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Theorem for the Identity of the $G_{1}(c, n)$ and $L_{1}(c, n)$ Numbers and Its Application to the Theory of Waveguides

机译: $ G_ {1}(c,n)$ $ L_ {1}(c, n)$ 数的恒等式定理及其对波导原理

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It is proved numerically that for the same restricted positive integers c and natural numbers n the real positive numbers G1(c, n) and L1(c, n), connected with certain kinds of zeros of the complex Kummer confluent hypergeometric function Φ(a, c;x) of a specially selected complex first parameter a, second parameter c-acquiring values, as pointed out above and a positive purely imaginary variable x, coincide, provided n designates the number of the zeros mentioned. This statement is advanced as a Theorem for the identity of the G1(c, n) and L1(c, n) numbers. The physical interpretation of the truthfulness of the result established made, reflects the possibility to substantiate in two different ways the existence of specific envelope curves in (to compute by means of two algorithms) the phase diagrams of the azimuthally magnetized circular ferrite waveguide for normal TE0n modes in case of negative magnetization which bound the wave propagation from the side of higher frequencies.
机译:数值证明,对于相同的限制正整数c和自然数n,实数G 1 (c,n)和L 1 (c,n),与特定选择的复杂第一参数a,第二参数c获取值(如上所述)和正数的复数Kummer汇合超几何函数Φ(a,c; x)的某些种类的零相关如果n表示所提到的零的数量,则纯虚变量x是一致的。该陈述作为G恒等式的一个定理而提出 1 (c,n)和L 1 (c,n)个数字。对所建立结果的真实性的物理解释,反映了以两种不同方式证实正常TE的方位磁化圆形铁氧体波导相图中(通过两种算法进行计算)特定包络曲线的存在的可能性。 0n 在负磁化的情况下,这些模式限制了波从较高频率侧的传播。

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