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Berlekamp essentially solved the problem for large values of the parameters.
As expected, the cost of PCD is high for large values of c, i.e. the PCD rate.
We observe that for large values of momentum, most variables (grey lines) follow the root μ convergence rate (red line).
However, for large values of N compared to Nt, "overcrowding" occurs and temporal synchronization is detrimental to firing frequency.
The asymptotical solution describing this front for large values of time is obtained.
These expressions show that η = 1ΦB2 for large values of ΦB.
The program provides a fast and exact calculation of the coefficients for large values of quantum angular momenta.
Integrals with a power-like divergence in N-space ∝aN,a∈R,a>1, for large values of N emerge.
for large values of,,, and.
For large values, the expression in (13) tends to 2.3.
Also, it is obvious that more coverage is acquired for large values of m.
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