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Laine and Yang [12] considered the entire functions coefficients case and got the following.
Pollicott Ruelle resonances of ( mathbf {P}_j )'s are exactly the zeros of the entire functions ( zeta _j ( lambda ) )'s.
In addition, the growth of the entire functions of exponential type on the integer sequence is estimated.
Groza et al. [30] presented a Newton interpolating series for approximate solutions of the entire functions of multipoint boundary value problems for differential equations.
Since the eigenvalues coincide with the zeros of the entire functions (omega ( lambda )), it follows that they have no finite accumulation point.
If F z) and Δ c F share 1, ∞ CM, then F z) = Δ c F. For the entire functions case, using the same method as in the proof of Theorem 1.4, we get the following result.
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("It may have been the entire function of communes to go big, fail and then go home," says Brand, to take one example.
In contrast to real differentiable functions, which are as "flexible" as string, complex differentiable functions are "rigid" in the sense that any region of the function determines the entire function.
Here (omega(lambda)) is the entire function defined in (2.24).
Here ω is the entire function defined in (2.5).
Taking into account the entire function, we also get the boundedness of .
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