant ε > 0 such that M q (f ) exp(ε(q 2)/q) 1/3m 3/2, 1 q < 2, and M q (f ) exp(ε(q 2)/q) 1/3m 3/2, 2 < q, for every conjugate reciprocal unimodular polynomial f m. The above results were well known before without the absolute constants δ > 0 and ε > 0, respectively. Remark 2.1. The factor (1+δ) in Theorem 2.2 cannot be replaced by (1+δ)3/2. Remark 2.2. The factor (1+δ) 4/3 in Theorem 2.3 cannot be replaced by (1+δ) 2. Remark 2.3. The factor (1+ε) 1/3 in Theorem 2.5 cannot be replaced by (1+ε) 1/2. Remark 2.4. The factor (1+ε) 4/3 in Theorem 2.6 cannot be replaced by (1+ε) 2. A polynomial f P c m is called skew-reciprocal if f (z) = f( z). A polynomial f P c m is called plain-reciprocal if f = f, that is, f(z) = z m f(1/z) for all z C\{0}. Observe that Corollary 2.8 in [28] may be formulated as follows. Remark 2.5. There is an absolute constant ε > 0 such that max z D f (z) min z D f (z) εm 3/2 for all conjugate reciprocal, plain-reciprocal, and skew-reciprocal unimodular polynomials f m. Observe that for conjugate reciprocal unimodular polynomials Theorem 2.5 is stronger than Remark 2.5. Problem 2.1. Is there an absolute constant ε > 0 such that M (f ) (1+ε) 1/3m 3/2 holds for all plain-reciprocal and skew-reciprocal unimodular polynomials f m? 5

6 Problem 2.2. Is there an absolute constant ε > 0 such that or at least M (f ) (1+ε) 1/3m 3/2 max z D f (z) min z D f (z) εm 3/2 holds for all unimodular polynomials f m? Our methodto provetheorem 2.5doesnot seem towork for allunimodular polynomials f m. In an communication several years ago B. Saffari speculated that the answer to Problem 2.2 is no. However we do not know the answer even to Problem 2.1. Let L m be the collection of all polynomials of degree m with each of their coefficients in { 1,1}. Problem 2.3. Is there an absolute constant ε > 0 such that or at least M (f ) (1+ε) 1/3m 3/2 max z D f (z) min z D f (z) εm 3/2 holds for all Littlewood polynomials f L m? The following problem due to Erdős [29] is open for a long time. Problem 2.4. Is there an absolute constant ε > 0 such that or at least M (f) (1+ε)m 1/2 max f(z) min f(z) εm1/2 z D z D holds for all Littlewood polynomials f L m? The same problem may be raised only for all skew reciprocal Littlewood polynomials f L m and as far as we know, it is also open. 3. Lemmas Let m(a) denote the Lebesgue measure of a measurable set A R. The following lemma is due to Littlewood, see Theorem 1 in [34]. Lemma 3.1. Let R T n be of the form n R(t) = R n (t) = a j cos(jt+γ j ) j=1 6 a j,γ j R, j = 1,2,...,n.

7 Let s m := m j=1 a2 j, m = 1,2,...,n, and let µ := R 2, that is, µ 2 = s n. Suppose R 1 cµ, where c > 0 is a constant (necessarily not greater than 1). Suppose also that the coefficients of R satisfy s [n/h] /s n = µ 2 a 2 j 2 9 c 6 1 j n/h for some constant h > 0. Let V = 2 5 c 3. Then there exists a constant B > 0 depending only on c and h such that m({t : v 1 µ R(t) v 2 µ}) B(v 2 v 1 ) 2 for every v 1 and v 2 such that V v 1 < v 2 V. Lemma 3.2. Associated with Q T n we define the sets E δ := {t : Q (t) < δn 3/2 } and We have F δ := {t : Q (t) δ 1/2 n 5/2 }. m(e δ \F δ ) 8δ 1/2. Proof of Lemma 3.2. Observe that E δ \F δ is the union of at most 4n pairwise disjoint open subintervals of the period. Let these intervals be (x j,y j ),j = 1,2,...,µ, where µ 4n. By the Mean Value Theorem we can deduce that there are ξ j (x j,y j ) such that and hence Hence 2δn 3/2 Q (y j ) Q (x j ) = Q (ξ j ) (y j x j ) δ 1/2 n 5/2 (y j x j ), y j x j 2δ 1/2 n 1, j = 1,2,...,µ. m(e δ \F δ ) = µ (y j x j ) µ(2δ 1/2 n 1 ) 8δ 1/2. j=1 Lemma 3.3. Let Q A n, P := (Q ) 2 +n 2 Q 2, δ (0,1), and Suppose G δ := {t : P(t) 1/2 P 1/2 1 δ 1/4 P 1/2 1 }. (3.1) P 1/2 (1 δ) P 1. 7

