162 $\cdots$ 2, 3, 5, 7, 11, 13, ( deterministic ) $\mathbb{r}$ ( -1 3 ) ( ) $\text{ }$ ( ). straightforward ( ) $p$ version ( ) - 2 $\mathrm{n}$ $\om
|
|
- あゆみ あきます
- 5 years ago
- Views:
Transcription
1 $L$ (Hirofumi Nagoshi) Research Institute for Mathematical Sciences, Kyoto Univ. 1. $L$ ( ) 2. ( 0 1 ) $X_{1},$ $X_{2},$ $X_{3},$ $\cdots$ $n^{-1/2}(x_{1}+$ $X_{2}+\cdots+X_{n})$ $X_{i}$ ( ) ( ) Probabilisitic number theory ( deterministic )
2 162 $\cdots$ 2, 3, 5, 7, 11, 13, ( deterministic ) $\mathbb{r}$ ( -1 3 ) ( ) $\text{ }$ ( ). straightforward ( ) $p$ version ( ) - 2 $\mathrm{n}$ $\omega(n)$ $n$ $p$ $\omega(n)$ $n$ 1 Erd\"os Kac [EK1][EK2] $\omega(n)$
3 $\mathrm{l}$ 163 ( $\mathrm{c}\mathrm{a}\mathrm{n}$ Kac one hear the $\mathrm{d}\mathrm{r}\mathrm{u}\mathrm{m}?\rfloor$ shape of a Feynman-Kac ) Kac Theorem 2.1. $x_{1},$ $x_{2}\in \mathbb{r}(x_{1}<x_{2})$ L $\lim_{narrow\infty}\frac{1}{n}\neq\{1\leq n\leq N x_{1}<\frac{\omega(n)-1\mathrm{o}\mathrm{g}1\mathrm{o}\mathrm{g}n}{\sqrt{1\mathrm{o}\mathrm{g}1\mathrm{o}\mathrm{g}n}}<x_{2}\}=\frac{1}{\sqrt{2\pi}}\int_{x_{1}}^{x_{2}}e^{-\frac{x^{2}}{2}}dx$ 2 ${\rm Re}(s)=1/2$ Selberg [S3] [S1] Theorem 2.2. $\mathbb{c}$ $E$ $\lim_{tarrow\infty}\frac{1}{t}m(\{t\in[0, T]$ $\frac{1\mathrm{o}\mathrm{g}\zeta(\frac{\mathrm{l}}{2}+it)}{\sqrt{\frac{1}{2}1\mathrm{o}\mathrm{g}\log t}}\in E\})=\frac{1}{2\pi}\int\int_{E}e^{-\frac{x^{2}+}{2}u_{-}^{2}}$ dxdy $\mathrm{r}$ $m$ $\log\zeta(s)$ ( ${\rm Re}(s)arrow\infty$ 0[ Selberg class [S3] [BH] [BH] 3. Selberg $L$ ( ) $\{s\in \mathbb{c} 0\leq{\rm Re}(s)\leq 1\}$ ( ${\rm Re}(s)=0,1$ ) : 1 2
4 Goldbach $\pi(x)\sim x/\log x$ ${\rm Re}(s)=1$ $\zeta(s)\neq 0$ on ${\rm Re}(s)=1$ Hadamard de la Valli Poussin I Eisenstein ${\rm Re}(s)=1$ $\zeta(s)\neq 0$ 3 2 Selberg Erdi Sieve (Elementary method) - Hardy-Littlewood prime -tuple conjecture. $n$ $p_{n+1}-p_{n}$ ( $p_{n}$ $n$ ) $\text{ }x_{n}:=p_{n}/\log p_{n}$ $x_{n+1}-x_{n}$ ( ) $\text{ }$ ( Sieve Method, Elementary Method) 2 (see [La]) Theorem 3.1. $D=\{s\in \mathbb{c} 1/2<{\rm Re}(s)<1\}$ $K$ $K$ $K$ $h(s)$ $\epsilon>0$ $t\in \mathrm{r}$ [ $\sup_{s\in K} \zeta(s+it)-h(s) <\epsilon$ $\lim_{tarrow}\inf_{\infty}\frac{1}{t}m(t\in[0,t] \sup_{s\in K} \zeta(s+it)-h(s) <\epsilon)>0$
5 $\psi\mathrm{a}$ 165 $D$ - $\log p$ $\mathbb{q}$ ( ) 1, 2 $\mathrm{v}$ $\sum_{n}n^{-s}$ ${\rm Re}(s)>1$ ( ) $0<{\rm Re}(s)<1$ Sieve 4. $f\mathrm{j}$ Wigner ( 1 ) (see e.g. $)$ [M] ( GUE(Gaussian Unitary Ensemble) J $\mathcal{h}_{n}$ $N\cross N$ -Hermite Gauss $P_{N}(dX)\propto$ $\exp(-\mathrm{r}(x^{2}))dx$ $(\mathcal{h}_{n}, P_{N})$ GUE. $Narrow\infty$ Montgomery (1973)
6 166 2 $\rho_{i}$ $\gamma_{i}$ Dyson GUE Odlyzko (1987) $n$ [KS] [C] survey GUE GUE GUE Dyson CUE(Circular Unitary Ensemble) $N\cross N$- $U(N)$ Haar $Q_{N}$ $(U(N), Q_{N})$ scaled limit $Narrow\infty$ $M_{k}(T)= \int_{0}^{t} \zeta(1/2+it) ^{2k}dt$ ) CUE $Z(U, \theta)=\det(i-ue^{-i\theta}),$ $U\in U(N)$ $k=1,2$ $\lim_{narrow\infty}n^{-k^{2}}q_{n}( Z(U, \theta) ^{2k})$ $k$ $M_{k}(T)$ ${\rm Re}(s)=1/2$ Keating-Snaith(2000) Theorem 4.1. $\mathbb{c}$ $E$ $\lim_{narrow\infty}q_{n}(u\in U(N)$ $\frac{1\mathrm{o}\mathrm{g}z(u,\theta)}{\sqrt{\frac{1}{2}1\mathrm{o}\mathrm{g}n}}\in E)=\frac{1}{2\pi}\int\int_{E}e^{-_{2}^{\underline{x^{2}}+x_{-}^{2}}}dxdy$ ( $\theta$ ) Selberg Theorem 2.2 \cdot$ }$\backslash 5.
