Abstract:We consider the polynomials tφnpz, wqu orthogonal on the circle with respect to a weight w that satisfies w, w´1 P L 8 pTq and show that }φnpe iθ , wq} L 8 pTq can grow in n at a certain rate.
“…Construct a Krein system with the coefficient a(r) = − 1 2 p(r/2)+ i 2 q(r/2), where p, q are the potentials in equation (1). Uniqueness theorem and (12) give that functions ϕ and ψ defined by (10) and (11) respectively are the unique solutions of equation (1). Since potentials p, q are in L 2 (R + ), coefficient a is also in L 2 (R + ).…”
Section: Dirac Equation Proof Of Theoremmentioning
We prove the Cesàro boundedness of eigenfunctions of the Dirac operator on the half-line with a square-summable potential. The proof is based on the theory of Krein systems and, in particular, on the continuous version of a theorem by A.
“…Construct a Krein system with the coefficient a(r) = − 1 2 p(r/2)+ i 2 q(r/2), where p, q are the potentials in equation (1). Uniqueness theorem and (12) give that functions ϕ and ψ defined by (10) and (11) respectively are the unique solutions of equation (1). Since potentials p, q are in L 2 (R + ), coefficient a is also in L 2 (R + ).…”
Section: Dirac Equation Proof Of Theoremmentioning
We prove the Cesàro boundedness of eigenfunctions of the Dirac operator on the half-line with a square-summable potential. The proof is based on the theory of Krein systems and, in particular, on the continuous version of a theorem by A.
“…Thus, log w P L 1 pTq as well. This means that µ : dµ " w 2π dθ belongs to Szegő class of measures and, consequently (see [9]),…”
Section: Weighted Operators Are Continuous In W Pmentioning
confidence: 99%
“…From lemma 3.2 and lemma 3.4, we get that p cr ptq ą 2 and lim tÑ1 p cr ptq " 8. To show that p cr ptq Ñ 2 when t Ñ 8, we use the following result established in [9], theorem 3.2: given any t ą 2, there is a weight w that satisfies 1 w t and a subsequence tk n u such that…”
Section: Weighted Operators Are Continuous In W Pmentioning
We consider weighted operators acting on L p pR d q and show that they depend continuously on the weight w P AppR d q in the operator topology. Then, we use this result to estimate L p w pTq norm of polynomials orthogonal on the unit circle when the weight w belongs to Muckenhoupt class A 2 pTq and p ą 2. The asymptotics of the polynomial entropy is obtained as an application.
Contentsw pTq 7 4. The Christoffel-Darboux Kernel and bounds for the associated Projection Operator 13 5. Weights in A 2 pTq and their Aleksandrov-Clark measures 14 6. Appendix: Fisher-Hartwig weights 17 References 182010 Mathematics Subject Classification. 42B20, 42C05.
“…This question was answered in the affirmative in [4,5], which imposed w, w −1 ∈ L ∞ (T) and w, w −1 ∈ BMO(T), respectively, although both consider only polynomials orthogonal with respect to absolutely continuous measures. Both conditions are sufficient to break the n 1/2 barrier, and lower bounds were established in [4] showing that its results are sharp in some regimes.…”
Section: Steklov Problems In Orthogonal Polynomialsmentioning
We consider randomized Verblunsky parameters for orthogonal polynomials on the unit circle as they relate to the problem of Steklov, bounding the polynomials' uniform norm independent of n.
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