### 抄録

This is a summarized version of the forthcoming paper [19]. Let m and n be any positive integers. We write e(x)=e^{2π}√-1, and use the vectorial notation x=(x_{1},...,x_{m}) for any complex x and x_{i}(i=1,...,m). The main object of this paper is the Shintani zeta-function φ̃_{n}(s,a,λ;z) defined by (1.4) below, where s_{j}(j=1,...,n) are complex variables, a_{i} and λ_{i}(i=1,2) real parameters with a_{i}>0, and z _{j} complex parameters with |argz_{j}|<π(j=1,...,n). We shall first present a complete asymptotic expansion of φ̃ _{n}(s,a,λ;z) in the ascending order of z_{n} as z _{n}→0 (Theorem 1), and that in the descending order of z _{n} as z_{n}→∞ (Theorem 2), both through the sectorial region |argz_{n}-θ_{0}|<π/2 for any angle θ_{0} with |θ_{0}|<π/2, while other z _{j}'s move within the same sector upon satisfying the conditions z _{j}≈z_{n}(j=1,...,n-1). It is significant that the Lauricella hypergeometric functions (defined by (2.1) below) appear in each term of the asymptotic series on the right sides of (2.7) and (2.10). Our main formulae (2.6) (with (2.7) and (2.8)) and (2.9) (with (2.10) and (2.11)) further yield several functional properties of φ̃_{n}(s,a,λ;z) (Corollaries 1-3).

元の言語 | English |
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ホスト出版物のタイトル | AIP Conference Proceedings |

ページ | 58-72 |

ページ数 | 15 |

巻 | 1385 |

DOI | |

出版物ステータス | Published - 2011 |

イベント | Diophantine Analysis and Related Fields 2011, DARF - 2011 - Musashino, Tokyo, Japan 継続期間: 2011 3 3 → 2011 3 5 |

### Other

Other | Diophantine Analysis and Related Fields 2011, DARF - 2011 |
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国 | Japan |

市 | Musashino, Tokyo |

期間 | 11/3/3 → 11/3/5 |

### Fingerprint

### ASJC Scopus subject areas

- Physics and Astronomy(all)

### これを引用

*AIP Conference Proceedings*(巻 1385, pp. 58-72) https://doi.org/10.1063/1.3630041

**Asymptotic expansions for double Shintani zeta-functions of several variables.** / Katsurada, Masanori.

研究成果: Conference contribution

*AIP Conference Proceedings.*巻. 1385, pp. 58-72, Diophantine Analysis and Related Fields 2011, DARF - 2011, Musashino, Tokyo, Japan, 11/3/3. https://doi.org/10.1063/1.3630041

}

TY - GEN

T1 - Asymptotic expansions for double Shintani zeta-functions of several variables

AU - Katsurada, Masanori

PY - 2011

Y1 - 2011

N2 - This is a summarized version of the forthcoming paper [19]. Let m and n be any positive integers. We write e(x)=e2π√-1, and use the vectorial notation x=(x1,...,xm) for any complex x and xi(i=1,...,m). The main object of this paper is the Shintani zeta-function φ̃n(s,a,λ;z) defined by (1.4) below, where sj(j=1,...,n) are complex variables, ai and λi(i=1,2) real parameters with ai>0, and z j complex parameters with |argzj|<π(j=1,...,n). We shall first present a complete asymptotic expansion of φ̃ n(s,a,λ;z) in the ascending order of zn as z n→0 (Theorem 1), and that in the descending order of z n as zn→∞ (Theorem 2), both through the sectorial region |argzn-θ0|<π/2 for any angle θ0 with |θ0|<π/2, while other z j's move within the same sector upon satisfying the conditions z j≈zn(j=1,...,n-1). It is significant that the Lauricella hypergeometric functions (defined by (2.1) below) appear in each term of the asymptotic series on the right sides of (2.7) and (2.10). Our main formulae (2.6) (with (2.7) and (2.8)) and (2.9) (with (2.10) and (2.11)) further yield several functional properties of φ̃n(s,a,λ;z) (Corollaries 1-3).

AB - This is a summarized version of the forthcoming paper [19]. Let m and n be any positive integers. We write e(x)=e2π√-1, and use the vectorial notation x=(x1,...,xm) for any complex x and xi(i=1,...,m). The main object of this paper is the Shintani zeta-function φ̃n(s,a,λ;z) defined by (1.4) below, where sj(j=1,...,n) are complex variables, ai and λi(i=1,2) real parameters with ai>0, and z j complex parameters with |argzj|<π(j=1,...,n). We shall first present a complete asymptotic expansion of φ̃ n(s,a,λ;z) in the ascending order of zn as z n→0 (Theorem 1), and that in the descending order of z n as zn→∞ (Theorem 2), both through the sectorial region |argzn-θ0|<π/2 for any angle θ0 with |θ0|<π/2, while other z j's move within the same sector upon satisfying the conditions z j≈zn(j=1,...,n-1). It is significant that the Lauricella hypergeometric functions (defined by (2.1) below) appear in each term of the asymptotic series on the right sides of (2.7) and (2.10). Our main formulae (2.6) (with (2.7) and (2.8)) and (2.9) (with (2.10) and (2.11)) further yield several functional properties of φ̃n(s,a,λ;z) (Corollaries 1-3).

KW - asymptotic expansion

KW - Mellin-Barnes integral

KW - Shintani zeta-function

UR - http://www.scopus.com/inward/record.url?scp=81755162353&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=81755162353&partnerID=8YFLogxK

U2 - 10.1063/1.3630041

DO - 10.1063/1.3630041

M3 - Conference contribution

AN - SCOPUS:81755162353

SN - 9780735409477

VL - 1385

SP - 58

EP - 72

BT - AIP Conference Proceedings

ER -