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On some Classes of Fourier Series
Author(s) -
Verblunsky S.
Publication year - 1932
Publication title -
proceedings of the london mathematical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.899
H-Index - 65
eISSN - 1460-244X
pISSN - 0024-6115
DOI - 10.1112/plms/s2-33.1.562-t
Subject(s) - mathematics , combinatorics , bounded function , locally integrable function , order (exchange) , measurable function , function (biology) , constant (computer programming) , mathematical analysis , integrable system , finance , evolutionary biology , computer science , economics , biology , programming language
Equation (36) on p. 320 of this paper is false. A consequence of this is that the conditions obtained in §§11, 12, and which are stated to be necessary and sufficient, have only been shown to be sufficient. To obtain conditions which are both necessary and sufficient, we observe that, if { g n ( t )} denote a sequence of integrable functions, then, in order that fov every bounded f ( t ) we havelimn → ∞∫ 0 2 πf ( t ) g n ( t ) d t= 0, it is necessary and sufficient that (i) there is a constant K such that∫ 0 2 π| g n ( t ) | d t< K , and (ii), given a measurable set e in (0, 2π),limn → ∞∫ e g n ( t ) d t = 0 .This is an easy congruence of Lemma 2, p. 293. To obtain condition (2, 6), we must characterize the functions g ( t ) for which equation (33), p. 320, is true. We amend the definition of class ( b ) as follows. Amended definition of class ( b ). Let g ( t ) be an integrable periodic function. To each n , let there correspond a number v n of non‐overlapping intervals in (0, 2π), {(α i ( n ) ,β i ( n ))} ( i = 1, 2, …, v n ), such thatlimn → ∞∑ i = 1 v n( β i ( n ) ‐ α i ( n ) ) = 0 .Let g n ( t ) =∑ i = 1 v n{ g ( t ‐ β i ( n )) ‐ g ( t ‐ α i ( n ) ) } .If there is a constant K such that (2) holds, and if, given a measurable set e in (0, 2π), (3) holds, then g ( t ) is absolutely continuous in mean. The sequence { g r ( t )} of functions is uniformly absolutely continuous in mean, if, with the notationg n ( r ) ( t )=∑ i = 1 v n{ g r ( t ‐ β i ( n )) ‐ g r ( t ‐ α i ( n ) ) }we have∫ 0 2 π| g n ( r )( t ) | d t < K ;limn → ∞∫ eg n ( r ) ( t ) d t = 0 ,where K is an absolute constant, and, for a given e , the limit is uniform in r . The propositions enunciated in §11 become true with this amended definition. For §12, we must introduce an amended definition of R ‐integrability in mean. Amended definition of R‐integrability in mean . Let g ( t ) be an integrable periodic function. To each n let there correspond a number v n of non‐overlapping intervals (4) in (0, 2π) such thatlimn → ∞Max1 ⩽ i ⩽ v n( β i ( n ) ‐ α i ( n ) = 0Letγ i ( n ),δ i ( n )be arbitrarily chosen to satisfyα i ( n )⩽γ i ( n )<δ i ( n )⩽β i ( n ). Let g n ( t ) =∑ i = 1v n{ g ( t ‐ δ i ( n ) ) ‐ g ( t ‐ γ i ( n ) ) } ( β i ( n ) ‐ α i ( n ) ) .If there is a constant K such that (2) holds, and if, given a measurable set e in (0, 2π), (3) holds, then g ( t ) is R ‐integrable in mean. The sequence { g r ( t ) is uniformly R ‐integrable in mean, if, with the notationg n ( r ) ( t )=∑ i = 1v n{ g ( r ) ( t ‐ δ i ( n ) ) ‐ g ( r ) ( t ‐ γ i ( n ) ) } ( β i ( n ) ‐ α i ( n ) )the relations (5) hold, where K is an absolute constant, and, for a given e , the limit is uniform in r . With this amended definition Lemma 8 is true. This lemma gives us a form of the condition (2, 3). I am, however, unable to give an amended definition of a function of R ‐integrable variation in mean, and thus to give the condition (2, 3) by characterizing the function of which Σ,λ n sin nx / n is the Fourier series.

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