8 Then m( \G δ ) 4πδ 1/2. Proof of Lemma 3.3. Using (3.1) we have (3.2) P 1/2 1/2 (1 δ)1/2 P 1/2 1 (1 δ) P 1/2 1. Hence P(t) 1/2 P 1/2 1 2 dt = 4π P 1/2 1 ( 1/2 P 1 P 1/2 ) 1/2 4π P 1/2 1 δ P 1/2 1 = 4πδ P 1. Letting a := m( \G δ ) we have and the lemma follows. aδ 1/2 P 1 4πδ P 1, Lemma 3.4. Let Q A n, P := (Q ) 2 + n 2 Q 2, and P 1/ P 1. Then R := n 2 Q 2 +Q satisfies the assumptions of Lemma 3.1 with c := 1/32 and h = for all sufficiently large n. Proof of Lemma 3.4. Let n 3. Observe that n R(t) = a j cos(jt+γ j ), j=1 a j := n 2 j 2, γ j R, j = 1,2,...,n. Then hence Using Parseval s formula, we have s n = µ 2 = R 2 2 = 1 2 (3.3) P 1 = 1 2 n (n 2 j 2 ) 2, j=1 n 5 6 s n = µ 2 n5 2. n j=1 (j 2 +n 2 ) 2n3 3, (3.4) Q 1 Q n j=1 8 j 4 1/2 (1+o(1)) n5/2 10,

9 and (3.5) Q n j=1 j 2 1/2 (1+o(1)) n3/2 6, and hence (3.6) nq 1 =(2π) 1 (2π) 1 P(t) Q (t) 2 1/2 dt P(t) 1/2 dt (2π) 1 Q (t) dt ( ) 1/2 = P 1/2 31 1/2 Q 1 P 1/2 1 Q n3/2 (1+o(1)) 6 n3/2. Combining (3.5) and (3.4) we conclude R 1 = n 2 Q+Q 1 n 2 Q 1 Q n5/2 (1+o(1)) 1 32 n5/2 6 n5/2 (1+o(1)) n5/2 10 forallsufficientlylargen. Also,s [n/h] (n/h)n 4 = n 5 /h,hences [n/h] /s n 1/h. Therefore the assumptions of Lemma 3.1 are satisfied with c := 1/32 and h = Proof of the Theorems Proof of Theorem 2.1. Let Q A n, P = (Q ) 2 +n 2 Q 2, and R := n 2 Q 2 +Q. Let δ (0,1). Suppose P 1/2 (1 δ) P 1. Lemma 3.4 states that if 0 < δ 1/32 then R satisfies the assumptions of Lemma 3.1 with c = 1/32 and h = Now let and E δ := {t : Q (t) < δn 3/2 }, F δ := {t : Q (t) δn 5/2 }, G δ := {t : P(t) 1/2 P 1/2 1 δ 1/4 P 1/2 1 }, Recall that by the Parseval formula we have H γ := {t : γn 5/2 R(t) < 2γn 5/2 }. (4.1) P 1 = n3 2 + n(n+1)(2n+1). 12 9