7 $\text{ }-$ $\mathbb{c}$ 167 Theorem 22 ( ( $t(={\rm Im}(s))$ $L$ $t$ $\chi \mathrm{m}\mathrm{o}\mathrm{d} q$ $L$ $L(s, \chi)$ ( $q$ $t$ $q$ [S2] $t$ $L$ $N$ $k$ [ILS] 3 $L$ [N1] $t$ $t$ Theorem 22 $L$ $N$ $\mathcal{f}_{n}$ $\Gamma_{0}(N)(\subset SL(2, \mathbb{z}))$ 2 Hecke eigen cusp forms $N$ $f\in \mathcal{f}_{n}$ Hecke $\lambda_{f}(n)$ $T_{n}(N)$ $n$ Hecke $T_{n} (N)f=\lambda f(n)f$, where $T_{n} (N):=T_{n}(N)/n^{\frac{1}{2}}$ $L$ $(s, f):= \sum_{n=1}^{\infty}\frac{\lambda_{f}(n)}{n^{s}}=\prod_{p N}(1-\frac{\lambda_{f}(p)}{p^{s}})^{-1}$ $(1- \frac{\lambda_{f}(p)}{p^{s}}+\frac{1}{p^{2s}})^{-1}$ for ${\rm Re}(s)>1$ Hecke ${\rm Re}(s)=1/2$ $N$ $N$ Theorem 5.1. $t\neq 0$ $\mathrm{r}$ $E$ $\lim_{narrow\infty}\frac{1}{\# F_{N}}\#\{f\in F_{N}$ $\frac{{\rm Im}\log L(\frac{1}{2}+it,f)}{\sqrt{\frac{1}{2}\log 1\mathrm{o}\mathrm{g}N}}\in E\}=\frac{1}{\sqrt{2\pi}}\int_{E}e^{-\frac{x^{2}}{2}}dx$.
8 168 $N$ Hecke eigen cusp forms $f\in \mathcal{f}_{n}$ $Narrow\infty$ $f$ $\mathrm{r}$ ) 6. [N2] Moment method Theorem 6.1. $m\in- \mathrm{n}$ $t\neq 0$ $\sum_{f\in F_{N}}({\rm Im}\log L(\frac{1}{2}+it,$ $f))^{m}$ $=C_{m} \#\mathcal{f}_{n}(\frac{1}{2}\log\log N)^{\frac{m}{2}}+O_{m,t}(N(\log\log N)^{\frac{m-1}{2}})$. $C_{m}=\{\begin{array}{l}m!!2T,ifmiseven0,ifmisodd\end{array}$ $C_{m}$ Theorem Selberg [S1] explicit formula Lemma 6.2. ${\rm Re} s\geq 1/2_{\text{ }}x\geq 10$ $\frac{l }{L}(s, f)=-\sum_{n\leq x^{3}}\frac{\lambda_{x}(n)c_{f}(n)}{n^{s}}+\frac{1}{\log^{2}x}\sum_{\rho}\frac{x^{\rho-s}(1-x^{\rho-s})^{2}}{(s-\sqrt)^{3}}$ (6.1) $- \frac{1}{\log^{2}x}\sum_{l=0}^{\infty}\frac{x^{-\frac{1}{2}-\ell-s}(1-x^{-\frac{1}{2}-\ell-s})^{2}}{(s+\frac{1}{2}+\ell)^{3}}$.
9 169 $\rho$ $\ovalbox{\tt\small REJECT}(n)$ ( $L(s, f)$ $\ovalbox{\tt\small REJECT}_{x}(n)$ ( von Mangolt where $\ovalbox{\tt\small REJECT}_{x}(n)\ovalbox{\tt\small REJECT}_{\ovalbox{\tt\small REJECT}}\ovalbox{\tt\small REJECT}(n)w_{x}(n)$ $w_{x}(n):=-\{_{0}^{1}\{$ $, \frac{1}{2}\log 2\frac{x^{3}}{n}-\log^{2}\frac{x^{2}}{n})/\log^{2}x$ for $1\leq n\leq x$,, for $x<n\leq x^{2}$, $\frac{1}{2}\log 2\frac{x^{3}}{n})/\log^{2}x$, for $x^{2}<n\leq x^{3}$, for $x^{3}<n$. (6.1) $\sum_{\rho}$ ( $\sum_{\ell}$ ) (by Kowalski-Michel1999) Lemma 6.3. $N$ $A>0$ : $t_{1},$ $t_{2}$ with $t_{1}<t_{2}$, $t_{2}-t_{1} \geq\frac{1}{\log q}$ $\alpha\geq 1/2+(\log N)^{-1}$ $c$ with $0<c<1/4$ ( $\sum_{f\in F_{N}}N_{f}(\alpha, t_{1}, t_{2})<<_{c}(1+ t_{1} + t_{2} )^{A}N^{1-c(\alpha-\frac{1}{2})_{(\log N)(t_{2}-t_{1})}}$ $\vee\supset_{\text{ }}$ $arrow>$. $N_{f}(\alpha, t_{1}, t_{2})l\mathrm{h}_{\text{ }}L(s, f)$ $\rho=\beta+i\gamma$ $\beta\leq\alpha$, $t_{1}\leq\gamma\leq t_{2}$. ( $\not\in-$ ) (6.1) Lemma 6.4. $N$ $(n, N)=1$ $\mathrm{t}\mathrm{r}t_{n} (N)=\frac{(N+1)}{12}n^{-1/2}\delta_{n=\square }+O(n^{c}N^{1/2})$. $c>0$ $\delta_{n=\square }$ $n$ 1 $n$ 0 ${\rm Im} \sum_{p\leq N^{\delta}\infty}p^{12+it}\lambda_{f}(p)$ $\delta$ ) Theorem 5.1, Theorem 6.1 $\log\log N$ $\sum_{p\leq x}1/p=\log\log x+o(1)$
