Functional equations with solutions of irregular singular type (Algebraic analytic methods in complex partial differential equations)
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(2) 87. Definition 0,1, Let s\geq 0. A formal power series f(z)=\displaystyle \sum_{m=0}^{\infty}f_{n}z^{n} is said to be of Gevrey order s if there exist constants A,C\geq 0 such that ,. |h|\leq A\mathrm{C}^{n} $\Gamma$(sn+1) for. \mathbb{C}_{\{\mathrm{s}\} [ z]. :. the. (0.4). n\in \mathbb{Z}+\cdot. totality ofallformal power series of Gevrey order s.. If s=0, f(z) converges and is holomorphic at following existence Theorems in \mathbb{C}[ z] Let. z=. O. We have the. .. \displaystyle \mathscr{A}(z)=\sum_{i=1}^{m}a_{i}(z). Suppose a_{i}(z)\in \mathbb{C}[[z]](1\leq i\leq m) \mathbb{C}[[z]] and one of thefollowing (1) -(2) holds. Theorem 0.2.. (1). \mathscr{A}(0)\neq 0.. (2). \mathscr{A}(0)=\cdots=\mathscr{A}^{(p-1)}(0)=0,. (0.5). .. and. f(z)=$\Sigma$_{n=0}^{\infty}hz^{n}\in. \displaystyle \sum_{=1}^{m}a_{i}(0)b_{i,p}\neq 0,. \displaystyle \frac{\mathscr{A}^{(p)}(0)}{p!}+n$\Sigma$_{i=1}^{m}a_{i}(0)b_{i,p}\neq 0 for n\in \mathbb{Z}+. and. f_{0}=f_{1}=\cdots=f_{p-1}=0.. Then there exists. a. unique formal. solution. if ai(z)\in \mathbb{C}[[z]]_{\{1/p\}}(1\leq i\leq m). and. \mathbb{C}[[z]]_{\{1/p\}}.. Theorem 0.3. \mathbb{C}[ z] Further .. u(z)\in \mathbb{C}[[z]] of (0.2). Moreover, f(z)\in \mathbb{C}[[z]]_{\{11p\}/} then u(z)\in. Suppose a_{i}(z)\in \mathbb{C}[[z]](1\leq i\leq m). and. f(z)=$\Sigma$_{n=0}^{\infty}f_{n}z^{n}\in. assume. \mathscr{A}(0)=\cdots=\mathscr{A}^{(p)}(0)=0,. \displaystyle \sum_{i=1}^{m}a_{i}(0)b_{i,p}\neq 0 and f_{0}=f_{1}=\cdots=f_{p}=0. .. Thenforgiven c_{0} there exists a uniqueformal solu‐ u(0)=c_{0} Moreover, if a_{i}(z)\in \mathbb{C}[[z]]_{\{1/p\}}(1\leq. u(z)\in \mathbb{C}[[z]] of(0.2) i\leq m) and f(z)\in \mathbb{C}[[z]]_{\{1/p\}}. tion. From Theorem 0.3 in. \mathbb{C}[[z]].. with. we. .. ,. then. u(z)\in \mathbb{C}[[z]]_{\{1/p\}}.. get existence non trivial homogeneous solutions.
(3) 88. Corollary 0.4. Suppose a_{i}(z)\in \mathbb{C}[[z]](1\leq i\leq m). ,. \mathscr{A}(0)=\cdots=\mathscr{A}^{(p)}(0)=0 and. \displaystyle \sum_{i=1}^{m}a_{i}(0)b_{i,p}\neq 0. Then there exists over,. u(z)\in \mathbb{C}[[z]]. ,. then. Theorem 0.5.. $\Sigma$_{i=1}^{m}a_{i}(0)b_{i,p}e^{-pb_{i,p}$\zeta$_{0} \neq 0. .. thefOrm. $\zeta$_{0} such. that. and. C_{p}=$\zeta$_{0}. w(z)\in \mathrm{C}[[z]]. \mathbb{C}[[z]]_{\{1/p\}}(1\leq i\leq m). ,. .. We ob‐. $\Sigma$_{i=1}^{m}a_{j}(0)e^{-pb_{i,p}$\zeta$_{0}}=0. Then there exists a formal solution. u(z)=\displaystyle \exp(\frac{C_{p} {z\mathrm{P} +\frac{C_{p-1} {z^{p-1} +\cdots+\frac{C_{1} {z})z^{ $\alpha$}w(z) where. More‐. exponential factor.. that there exists. Suppose. .. u(z)\in \mathbb{C}[[z]]_{\{1/p\}}.. try to find homogeneous solutions wider class than \mathbb{C}[ z]. tain formal solutions with. 0 in. u(0)=1 satisfying L(z,u(z))=0. if a_{i}(z)\in \mathbb{C}[[z]]_{\{1/p\}}(1\leq i\leq m). We. with. with. then. with. w(0)=1. .. of L(z,u(z))=. Moreover,. w(z)\in \mathbb{C}[[z]]_{\{1/p\}}.. (0.6). ,. if a_{i}(z)\in. previous part we find formal solutions. The next aim is to give analytical meanings to them. We define S( $\theta,\ \delta$,r)=\{z, |\arg z- $\theta$|< In the. $\delta$,. |z|<r\} which is a sector in z ‐space.. Definition 0.6. We say that \overline{w}(z)=$\Sigma$_{n=0}^{\infty}c_{n}\mathrm{z}^{n}\in \mathbb{C}[ z] is $\gamma$‐Borel summable in a direction $\theta$ if there exists a holomorphicfunction w(z) on S( $\theta,\ \delta$,r) $\delta$> ,. $\pi$/(2 $\gamma$). ,. ,. such that. |w(z)-\displaystyle \sum_{n=0}^{N-1}c_{n}z^{n}|\leq AC^{N} $\Gamma$(\frac{N}{ $\gamma$}+1)|z^{N} holdsfor all N\in \mathbb{Z}+\cdot. We denote. (0.7) by. (0.7). w(z)\sim $\gamma \Sigma$_{n=0}^{\infty}c_{n}z^{n}.. $\delta$> $\pi$/(2 $\gamma$) w(z) is umquely deter‐ \overline{w}(z) may identify \overline{w}(z) with w(z) As for the Borel summability (multi‐summability) of functions we refer to [1] and [2]. We have. mined for. \overline{w}(z)\in \mathbb{C}[ z] _{\{1/ $\gamma$\}}. .. Hence. we. Since. ,. ..