10 Hence, if t G δ E δ F δ and the absolute constant δ > 0 is sufficiently small, then that is, R(t) n 2 Q(t) Q (t) = n(p(t) Q (t) 2 ) 1/2 Q (t) ( n n ((1 δ 1/4 ) n(n+1)(2n+1) ) ) 1/2 δ 2 n 3 δn 5/ n5/2, (4.2) R(t) 1 2 n5/2, t G δ E δ F δ. By Lemma 3.2 we have (4.3) m(e δ \F δ ) 8δ 1/2. By Lemma 3.3 we have (4.4) m( \G δ ) 4πδ 1/2. Observe that if 0 < γ < 1/4 then (4.2) implies that H γ \(G δ E δ F δ ), hence H γ E δ (E δ \G δ ) (E δ \F δ ). Therefore, by (4.3) and (4.4) we can deduce that (4.5) m(h γ E δ ) m(e δ \G δ )+m(e δ \F δ ) 4πδ 1/2 +8δ 1/2. By Lemmas 3.1 and 3.4 there are absolute constants 0 < γ < 1/4 and B > 0 such that (4.6) m(h γ ) Bγ 2. It follows from (4.5) and (4.6) that (4.7) m(h γ \E δ ) 1 2 Bγ2 for all sufficiently small absolute constants δ > 0. Observe that (4.8) 2Q (t)r(t) 2δn 3/2 γn 5/2 = 2γδn 4, t H γ \E δ, and (4.9) P (t) = 2Q (t)r(t). 10

11 Combining (4.7), (4.8), and (4.9), we obtain m({t : P (t) 2γδn 4 }) 1 2 Bγ2, and hence (4.10) P (t) dt 1 2 Bγ2 (2γδn 4 ) = Bγ 3 δn 4. Now let P := P 2π P 1 T 2n. Then (4.10) can be rewritten as P (t) dt Bγ 3 δn 4, and by Bernstein s inequality in L 1 (see p. 390 of [7], for instance), we have (4.11) 2π P 1 = P(t) dt 1 2 Bγ3 δn 3. Observe that (4.12) 2π P 1 = = ( P(t) dt P(t) P 1 dt (P(t) 1/2 P 1/2 1 =2π ( 2 P 1/2 1 ( P 1/2 1 P 1/2 4π P 1/2 1 Combining (4.11), (4.12), and (4.1), we conclude ( P(t) 1/2 P 1/2 )( 1 P(t) 1/2 + P 1/2 ) dt 1 ) 1/2 ( ) 2 dt (P(t) 1/2 + P 1/2 1/2 2 1 dt )) 1/2 ( 1/2 1/2 2 P 1 ( ) P 1 P ( 1/2 ) 1/2 = 4πn 3/2 1/2. P 1 P 1/2 P 1 P 1/2 ( 2π P 1 4πn 3/2 δ P 1 with an absolute constant δ > 0. ( P 1/2 1 + P 1/2 ) 2 ( Bγ 3 δn 3/2 ) 2 δ n 3 8π 1/2 )) 1/2 Proof of Theorem 2.2. By Theorem 2.1 there is an absolute constant δ > 0 such that P 1 = 2π P(t) dt = 2π P(t) 1/2 P(t) 1/2 dt 2π P(t) 1/2 P 1/2 dt P 1/2 1/2 P 1/2 (1 δ)1/2 P 1/2 1 P 1/2. 11

12 Hence and the result follows. P 1/2 1 (1 δ) 1/2 P 1/2, Proof of Theorem 2.3. The Bernstein Sze go inequality(see p. 232 of[7],for instance) yields hence if P = (Q ) 2 +n 2 Q 2, then Q (t) 2 +n 2 Q(t) 2 n 2 Q 2, t R, Q A n T n, P n 2 Q. Hence, using Theorem 2.1 and Parseval s formula we can deduce that Q 2 n 2 P n 2 (1+δ) P 1 = n 2 (1+δ) ( ) Q 2 2 +n2 Q 2 2 ( ) n(n+1)(2n+1) =n 2 (1+δ) + n3 (1+δ)(4/3)(n/2) 12 2 with an absolute constant δ > 0 and the theorem follows. The proofs of Theorems 2.1*, 2.2*, and 2.3* are similar to those of Theorems 2.1 and 2.2, respectively. The modifications required in the proofs of Theorems 2.1* and 2.2* are straightforward for the experts and we omit the details. Proof of Theorem 2.4. First assume that m = 2n is even and f m is a conjugate reciprocal unimodular polynomial. Let f(z) = m j=0 a jz j, where a j C and a j = 1 for each j = 0,1,...m. As f is conjugate reciprocal, we have a m j = a j, j = 0,1,...,m, and a n { 1,1}, in particular. Let Q A n be defined by 2Q(t) = e int f(e it ) a n. Then hence the triangle inequality implies that ie it f (e it ) = e int (2Q (t)+in(2q(t)+a n )), f (e it ) 2 e int (Q (t)+inq(t)) + e int ina n = 2 Q (t)+inq(t) +n = 2 P(t) 1/2 +n, where P := (Q ) 2 + n 2 Q 2 is the same as in Theorem 2.1, and the theorem follows from Theorem 2.1 as M 1 (f ) 2 P 1/2 1/2 +n 2(1 δ)1/2 P 1/2 1 +n ( ) 1/2 n(n+1)(2n+1) 2(1 δ) 1/2 + n3 +n 12 2 ( ) 2(n+1) 2(1 δ) 1/2 3 1/2 +n 3 (1 δ) 1/2 1/3m 3/2 +o(m 3/2 ). 12