10 :Limit \mathrm{f}\mathrm{u}\mathrm{n}\overline{\mathrm{c}}$ tions $\mathrm{v}^{\mathrm{a}}$ $\mathrm{v}$ rx- deterministic [ $\nearrow^{\text{ }}$ [ 1933 (Kolmogorov ) ( ) SatO-Tate SatO-Tate ( symmetric power L-functions ) $\mathrm{v}^{\mathrm{a}}$ REFERENCES products, Duke Math. J. 80 (1995), $L- [C] J. B. Conrey: and random matrices, in Mathematioe unlimited-2001 and beyond Springer-Verlag, 2001, $\mathrm{i},$ [E] P. D. T. A. Elliott: Probabilistic number theory, $\mathrm{i}\mathrm{i}$, Springer-Verlag, 1979, [EK1] P. Erdi, M. Kac: On the Gaussia law of errors in the theory of additive functions, $20\triangleright Proc. Nat. Acad. Sci. USA. 25 (1939), 207$. [EK2] P. Erd\"os, M. Kac: The Gaussia law of errors in the theory of additive numbertheoretic functions, Amer. J. Math. 62 (1940), [ILS] H. Iwaniec, W. Luo, P. Sarnak: Low lying zeros of families of Afunctions, IHES 91 (2001), [K] M. Kac: Statistical independence in probability, analysis and number theory, Carus Monograph No. 12, [KS] N. M. Katz, P. Sarnak: Zeros of zeta functions and symmetry, Bull. Amer. Math. Soc. 36 (1999), [Ku] J. Kubilius: Probabilistic methods in the theory of numbers, AMS, $\mathrm{l}\mathrm{a}\mathrm{u}\mathrm{r}\mathrm{i}\mathrm{n}\check{\mathrm{c}}\mathrm{i}\mathrm{f}\mathrm{f}\mathrm{i}$ [La] A. Theorems for the Riemann Zeta-Function, Kluwer, [Li] U. V. Linnik: Ergodic properties of algebraic fields, Springer-Verlag, [M] M. L. Mehta: Random matrices, Academic Press, [N1] H. Nagoshi: The universality of families of automorphic&functions, preprint. distribution and afamily of automorphic preprint. [N2] H. Nagoshi: Gaussian- $\mathrm{l}$-functions,
11 Sinai: 48 \mathrm{r}\mathrm{y},$ Princeton. 171 [S1] A. Selberg: Contributions to the theory of the Riemann zeta-function, Arch$\cdot$ Math. $\cdot$ Naturvid (1946), ; Collected Papers, Springer-Verlag. $\mathrm{v}\mathrm{o}\mathrm{l}1, ,$ $\mathrm{s}\mathrm{k}\mathrm{r}$ [S2] A. Selberg: Contributions to the theory of Dirichlet s L-function, Norske Vid. Akad. Oslo (1946), 1-62: Collected Papers, Springer-Verlag. $\mathrm{v}\mathrm{o}\mathrm{l}1, ,$ [S3] A. Selberg: Old and new conjectures and results about a class of Dirichlet series, Proceedings $\mathrm{t}\mathrm{h}\infty of the Amalfi Conference on Analytic Number \mathrm{r}\mathrm{y}(1992)$, ; Collected Papers, Springer-Verlag. $\mathrm{v}\mathrm{o}\mathrm{l}2,47-63,$ $\mathrm{g}\cdot$ $\mathrm{e}\mathrm{r}\mathrm{g}6\mathrm{d}\mathrm{i}\mathrm{c}\mathrm{t}\mathrm{h}\infty [Si] Y. Introduction to University Press, 1976.
SAMA- SUKU-RU Contents p-adic families of Eisenstein series (modular form) Hecke Eisenstein Eisenstein p T
SAMA- SUKU-RU Contents 1. 1 2. 7.1. p-adic families of Eisenstein series 3 2.1. modular form Hecke 3 2.2. Eisenstein 5 2.3. Eisenstein p 7 3. 7.2. The projection to the ordinary part 9 3.1. The ordinary
More information(Kohji Matsumoto) 1 [18] 1999, $- \mathrm{b}^{\backslash }$ $\zeta(s, \alpha)$ Hurwitz, $\Re s>1$ $\Sigma_{n=0}^{\infty}(\alpha+
1160 2000 259-270 259 (Kohji Matsumoto) 1 [18] 1999 $- \mathrm{b}^{\backslash }$ $\zeta(s \alpha)$ Hurwitz $\Re s>1$ $\Sigma_{n=0}^{\infty}(\alpha+n)^{-S}$ $\zeta_{1}(s \alpha)=\zeta(s \alpha)-\alpha^{-}s$
More information0. I II I II (1) linear type: GL( ), Sp( ), O( ), (2) loop type: loop current Kac-Moody affine, hyperbolic (3) diffeo t
e-mail: koyama@math.keio.ac.jp 0. I II I II (1) linear type: GL( ), Sp( ), O( ), (2) loop type: loop current Kac-Moody affine, hyperbolic (3) diffeo type: diffeo universal Teichmuller modular I. I-. Weyl
More informationcubic zeta 1ifting (Tomoyoshi IBUKIYAMA) (Department of Math., Graduate School of Sci., Osaka Univ. 1 \Re $\Phi^{\mathrm{J}}$ 1
1398 2004 137-148 137 cubic zeta 1ifting (Tomoyoshi IBUKIYAMA) (Department of Math., Graduate School of Sci., Osaka Univ. 1 \Re $\Phi^{\mathrm{J}}$ 1 W. Kohnen } $SL_{2}(\mathbb{Z})$ 1 1 2 1 1 1 \sigma
