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On entire solutions to eikonal-type equations

Journal of Mathematical Analysis and Applications, 2022
Abstract This paper characterizes equivalence conditions on entire solutions to eikonal-type nonlinear partial differential equations u z 1 2 + u z 2 2 = p ( z 1 , z 2 ) e g ( z 1 , z 2 ) in C 2 with two polynomials g ( z 1 , z 2
Wei Chen, Qi Han
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Properties of entire solutions of differential equations [PDF]

open access: possibleUkrainian Mathematical Journal, 2006
We investigate the close-to-convexity and l-index boundedness of entire solutions of the differential equations z 2 w″ + βzw′ + (γz 2 − β)w = 0 and zw″ + βw′ + γzw = 0.
Z. M. Sheremeta, M. M. Sheremeta
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Entire solutions of eiconal type equations [PDF]

open access: possibleArchiv der Mathematik, 2007
The paper characterizes entire solutions to partial differential equations $$u_{z_{1}}^{2} + u_{z_{2}}^{2} = p$$ for polynomials p in $${\mathbb{C}}^2$$ .
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Entire solutions of quasilinear elliptic equations

Nonlinear Analysis: Theory, Methods & Applications, 2007
Abstract We consider the existence of entire solutions of a quasilinear elliptic equation div ( | D u | p − 2 D u ) = k ( x ) f ( u ) , x ∈ R N , where p > 1 , N ∈ N . Conditions of the existence of entire solutions have been obtained by different authors. We prove an optimality of
Nickolai Slepchenkov, Alexander Gladkov
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ON EXPLICIT RADIAL ENTIRE AND NON-ENTIRE SOLUTIONS

Progress in Analysis, 2003
Vinod B. Goyal, Philip W. Schaefer
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Entire solution of the degenerate Fisher equation

Acta Mathematicae Applicatae Sinica, English Series, 2017
This paper deals with the solutions defined for all time of the degenerate Fisher equation. Some solutions are obtained by considering two traveling fronts with critical speed that come from both sides of the X-axis and mix. Unfortunately, the entire solutions which behave as two opposite wave fronts with non-critical speed approaching each other from ...
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A Note on Entire Solutions of the Eiconal Equation

The American Mathematical Monthly, 1995
A1< 2| [u2(sin2s-COS2S)2uusinscoss-u2sin2s+1]ds. (S) The product 2uu is the derivative of u2; integrating by parts changes (5) into 1 v A1< 21 (1-u2sin2s)ds, clearly < Fr/2. Equality holds only if u O, which makes y(s) constant sin s. Since equality in (3) holds only if y = x = 21 _ y2, y(5) _ sin s, x(s) + cos s + constant. This is a semicircle. Q.e.d.
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