(4) 89. give a condition to study the relation between formal solutions and genuine solutions. Let b_{1,p}=0 and B=\{b_{i,p};1\leq i\leq m\} which is a finite We. set in \mathbb{C}.. Let. us. remember. Theorem 0.7.. (I) (2). Suppose. and. that Condition B and. f(z)=$\Sigma$_{m=0}^{\infty}f_{n}z^{n}.. one. of the following (1)-(3) hold.. \mathscr{A}(0)\neq 0.. \mathscr{A}(0)=\cdots=\mathscr{A}^{(p)}(0)=0,. and. (3). \mathscr{A}(z)=$\Sigma$_{i=1}^{m}a_{i}(z). $\Sigma$_{i=1}^{m}a_{i}(0)b_{i,p}\neq 0. f_{0}=f_{1}=\cdots=f_{p}=0.. of(O) =\cdots=\mathscr{A}^{(p-1)}(0)=0,. $\Sigma$_{i=1}^{m}a_{i}(0)b_{i,p}\neq 0,. \displaystyle \frac{\mathscr{A}^{(p)}(0)}{p!}+n($\Sigma$_{i=1}^{m}a_{i}(0)b_{i,p})\neq 0 for n\in \mathbb{Z}+. and. f_{0}=f_{1}=\cdots=f_{p-1}=0.. Then there exists. (0.2). f(z). direction $\theta$_{0} such that the formal solution u(z)\in \mathbb{C}[[z]] of is p ‐Borel summable in the direction $\theta$_{0/} provided a_{i}(z)(1\leq i\leq m) and are p ‐Borel summable in the direction $\theta$_{0}.. As for. a. homogeneous formal solutions in Theorem 0.5 we have. Theorem 0.8. such that. Suppose that Condition B holds. Then there exists a direction $\theta$_{0} if a_{i}(z) is p ‐Borel summable in the direction $\theta$_{0}, w(z)\in \mathbb{C}[[z]] of(0.6). in Theorem 0.5 is also p ‐Borel summable in the direction. The direction $\theta$_{0} is determined. by the location of zeros of. h( $\zeta$)=\displaystyle \sum_{i=1}^{m}a_{i}(0)e^{pb_{i,p}$\zeta$^{p} We. sum. $\theta$_{0}.. up the obtained results..
(5) 90. It follows from Theorems 0.2, 0.3 and 0.7 that there exist solutions of Gevrey order.. (1). formal power series with. Theorem 0.5 is the existence of formal solutions of the. (2). homogeneous equation, which are represented with exponential factors.. These facts. equations. are. of solutions to. [3]. and. similar to the properties of solutions of ordinary differential. with. irregular singular point at z=0 As for the properties of irregular singular ordinary differential equations we refer. [5]. an. .. and papers cited there.. Finally we give cretely. Example.. a. simple example to. understand the results. more con‐. \left{\begin{ar y}{l u(z)+ /(1-z)=\frac{z}2-\ u(z)=\int_{0}^e{i$\thea$}\infty}\rac{e-$\psilon$_{+}\zeta$}{2(1+e^{$\zeta$})d\zeta$ \end{ar y}\ight.. û. ($\zeta$)=\displaystyle\frac{\exp(\frac{$\zeta$}{2}){2(1+\exp$\zeta$)}=\sum_{n=0}^{\infty}c_{n}$\zeta$^{n}. (| $\zeta$|< $\pi$). u(z)\displaystyle \sim\sum_{n=1}^{\infty}c_{n-1} $\Gamma$(n)z^{n}1 |\arg z|< $\pi$- $\epsilon$ \displaystyle \{\exp\frac{(2n+1) $\pi$ i}{\mathrm{z} ;n\in \mathbb{Z}\}. are. homogeneous solutions.. References Balser, From Divergent Power Series to Analytic Functions, vol.1582, Lecture Notes in Math., Springer, 1994.. [1]. W.. [2]. W.. [3]. W.. Balser, Formal power series and linear systems of meromorphic ordinary differential equations, Universitext, Springer, 1999. Balser, B.L.J. Braaksma, J.‐P Ramis and Y. Sibuya, Multisumma‐. bilty. of formal power series solutions of linear. equations, Asymptotic Analysis,. 5. (1991), 27‐45.. ordinary. differential.
(6) 91. [4] S. Ouchi. On tions.. [5]. some. functional. Funkcialaj Ekvacioj. 58. equation with (2015), 223‐251.. Borel summable solu‐. W. Wasow, Asymptotic Expansions of Ordinary Differential tions, Dover Publications, New York, 1987.. Equa‐.
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