More informationSiegel Hecke 1 Siege Hecke L L Fourier Dirichlet Hecke Euler L Euler Fourier Hecke [Fr] Andrianov [An2] Hecke Satake L van der Geer ([vg]) L [Na1] [Yo
Siegel Hecke 1 Siege Hecke L L Fourier Dirichlet Hecke Euler L Euler Fourier Hecke [Fr] Andrianov [An2] Hecke Satake L van der Geer ([vg]) L [Na1] [Yo] 2 Hecke ( ) 0 1n J n =, Γ = Γ n = Sp(n, Z) = {γ GL(2n,
More informationhave is The explicit upper bound of the multiple integral of $S(t)$ on the Riemann Hypothesis Takahiro Wakasa Graduate School of Ma
The explicit upper bound of the mul Titlethe Riemann Hypothesis (Analytic Nu Theory through Approximation As Author(s) Wakasa, Takahiro Citation 数理解析研究所講究録 (2014), 1874: 12-21 Issue Date 2014-01 URL http://hdlhlenet/2433/195548
More information(Masatake MORI) 1., $I= \int_{-1}^{1}\frac{dx}{\mathrm{r}_{2-x})(1-\mathcal{i}1}.$ (1.1) $\overline{(2-x)(1-\mathcal{i})^{1}/4(1
1040 1998 143-153 143 (Masatake MORI) 1 $I= \int_{-1}^{1}\frac{dx}{\mathrm{r}_{2-x})(1-\mathcal{i}1}$ (11) $\overline{(2-x)(1-\mathcal{i})^{1}/4(1+x)3/4}$ 1974 [31 8 10 11] $I= \int_{a}^{b}f(\mathcal{i})d_{x}$
More information(Osamu Ogurisu) V. V. Semenov [1] :2 $\mu$ 1/2 ; $N-1$ $N$ $\mu$ $Q$ $ \mu Q $ ( $2(N-1)$ Corollary $3.5_{\text{ }}$ Remark 3
Title 異常磁気能率を伴うディラック方程式 ( 量子情報理論と開放系 ) Author(s) 小栗栖, 修 Citation 数理解析研究所講究録 (1997), 982: 41-51 Issue Date 1997-03 URL http://hdl.handle.net/2433/60922 Right Type Departmental Bulletin Paper Textversion
More information$6\mathrm{V}\mathrm{I}\mathrm{I}\mathrm{I}$ (p (Kazuhiro Sakuma) Dept. of Math. and Phys., Kinki Univ.,. (,,.) \S 0. $C^{\infty
$6\mathrm{V}\mathrm{I}\mathrm{I}\mathrm{I}$ (p 1233 2001 111-121 111 (Kazuhiro Sakuma) Dept of Math and Phys Kinki Univ ( ) \S 0 $M^{n}$ $N^{p}$ $n$ $p$ $f$ $M^{n}arrow N^{p}$ $n
More informationSiegel modular forms of middle parahoric subgroups and Ihara lift ( Tomoyoshi Ibukiyama Osaka University 1. Introduction [8] Ihara Sp(2, R) p
Siegel modular forms of middle parahoric subgroups and Ihara lift ( Tomoyoshi Ibukiyama Osaka University 1. Introduction [8] Ihara 80 1963 Sp(2, R) p L holomorphic discrete series Eichler Brandt Eichler
More information2.1 H f 3, SL(2, Z) Γ k (1) f H (2) γ Γ f k γ = f (3) f Γ \H cusp γ SL(2, Z) f k γ Fourier f k γ = a γ (n)e 2πinz/N n=0 (3) γ SL(2, Z) a γ (0) = 0 f c
GL 2 1 Lie SL(2, R) GL(2, A) Gelbart [Ge] 1 3 [Ge] Jacquet-Langlands [JL] Bump [Bu] Borel([Bo]) ([Ko]) ([Mo]) [Mo] 2 2.1 H = {z C Im(z) > 0} Γ SL(2, Z) Γ N N Γ (N) = {γ SL(2, Z) γ = 1 2 mod N} g SL(2,
More information数論的量子カオスと量子エルゴード性
$\lambda$ 1891 2014 1-18 1 (Shin-ya Koyama) ( (Toyo University))* 1. 1992 $\lambdaarrow\infty$ $u_{\lambda}$ 2 ( ) $($ 1900, $)$ $*$ $350-8585$ 2100 2 (1915 ) (1956 ) ( $)$ (1980 ) 3 $\lambda$ (1) : $GOE$
More informationTitle 二重指数関数型変数変換を用いたSinc 関数近似 ( 科学技術における数値計算の理論と応用 II) Author(s) 杉原, 正顯 Citation 数理解析研究所講究録 (1997), 990: Issue Date URL
Title 二重指数関数型変数変換を用いたSinc 関数近似 ( 科学技術における数値計算の理論と応用 II) Author(s) 杉原 正顯 Citation 数理解析研究所講究録 (1997) 990 125-134 Issue Date 1997-04 URL http//hdlhandlenet/2433/61094 Right Type Departmental Bulletin Paper
More information105 $\cdot$, $c_{0},$ $c_{1},$ $c_{2}$, $a_{0},$ $a_{1}$, $\cdot$ $a_{2}$,,,,,, $f(z)=a_{0}+a_{1}z+a_{2}z^{2}+\cdots$ (16) $z=\emptyset(w)=b_{1}w+b_{2
1155 2000 104-119 104 (Masatake Mori) 1 $=\mathrm{l}$ 1970 [2, 4, 7], $=-$, $=-$,,,, $\mathrm{a}^{\mathrm{a}}$,,, $a_{0}+a_{1}z+a_{2}z^{2}+\cdots$ (11), $z=\alpha$ $c_{0}+c_{1}(z-\alpha)+c2(z-\alpha)^{2}+\cdots$
