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The objective in this step is to find an equation that will allow us to solve for the generating function A x).
We deduced its generating function, recurrence relations and q-difference equation, which gives us the differential equation of each of the Bessel function and the modified Bessel function when q tends to 1. Finally, the quantum algebra E 2 ( q ) and its representations presented an algebraic derivation for the generating function of the generalized q-Bessel function.
For, one now considers the Mellin transformation for the generating function of.
For, we now consider the Mellin transformation for the generating function of.
This approach allows for the generating a broad range of different output spectral distributions of almost arbitrary shape.
In this paper, we present linear differential equations for the generating functions of the Poisson-Charlier, actuarial, and Meixner polynomials.
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For instance, the generating capacity of renewable energy systems has surpassed coal power.
See Additional file 2 for the generated structures.
This was due to the increase in time for the generated anions to reach the sensor.
The sources at the teeth radiate incoherently as baffled dipoles and account for the generated noise.
Finally, we prove a Kummer-type congruence for the generated weighted q-Genocchi numbers.
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