13 Now assume that m = 2n+1 is odd and f m is a conjugate reciprocal unimodular polynomial. Let Q B m/2 be defined by 2Q(t) = e imt/2 f(e it ). Then implies that ie it f (e it ) = 2e imt/2 (Q (t)+(im/2)q(t)) f (e it ) = 2 e imt/2 (Q (t)+(im/2)q(t)) = 2 Q (t)+(im/2)q(t) = 2 P(t) 1/2, where P := (Q ) 2 +(n+1/2) 2 Q 2 is the same as in Theorem 2.1*, and the theorem follows from Theorem 2.1* as M 1 (f ) 2 P 1/2 1/2 2(1 δ)1/2 P 1/2 1 ( (n+1)(n+2)(2n+3) 2(1 δ) 1/2 12 ( ) 2(n+1) 2(1 δ) 1/2 3 1/2 3 (1 δ) 1/2 1/3m 3/2 +o(m 3/2 ). ) 1/2 + (n+1)3 2 Proof of Theorem 2.5. Let f m be a conjugate reciprocal unimodular polynomial. By Theorem 2.4 there is an absolute constant ε > 0 such that m(m+1)(2m+1) 6 = ( M 2 (f ) ) 2 = 2π 2π M 1 (f )M (f ) f (e it ) max τ f (e iτ ) dt (1 ε) 1/3m 3/2 M (f ). f (e it ) 2 dt = 2π f (e it ) f (e it ) dt Hence 1/3m 3/2 (1 ε)m (f ), and the theorem follows. Proof 1 of Theorem 2.6. First assume that m = 2n is even and f m is a conjugate reciprocal unimodular polynomial. Let f(z) = m j=0 a jz j, where a j C and a j = 1 for each j = 0,1,...m. As f is conjugate reciprocal, we have a m j = a j, j = 0,1,...,m, 13

14 and a n { 1,1}, in particular. Let Q A n be defined by 2Q(t) = e int f(e it ) a n. Observe that max f(z) 2Q z D 1, hence the theorem follows from Theorem 2.3. Now assume that m = 2n + 1 is odd and f m is a conjugate reciprocal unimodular polynomial. Let Q B n/2 be defined by 2Q(t) = e imt/2 f(e it ). Observe that max f(z) = 2Q, z D hence the theorem follows from Theorem 2.3*. Proof 2 of Theorem 2.6. It is well known (see p. 438 of [7], for instance) that if f is a conjugate reciprocal unimodular polynomial of degree m then f = (m/2) f. Hence the theorem follows from a combination of this and Theorem 2.5. Proof of Theorem 2.7. Let f m be conjugate reciprocal. Observe that by Parseval s formula we have ( ) 1/2 m(m+1)(2m+1) (4.13) M 2 (f ) = = (1+o(1)) m3/ As we will see, both inequalities of the theorem follow from Theorem 2.4, (4.13), and the following convexity property of the function h(q) := qlog(m q (f)) on (0, ). Let f be a continuous function on D and let I q (f) := M q (f) q = 1 2π f(e it ) q dt. Then h(q) := log(i q (f)) = qlog(m q (f)) is a convex function of q on (0, ). This is a simple consequence of Hölder s inequality. For the sake of completeness, before we apply it, we present the short proof of this fact. We need to see that if q < r < p, then that is, (4.14) To see this let I r (f) I p (f) r q p q Iq (f) p r p q, ( p q ( ) r q ( p r f(e it ) dt) r f(e it ) p dt f(e it ) dt) q. 2π 2π 2π α := p q r q, hence 1/α+1/β = 1 and γ +δ = r. Let p q β := p r, γ := p α, δ := q β, F(t) := f(e it ) γ = f(e it ) p(r q) p q, 14