More informationTitle 素数の3 乗の和で表せない自然数の密度について ( 解析的整数論とその周辺 ) Author(s) 川田, 浩一 Citation 数理解析研究所講究録 (2009), 1665: Issue Date URL
Title 素数の3 乗の和で表せない自然数の密度について ( 解析的整数論とその周辺 ) Author(s) 川田 浩一 Citation 数理解析研究所講究録 (2009) 1665: 175-184 Issue Date 2009-10 URL http://hdlhandlenet/2433/141041 Right Type Departmental Bulletin Paper Textversion
More informationuntitled
Lie L ( Introduction L Rankin-Selberg, Hecke L (,,, Rankin, Selberg L (GL( GL( L, L. Rankin-Selberg, Fourier, (=Fourier (= Basic identity.,,.,, L.,,,,., ( Lie G (=G, G.., 5, Sp(, R,. L., GL(n, R Whittaker
More information共役類の積とウィッテンL-関数の特殊値との関係について (解析的整数論 : 数論的対象の分布と近似)
数理解析研究所講究録第 2013 巻 2016 年 1-6 1 共役類の積とウィッテン \mathrm{l} 関数の特殊値との関係に ついて 東京工業大学大学院理工学研究科数学専攻関正媛 Jeongwon {\rm Min} Department of Mathematics, Tokyo Institute of Technology * 1 ウィツテンゼータ関数とウィツテン \mathrm{l}
More information1980年代半ば,米国中西部のモデル 理論,そして未来-モデル理論賛歌
2016 9 27 RIMS 1 2 3 1983 9-1989 6 University of Illinois at Chicago (UIC) John T Baldwin 1983 9-1989 6 University of Illinois at Chicago (UIC) John T Baldwin Y N Moschovakis, Descriptive Set Theory North
More informationHierarchical model and triviality of $\phi_{4}^{4}$ abstract (Takashi Hara) (Tetsuya Hattori) $\mathrm{w}\mathrm{a}\mathrm{t}\mat
1134 2000 70-80 70 Hierarchical model and triviality of $\phi_{4}^{4}$ abstract (Takashi Hara) (Tetsuya Hattori) $\mathrm{w}\mathrm{a}\mathrm{t}\mathrm{a}\mathrm{n}\mathrm{a}\mathrm{b}\mathrm{e}$ (Hiroshi
More information$\mathfrak{m}$ $K/F$ the 70 4(Brinkhuis) ([1 Corollary 210] [2 Corollary 21]) $F$ $K/F$ $F$ Abel $Gal(Ic/F)$ $(2 \cdot\cdot \tau 2)$ $K/F$ NIB ( 13) N
$\mathbb{q}$ 1097 1999 69-81 69 $\mathrm{m}$ 2 $\mathrm{o}\mathrm{d}\mathfrak{p}$ ray class field 2 (Fuminori Kawamoto) 1 INTRODUCTION $F$ $F$ $K/F$ Galois $G:=Ga\iota(K/F)$ Galois $\alpha\in \mathit{0}_{k}$
More information110 $\ovalbox{\tt\small REJECT}^{\mathrm{i}}1W^{\mathrm{p}}\mathrm{n}$ 2 DDS 2 $(\mathrm{i}\mathrm{y}\mu \mathrm{i})$ $(\mathrm{m}\mathrm{i})$ 2
1539 2007 109-119 109 DDS (Drug Deltvery System) (Osamu Sano) $\mathrm{r}^{\mathrm{a}_{w^{1}}}$ $\mathrm{i}\mathrm{h}$ 1* ] $\dot{n}$ $\mathrm{a}g\mathrm{i}$ Td (Yisaku Nag$) JST CREST 1 ( ) DDS ($\mathrm{m}_{\mathrm{u}\mathrm{g}}\propto
More information$\mathrm{s}$ DE ( Kenta Kobayashi ), (Hisashi Okamoto) (Research Institute for Mathematical Sciences, Kyoto Univ.) (Jinghui Zhu)
$\mathrm{s}$ 1265 2002 209-219 209 DE ( Kenta Kobayashi ), (Hisashi Okamoto) (Research Institute for Mathematical Sciences, Kyoto Univ) (Jinghui Zhu) 1 Iiitroductioii (Xiamen Univ) $c$ (Fig 1) Levi-Civita
More information時間遅れをもつ常微分方程式の基礎理論入門 (マクロ経済動学の非線形数理)
1713 2010 72-87 72 Introduction to the theory of delay differential equations (Rinko Miyazaki) Shizuoka University 1 $\frac{dx(t)}{dt}=ax(t)$ (11), $(a$ : $a\neq 0)$ 11 ( ) $t$ (11) $x$ 12 $t$ $x$ $x$
More information1 M = (M, g) m Riemann N = (N, h) n Riemann M N C f : M N f df : T M T N M T M f N T N M f 1 T N T M f 1 T N C X, Y Γ(T M) M C T M f 1 T N M Levi-Civi
1 Surveys in Geometry 1980 2 6, 7 Harmonic Map Plateau Eells-Sampson [5] Siu [19, 20] Kähler 6 Reports on Global Analysis [15] Sacks- Uhlenbeck [18] Siu-Yau [21] Frankel Siu Yau Frankel [13] 1 Surveys
More information平成 29 年度 ( 第 39 回 ) 数学入門公開講座テキスト ( 京都大学数理解析研究所, 平成 29 ~8 年月 73 月日開催 31 日 Riemann Riemann ( ). π(x) := #{p : p x} x log x (x ) Hadamard de
