“…The graphs in Fig. 1 complements those in [24, p. 510] where ±j νk is graphed against ν for k = 1, 2, 3, 4, and in [7] where j νκ is graphed against ν for various values of κ between 0 and 1. It is also worth mentioning that Olver [20] considered what amounts to j νκ for continuous κ while in [21], he considered it for continuous ν, both situations arising from a need to evaluate the zeros numerically.…”
We reexamine and continue the work of J. Vosmansky [J. Vosmanský, Zeros of solutions of linear differential equations as continuous functions of the parameter k, in: the concept of continuous ranking of zeros of certain special functions from the point of view of the transformation theory of second-order linear differential equations. This leads to results on higher monotonicity of such zeros with respect to the rank and to the evaluation of some definite integrals. The applications are to Airy, Bessel and Hermite functions.
“…The graphs in Fig. 1 complements those in [24, p. 510] where ±j νk is graphed against ν for k = 1, 2, 3, 4, and in [7] where j νκ is graphed against ν for various values of κ between 0 and 1. It is also worth mentioning that Olver [20] considered what amounts to j νκ for continuous κ while in [21], he considered it for continuous ν, both situations arising from a need to evaluate the zeros numerically.…”
We reexamine and continue the work of J. Vosmansky [J. Vosmanský, Zeros of solutions of linear differential equations as continuous functions of the parameter k, in: the concept of continuous ranking of zeros of certain special functions from the point of view of the transformation theory of second-order linear differential equations. This leads to results on higher monotonicity of such zeros with respect to the rank and to the evaluation of some definite integrals. The applications are to Airy, Bessel and Hermite functions.
“…or, in terms of our present notation, Now the first term on the right here is negative [1] and the sum of the two remaining terms will certainly be negative provided that (3.9) from (3.4) and (3.6) and this is certainly negative in case -0.8 < v < 0. Thus the second derivative of p 2 with respect to v is negative at points where the first derivative is 0; hence there can be only one such point and it is a relative maximum.…”
We show, among other things, that, for n = 0,1, the negative of the square of a purely imaginary zero of is unimodal on (n — 2, n — 1). One of the important tools in the proof is the Mittag-Leffler partial fractions expansion of .
“…we have g (ν) = dy ν1 /dν − π/4 which, in view of results in [4] decreases to the positive number 1−π/4, as ν → ∞. Thus g(ν) is increasing, g(− Watson [15, pp.…”
Abstract. In the course of their work on Salem numbers and uniform distribution modulo 1, A. Akiyama and Y. Tanigawa proved some inequalities concerning the values of the Bessel function J 0 at multiples of π, i.e., at the zeros of J 1/2 . This raises the question of inequalities and monotonicity properties for the sequences of values of one cylinder function at the zeros of another such function. Here we derive such results by differential equations methods.
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