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for arbitrary values of l=0,1,2,….
The obtained solutions are applicable for arbitrary values of time.
The solutions are applicable for arbitrary values of time.
For arbitrary values of the exponential parameter, the equations are solved numerically.
The bound state energy eigenvalues for these potentials and for arbitrary values of n and l quantum numbers are presented.
The solution is evaluated for arbitrary values of r but restricted to the case of low frequencies.
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Moreover, this is true for arbitrary value of g > 0. The interesting implication here is that, unlike system where sustained oscillation is only attainable for certain n1 (n1 must be greater than 4), the inclusion of g, even small, has enabled the system to attain oscillation at any n1.
We see that for the arbitrary values of E ( t ) and F ( t ), infinitely many nonlocal conservation laws exist for the system (1a) and (1b).
This test bed has been designed to monitor the errors in the WiMAX channel for any arbitrary values of SNR and SIR. The test bed has the advantage of employing a realtime spectrum analyzer as a programmable WiMAX receiver.
Since B ≥ 8 for any arbitrary values of kd1, kd2 and kd3, the interval (0,8] becomes the "global" RGS of n1, i.e. with respect to all model parameters.
Analytical and numerical results are given for polarization curves for electrochemical cells with arbitrary values of transfer coefficient α and exchange current density.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com