Riemann Riemann 07 7 3 8 4 ). π) : #{p : p } log ) Hadamard de la Vallée Poussin 896 )., f) g) ) lim f) g).. π) Chebychev. 4 3 Riemann. 6 4 Chebychev Riemann. 9 5 Riemann Res). A :. 5 B : Poisson Riemann-Lebesgue
More informationDesign of highly accurate formulas for numerical integration in weighted Hardy spaces with the aid of potential theory 1 Ken ichiro Tanaka 1 Ω R m F I = F (t) dt (1.1) Ω m m 1 m = 1 1 Newton-Cotes Gauss
More informationベクトルの近似直交化を用いた高階線型常微分方程式の整数型解法
1848 2013 132-146 132 Fuminori Sakaguchi Graduate School of Engineering, University of Fukui ; Masahito Hayashi Graduate School of Mathematics, Nagoya University; Centre for Quantum Technologies, National
More information2016 Course Description of Undergraduate Seminars (2015 12 16 ) 2016 12 16 ( ) 13:00 15:00 12 16 ( ) 1 21 ( ) 1 13 ( ) 17:00 1 14 ( ) 12:00 1 21 ( ) 15:00 1 27 ( ) 13:00 14:00 2 1 ( ) 17:00 2 3 ( ) 12
More information$\text{ ^{ } }\dot{\text{ }}$ KATSUNORI ANO, NANZAN UNIVERSITY, DERA MDERA, MDERA 1, (, ERA(Earned Run Average) ),, ERA 1,,
併殺を考慮したマルコフ連鎖に基づく投手評価指標とそ Titleの 1997 年度日本プロ野球シーズンでの考察 ( 最適化のための連続と離散数理 ) Author(s) 穴太, 克則 Citation 数理解析研究所講究録 (1999), 1114: 114-125 Issue Date 1999-11 URL http://hdlhandlenet/2433/63391 Right Type Departmental
More informationWolfram Alpha と数学教育 (数式処理と教育)
1735 2011 107-114 107 Wolfram Alpha (Shinya Oohashi) Chiba prefectural Funabashi-Asahi Highschool 2009 Mathematica Wolfram Research Wolfram Alpha Web Wolfram Alpha 1 PC Web Web 2009 Wolfram Alpha 2 Wolfram
More informationTitle 井草氏の結果の多変数化 : 局所ゼータ関数がガンマ関数の積で書ける場合について ( 概均質ベクトル空間の研究 ) Author(s) 天野, 勝利 Citation 数理解析研究所講究録 (2001), 1238: 1-11 Issue Date URL
Title 井草氏の結果の多変数化 : 局所ゼータ関数がガンマ関数の積で書ける場合について ( 概均質ベクトル空間の研究 ) Author(s) 天野 勝利 Citation 数理解析研究所講究録 (2001) 1238: 1-11 Issue Date 2001-11 URL http://hdlhandlenet/2433/41569 Right Type Departmental Bulletin
More informationヘンリー・ブリッグスの『対数算術』と『数理精蘊』の対数部分について : 会田安明『対数表起源』との関連を含めて (数学史の研究)
1739 2011 214-225 214 : 1 RJMS 2010 8 26 (Henry Briggs, 1561-16301) $Ar ithmetica$ logarithmica ( 1624) (Adriaan Vlacq, 1600-1667 ) 1628 [ 2. (1628) Tables des Sinus, Tangentes et Secantes; et des Logarithmes
More information数理解析研究所講究録 第1908巻
1908 2014 78-85 78 1 D3 1 [20] Born [18, 21] () () RIMS ( 1834) [19] ( [16] ) [1, 23, 24] 2 $\Vert A\Vert^{2}$ $c*$ - $*:\mathcal{x}\ni A\mapsto A^{*}\in \mathcal{x}$ $\Vert A^{*}A\Vert=$ $\Vert\cdot\Vert$
More information[bica]) our gmeff means Abel Milnor $K$ - motif (Mochizuki Satoshi) * Graduate School of Mathematical Sciences, the University o
Title 半 Abel 多様体に付随するMilnor $K$- 群のmotif 論的解釈 ( 代数的整数論とその周辺 ) Author(s) 望月, 哲史 Citation 数理解析研究所講究録 (2005), 1451: 155-164 Issue Date 2005-10 URL http://hdl.handle.net/2433/47730 Right Type Departmental
More information2016 Institute of Statistical Research
2016 Institute of Statistical Research 2016 Institute of Statistical Research 2016 Institute of Statistical Research 2016 Institute of Statistical Research 2016 Institute of Statistical Research 2016 Institute
More information(Keiko Harai) (Graduate School of Humanities and Sciences Ochanomizu University) $\overline{\mathrm{b} \rfloor}$ (Michie Maeda) (De
Title 可測ノルムに関する条件 ( 情報科学と函数解析の接点 : れまでとこれから ) こ Author(s) 原井 敬子 ; 前田 ミチヱ Citation 数理解析研究所講究録 (2004) 1396: 31-41 Issue Date 2004-10 URL http://hdlhandlenet/2433/25964 Right Type Departmental Bulletin Paper
More informationTitle 疑似乱数生成器の安全性とモンテカルロ法 ( 確率数値解析に於ける諸問題,VI) Author(s) 杉田, 洋 Citation 数理解析研究所講究録 (2004), 1351: Issue Date URL
