2012
DOI: 10.1134/s001226611206002x
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On the best constants in the solvability conditions for the periodic boundary value problem for higher-order functional differential equations

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Cited by 3 publications
(7 citation statements)
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“…From Lemma 3 it follows that a non-constant component x j (from the proof of Lemma 3) of the solution x to (5) is a solution to (16) with p = p j , some constant C, some measurable function τ : [0, T ] → [0, T ]. If (17), it follows from Lemma 4 that the solution x j is unique: x j (t) ≡ −C. From ( 14) it follows that each component x i of the non-constant solution x is constant.…”
Section: Resultsmentioning
confidence: 98%
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“…From Lemma 3 it follows that a non-constant component x j (from the proof of Lemma 3) of the solution x to (5) is a solution to (16) with p = p j , some constant C, some measurable function τ : [0, T ] → [0, T ]. If (17), it follows from Lemma 4 that the solution x j is unique: x j (t) ≡ −C. From ( 14) it follows that each component x i of the non-constant solution x is constant.…”
Section: Resultsmentioning
confidence: 98%
“…Let a positive number P be given. Problem For n = 1, n = 2, n = 3, n = 4 this Lemma is proved in [19,20,21,22], for arbitrary n in [23,24,17].…”
Section: Resultsmentioning
confidence: 99%
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“…Other interesting results about problems (6), (4) can be found also in the papers [10][11][12][13][14][15].…”
Section: Definition 12mentioning
confidence: 90%
“…For the case i ≡ 0 (i = 1, n -1), these results are generalized in [9]. It is interesting that the numbers N n are in some connection with Favard's, Bernoulli's, and Euler's numbers (see [10] and [11]) and if the operator 0 is monotone, then condition (8) transforms to the condition 0 < b…”
Section: Definition 12mentioning
confidence: 91%