15 and Then by Hölder s inequality we conclude G(t) := f(e it ) δ = f(e it ) q(p r) p q. ( F(t)G(t)dt ) 1/α ( 1/β F(t) α dt G(t) dt) β, and (4.14) follows. Let q [1,2). Then, using the convexity property of the function h(q) := qlog(m q (f)) on (0, ), we obtain 2logM 2 qlogm q 2 q 2logM 2 logm Combining this with the Theorem 2.4 and (4.13) gives theorem. Now let q (2, ). Then, using the convexity property of the function h(q) := qlog(m q (f)) on (0, ), we obtain qlogm q 2logM 2 q 2 2logM 2 logm Combining this with the Theorem 2.4 and (4.13) gives theorem. Proof of Remark 2.1. Let (f n ) be anultraflat sequence of unimodular polynomialsf n n satisfying M (f n ) (1+ε n ) n with a sequence (ε n ) of numbers ε n > 0 converging to 0. It is shown in [7] that such a sequence (f n ) exists. Let g n (z) = zf n 1 (z). Let Q n A n be defined by Q n (t) := Re(g n (e it )). Then the Bernstein Szegő inequality (see p. 232 in [7], for instance) gives that P n := (Q n) 2 +n 2 Q 2 n satisfy while by Parseval s formula we have P n n 2 Q n 2 (1+ε n) 2 n 3, P n 1 = n3 2 + n(n+1)(2n+1) 12 2n3 3. Proof of Remark 2.2. Let Q n A n be the same as in the proof of Remark 2.1. Then Q n P n 1/2 (1+ε n)n 3/2. Proof of Remark 2.4. Let f n n and g n (z) = zf n 1 (z) be the same as in the proof of Remark 2.1. For m = 2n we define h m m by h m (z) := z n (g n (z)+g n (1/z)+1. 15

16 We have M (h m ) 2(1+ε n ) n+1 (1+ε n ) 2 m+1. Proof of Remark 2.3. For m = 2n let h m m be the same as in the proof of Remark 2.4. Then using the well-known Bernstein-type inequality for conjugate reciprocal polynomials (see p. 438 in [7], for instance), we have M (h m ) m 2 (1+ε n) 2 m 1 2 (1+ε n )m 3/2. References 1. J. Beck, Flat polynomials on the unit circle note on a problem of Littlewood, Bull.London Math. Soc. 23 (1991), E. Bombieri and J. Bourgain, On ahane s ultraflat polynomials, J. Eur. Math. Soc. 11 (2009, 3), P. Borwein, Computational Excursions in Analysis and Number Theory, Springer, New York, P. Borwein and.-. S. Choi, Explicit merit factor formulae for Fekete and Turyn polynomials, Trans. Amer. Math. Soc. 354 (2002), no P. Borwein and T. Erdélyi, Polynomials and Polynomial Inequalities, Springer-Verlag, New York, P. Borwein and.-. S. Choi, The average norm of polynomials of fixed height, Trans. Amer. Math. Soc. 359 (2007), no P. Borwein,.S. Choi, and R. Ferguson, Norm of Littlewood cyclotomic polynomials, Math. Proc. Camb. Phil. Soc. 138 (2005), P. Borwein, T. Erdélyi, and G. ós, Littlewood-type problems on [0, 1], Proc. London Math. Soc. (3) 79 (1999), P. Borwein and M.J. Mossinghoff, Rudin-Shapiro like polynomials in L 4, Math. Comp. 69 (2000), P. Borwein and R. Lockhart, The expected L p norm of random polynomials, Proc. Amer. Math. Soc. 129 (2001), J. Brillhart, J.S. Lemont, and P. Morton, Cyclotomic properties of the Rudin-Shapiro polynomials, J. Reine Angew. Math. (Crelle s J.) 288 (1976), J.S. Byrnes, On polynomials with coefficients of modulus one, Bull London Math. Soc. 9 (1977), S. Choi and T. Erdélyi, Sums of monomials with large Mahler measure, J. Approx. Theory 197 (2015), S. Choi and T. Erdélyi, On the average Mahler measures on Littlewood polynomials, Proc. Amer. Math. Soc. Ser. B 1 (2015),