Title 疑似乱数生成器の安全性とモンテカルロ法 ( 確率数値解析に於ける諸問題,VI) Author(s) 杉田, 洋 Citation 数理解析研究所講究録 (2004), 1351: 33-40 Issue Date 2004-01 URL http://hdlhandlenet/2433/64973 Right Type Departmental Bulletin Paper Textversion
More information14 6. $P179$ 1984 r ( 2 $arrow$ $arrow$ F 7. $P181$ 2011 f ( 1 418[? [ 8. $P243$ ( $\cdot P260$ 2824 F ( 1 151? 10. $P292
1130 2000 13-28 13 USJC (Yasukuni Shimoura I. [ ]. ( 56 1. 78 $0753$ [ ( 1 352[ 2. 78 $0754$ [ ( 1 348 3. 88 $0880$ F ( 3 422 4. 93 $0942$ 1 ( ( 1 5. $P121$ 1281 F ( 1 278 [ 14 6. $P179$ 1984 r ( 2 $arrow$
More informationカルマン渦列の発生の物理と数理 (オイラー方程式の数理 : カルマン渦列と非定常渦運動100年)
1776 2012 28-42 28 (Yukio Takemoto) (Syunsuke Ohashi) (Hiroshi Akamine) (Jiro Mizushima) Department of Mechanical Engineering, Doshisha University 1 (Theodore von Ka rma n, l881-1963) 1911 100 [1]. 3 (B\
More informationTitle 素数判定の決定的多項式時間アルゴリズム ( 代数的整数論とその周辺 ) Author(s) 木田, 雅成 Citation 数理解析研究所講究録 (2003), 1324: Issue Date URL
Title 素数判定の決定的多項式時間アルゴリズム ( 代数的整数論とその周辺 ) Author(s) 木田 雅成 Citation 数理解析研究所講究録 (2003) 1324: 22-32 Issue Date 2003-05 URL http://hdlhandlenet/2433/43143 Right Type Departmental Bulletin Paper Textversion
More informationTitle SIEGEL CUSP FORMS の LIFTING の実例 ( 代数群上の形式 保型表現と保型的 $L$ 関数 ) Author(s) 池田, 保 Citation 数理解析研究所講究録 (2000), 1173: Issue Date URL http:
Title SIEGEL CUSP FORMS の LIFTING の実例 ( 代数群上の形式 保型表現と保型的 $L$ 関数 ) Author(s) 池田, 保 Citation 数理解析研究所講究録 (2000), 1173: 82-97 Issue Date 2000-10 URL http://hdlhandlenet/2433/64447 Right Type Departmental Bulletin
More information( ) 1., ([SU] ): F K k., Z p -, (cf. [Iw2], [Iw3], [Iw6]). K F F/K Z p - k /k., Weil., K., K F F p- ( 4.1).,, Z p -,., Weil..,,. Weil., F, F projectiv
( ) 1 ([SU] ): F K k Z p - (cf [Iw2] [Iw3] [Iw6]) K F F/K Z p - k /k Weil K K F F p- ( 41) Z p - Weil Weil F F projective smooth C C Jac(C)/F ( ) : 2 3 4 5 Tate Weil 6 7 Z p - 2 [Iw1] 2 21 K k k 1 k K
More informationConnection problem for Birkhoff-Okubo equations (Yoshishige Haraoka) Department of Mathematics Kumamoto University 50. $\Lambda$ $n\c
Title Connection problem for Birkhoff-Oku systems and hypergeometric systems) Author(s) 原岡 喜重 Citation 数理解析研究所講究録 (2001) 1239: 1-10 Issue Date 2001-11 URL http://hdl.handle.net/2433/41585 Right Type Departmental
More information$2_{\text{ }}$ weight Duke-Imamogle weight Saito-Kurokawa lifting ( ) weight $2k-2$ ( : ) Siegel $k$ $k$ Hecke compatible liftin
$2_{\text{ }}$ weight 1103 1999 187-199 187 Duke-Imamogle weight Saito-Kurokawa lifting ( ) weight $2k-2$ ( : ) Siegel $k$ $k$ Hecke compatible lifting $([\mathrm{k}\mathrm{u}])$ 1980 Maass [Ma2], Andrianov
More information$\mathbb{h}_{1}^{3}(-c^{2})$ 12 $([\mathrm{a}\mathrm{a}1 [\mathrm{a}\mathrm{a}3])$ CMC Kenmotsu-Bryant CMC $\mathrm{l}^{3}$ Minkowski $H(\neq 0)$ Kenm
995 1997 11-27 11 3 3 Euclid (Reiko Aiyama) (Kazuo Akutagawa) (CMC) $H$ ( ) $H=0$ ( ) Weierstrass $g$ 1 $H\neq 0$ Kenmotsu $([\mathrm{k}])$ $\mathrm{s}^{2}$ 2 $g$ CMC $P$ $([\mathrm{b}])$ $g$ Gauss Bryant
More informationTitle 改良型 S 字型風車についての数値シミュレーション ( 複雑流体の数理とシミュレーション ) Author(s) 桑名, 杏奈 ; 佐藤, 祐子 ; 河村, 哲也 Citation 数理解析研究所講究録 (2007), 1539: Issue Date URL
Title 改良型 S 字型風車についての数値シミュレーション ( 複雑流体の数理とシミュレーション ) Author(s) 桑名, 杏奈 ; 佐藤, 祐子 ; 河村, 哲也 Citation 数理解析研究所講究録 (2007), 1539 43-50 Issue Date 2007-02 URL http//hdlhandlenet/2433/59070 Right Type Departmental
More informationL. S. Abstract. Date: last revised on 9 Feb translated to Japanese by Kazumoto Iguchi. Original papers: Received May 13, L. Onsager and S.
