1964
DOI: 10.1137/0112049
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Remarks on the Zeros of Cross-Product Bessel Functions

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Cited by 28 publications
(22 citation statements)
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“…However, unlike the widely developed theory of zeros of Bessel functions , , and corresponding cylinder functions (see, e.g., the surveys [7,11,19] and references therein), significantly less inequalities and asymptotic results are known for zeros of , . Among known ones, the inequality of McCann [14, (10)] reads as , ≥ √︂ 2 0, + 2 2 , (1.1) and the following approximation of , for a fixed of McMahon [15, (24)] (see also [5,Theorem,p. 583]) states that…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…However, unlike the widely developed theory of zeros of Bessel functions , , and corresponding cylinder functions (see, e.g., the surveys [7,11,19] and references therein), significantly less inequalities and asymptotic results are known for zeros of , . Among known ones, the inequality of McCann [14, (10)] reads as , ≥ √︂ 2 0, + 2 2 , (1.1) and the following approximation of , for a fixed of McMahon [15, (24)] (see also [5,Theorem,p. 583]) states that…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Recalling that any zero of , is simple (see, e.g., [5]), the rate of change of = ( ) with respect to can be found from the total derivative Finally, recalling that ( ) = ( ) = 0, > 1, and that 2 ( ) + 2 ( ) decreases with respect to > 0 [19, p. 446], we have 2 ( ) 2 ( ) = 2 ( ) + 2 ( ) 2 ( ) + 2 ( ) > 1, and hence (1.3) follows. The proof of (1.3) in the case ( ) = ( ) = 0 can be handled in much the same way as above; see also [20].…”
Section: Pleijel's Constant For Annulimentioning
confidence: 99%
“…For given waveguide dimensions (a, Tt, r2), dielectric medium, and operating frequency, the admissible angular propagation constants (it is certainly inappropriate to talk in terms of linear propagation constants) appear as the zeros with respect to 11 of one or the other of the cross-product combinations of Bessel functions (6) or (7). It is known [Cochran, 1964] that for positive h both of these sets of 11-zeros are discrete and countably infinite, in general, and only a finite number of the zeros are real, the. remainder being pure imaginary.…”
Section: General Remarksmentioning
confidence: 99%
“…The paper is organised as follows. In Section 2 we present a detailed study of the mode structure in the bend, which is closely related to the work of Cochran [15,16,17]. In comparison to the work of others, ours is directed more towards the application of the mode structure to scattering calculations.…”
Section: Introductionmentioning
confidence: 98%