17 S. Choi and T. Erdélyi, On a problem of Bourgain concerning the L p norms of exponential sums, Math. Zeitschrift 279 (2015), S. Choi and M.J. Mossinghoff, Average Mahler s measure and Lp norms of unimodular polynomials, Pacific J. Math. 252 (2011), no. 1, Ch. Doche, Even moments of generalized Rudin-Shapiro polynomials, Math. Comp. 74 (2005), no. 252, Ch. Doche and L. Habsieger, Moments of the Rudin-Shapiro polynomials, J. Fourier Anal. Appl. 10 (2004), no. 5, T. Erdélyi, The resolution of Saffari s phase problem, C.R. Acad. Sci. Paris Sér. I Math. 331 (2000), T. Erdélyi, The phase problem of ultraflat unimodular polynomials: the resolution of the conjecture of Saffari, Math. Ann. 321 (2001), T. Erdélyi, Proof of Saffari s near orthogonality conjecture for ultraflat sequences of unimodular polynomials, C.R. Acad. Sci. Paris Sér. I Math. 333 (2001), T. Erdélyi, Polynomials with Littlewood-type coefficient constraints, in Approximation Theory X: Abstract and Classical Analysis, Charles. Chui, Larry L. Schumaker, and Joachim Stöckler (Eds.) (2002), Vanderbilt University Press, Nashville, TN, T. Erdélyi, On the real part of ultraflat sequences of unimodular polynomials, Math. Ann. 326 (2003), T. Erdélyi, On the L q norm of cyclotomic Littlewood polynomials on the unit circle., Math. Proc. Cambridge Philos. Soc. 151 (2011), T. Erdélyi, Sieve-type lower bounds for the Mahler measure of polynomials on subarcs, Computational Methods and Function Theory 11 (2011), T. Erdélyi, Upper bounds for the Lq norm of Fekete polynomials on subarcs, Acta Arith. 153 (2012), no. 1, T. Erdélyi and D. Lubinsky, Large sieve inequalities via subharmonic methods and the Mahler measure of Fekete polynomials, Canad. J. Math. 59 (2007), T. Erdélyi and P. Nevai, On the derivatives of unimodular polynomials, manuscript (2014). 29. P. Erdős, Some unsolved problems, Michigan Math. J. 4 (1957), P. Erdős, An inequality for the maximum of trigonometric polynomials, Annales Polonica Math. 12 (1962), M.J. Golay, Static multislit spectrometry and its application to the panoramic display of infrared spectra,, J. Opt. Soc. America 41 (1951), J.P. ahane, Sur les polynomes a coefficient unimodulaires, Bull. London Math. Soc. 12 (1980), T. örner, On a polynomial of J.S. Byrnes, Bull. London Math. Soc. 12 (1980), J.E. Littlewood, The real zeros and value distributions of real trigonometrical polynomials, J. London Math. Soc. 41 (1966), J.E. Littlewood, On polynomials ±z m, exp(α m i)z m,z = e iθ, J. London Math. Soc. 41 (1966), J.E. Littlewood, Some Problems in Real and Complex Analysis, Heath Mathematical Monographs, Lexington, Massachusetts,

18 37. H.L. Montgomery, An exponential polynomial formed with the Legendre symbol, Acta Arith. 37 (1980), H. Queffelec and B. Saffari, On Bernstein s inequality and ahane s ultraflat polynomials, J. Fourier Anal. Appl. 2 (1996, 6), B. Saffari, The phase behavior of ultraflat unimodular polynomials, Probabilistic and Stochastic Methods in Analysis, with Applications (J. S. Byrnes et al., eds.), luwer Academic Publishers, Printed in the Netherlands, 1992, pp H.S. Shapiro, Master thesis, MIT, Department of Mathematics, Texas A&M University, College Station, Texas (T. Erdélyi) address: terdelyi@math.tamu.edu 18

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