L. S. Abstract. Date: last revised on 9 Feb 01. translated to Japanese by Kazumoto Iguchi. Original papers: Received May 13, 1953. L. Onsager and S. Machlup, Fluctuations and Irreversibel Processes, Physical
More information教科専門科目の内容を活用する教材研究の指導方法 III : TitleTeam 2 プロジェクト ( 数学教師に必要な数学能力に関連する諸問題 ) Author(s) 青山, 陽一 ; 神, 直人 ; 曽布川, 拓也 ; 中馬, 悟朗 Citation 数理解析研究所講究録 (2013), 1828
教科専門科目の内容を活用する教材研究の指導方法 III : TitleTeam 2 プロジェクト ( 数学教師に必要な数学能力に関連する諸問題 Author(s 青山, 陽一 ; 神, 直人 ; 曽布川, 拓也 ; 中馬, 悟朗 Citation 数理解析研究所講究録 (2013, 1828: 61-85 Issue Date 2013-03 URL http://hdl.handle.net/2433/194795
More informationTwist knot orbifold Chern-Simons
Twist knot orbifold Chern-Simons 1 3 M π F : F (M) M ω = {ω ij }, Ω = {Ω ij }, cs := 1 4π 2 (ω 12 ω 13 ω 23 + ω 12 Ω 12 + ω 13 Ω 13 + ω 23 Ω 23 ) M Chern-Simons., S. Chern J. Simons, F (M) Pontrjagin 2.,
More information(Kazuo Iida) (Youichi Murakami) 1,.,. ( ).,,,.,.,.. ( ) ( ),,.. (Taylor $)$ [1].,.., $\mathrm{a}1[2]$ Fermigier et $56\mathrm{m}
1209 2001 223-232 223 (Kazuo Iida) (Youichi Murakami) 1 ( ) ( ) ( ) (Taylor $)$ [1] $\mathrm{a}1[2]$ Fermigier et $56\mathrm{m}\mathrm{m}$ $02\mathrm{m}\mathrm{m}$ Whitehead and Luther[3] $\mathrm{a}1[2]$
More information& 3 3 ' ' (., (Pixel), (Light Intensity) (Random Variable). (Joint Probability). V., V = {,,, V }. i x i x = (x, x,, x V ) T. x i i (State Variable),
.... Deeping and Expansion of Large-Scale Random Fields and Probabilistic Image Processing Kazuyuki Tanaka The mathematical frameworks of probabilistic image processing are formulated by means of Markov
More information$w_{ij}^{\infty}(t)=\delta_{ij},$ $i\leq j,$ $w_{ij}^{0}(t)=0,$ $i>j$ $w_{ii}(t)\neq 0,$ $i=1,$ $\ldots,$ $n$ $W_{\infty}(t),$ $W_{0}(t)$ (14) $L(f)=W
, 2000 pp72-87 $\overline{n}b_{+}/b_{+}$ e-mail: ikeka@math scikumamoto-uacjp September 27, 2000 \S 1 Introduction $\#_{dt}^{1}d^{2}=\exp(q_{2}-q_{1})$ $arrow_{dt}^{d^{2}}2=\exp(q_{3}-q_{2})-\exp(q_{2}-q_{1})$
More informationKullback-Leibler
Kullback-Leibler 206 6 6 http://www.math.tohoku.ac.jp/~kuroki/latex/206066kullbackleibler.pdf 0 2 Kullback-Leibler 3. q i.......................... 3.2........... 3.3 Kullback-Leibler.............. 4.4
More informationCAPELLI (T\^o $\mathrm{r}\mathrm{u}$ UMEDA) MATHEMATICS, KYOTO UNIVERSITY DEPARTMENT $\mathrm{o}\mathrm{p}$ $0$:, Cape i,.,.,,,,.,,,.
1508 2006 1-11 1 CAPELLI (T\^o $\mathrm{r}\mathrm{u}$ UMEDA) MATHEMATICS KYOTO UNIVERSITY DEPARTMENT $\mathrm{o}\mathrm{p}$ $0$: Cape i Capelli 1991 ( ) (1994 ; 1998 ) 100 Capelli Capelli Capelli ( ) (
More informationQ p G Qp Q G Q p Ramanujan 12 q- (q) : (q) = q n=1 (1 qn ) 24 S 12 (SL 2 (Z))., p (ordinary) (, q- p a p ( ) p ). p = 11 a p ( ) p. p 11 p a p
.,.,.,..,, 1.. Contents 1. 1 1.1. 2 1.2. 3 1.3. 4 1.4. Eisenstein 5 1.5. 7 2. 9 2.1. e p 9 2.2. p 11 2.3. 15 2.4. 16 2.5. 18 3. 19 3.1. ( ) 19 3.2. 22 4. 23 1. p., Q Q p Q Q p Q C.,. 1. 1 Q p G Qp Q G
More informationMazur [Ma1] Schlessinger [Sch] [SL] [Ma1] [Ma1] [Ma2] Galois [] 17 R m R R R M End R M) M R ut R M) M R R G R[G] R G Sets 1 Λ Noether Λ k Λ m Λ k C Λ
Galois ) 0 1 1 2 2 4 3 10 4 12 5 14 16 0 Galois Galois Galois TaylorWiles Fermat [W][TW] Galois Galois Galois 1 Noether 2 1 Mazur [Ma1] Schlessinger [Sch] [SL] [Ma1] [Ma1] [Ma2] Galois [] 17 R m R R R
More information$\hat{\grave{\grave{\lambda}}}$ $\grave{\neg}\backslash \backslash ^{}4$ $\approx \mathrm{t}\triangleleft\wedge$ $10^{4}$ $10^{\backslash }$ $4^{\math
$\mathrm{r}\mathrm{m}\mathrm{s}$ 1226 2001 76-85 76 1 (Mamoru Tanahashi) (Shiki Iwase) (Toru Ymagawa) (Toshio Miyauchi) Department of Mechanical and Aerospaoe Engineering Tokyo Institute of Technology
More informationFeynman Encounter with Mathematics 52, [1] N. Kumano-go, Feynman path integrals as analysis on path space by time slicing approximation. Bull
Feynman Encounter with Mathematics 52, 200 9 [] N. Kumano-go, Feynman path integrals as analysis on path space by time slicing approximation. Bull. Sci. Math. vol. 28 (2004) 97 25. [2] D. Fujiwara and
More informationR R P N (C) 7 C Riemann R K ( ) C R C K 8 (R ) R C K 9 Riemann /C /C Riemann 10 C k 11 k C/k 12 Riemann k Riemann C/k k(c)/k R k F q Riemann 15
(Gen KUROKI) 1 1 : Riemann Spec Z 2? 3 : 4 2 Riemann Riemann Riemann 1 C 5 Riemann Riemann R compact R K C ( C(x) ) K C(R) Riemann R 6 (E-mail address: kuroki@math.tohoku.ac.jp) 1 1 ( 5 ) 2 ( Q ) Spec
More information, CH n. CH n, CP n,,,., CH n,,. RH n ( Cartan )., CH n., RH n CH n,,., RH n, CH n., RH n ( ), CH n ( 1.1 (v), (vi) )., RH n,, CH n,., CH n,. 1.2, CH n
( ), Jürgen Berndt,.,. 1, CH n.,,. 1.1 ([6]). CH n (n 2), : (i) CH k (k = 0,..., n 1) tube. (ii) RH n tube. (iii). (iv) ruled minimal, equidistant. (v) normally homogeneous submanifold F k tube. (vi) normally
More informationcompact compact Hermann compact Hermite ( - ) Hermann Hermann ( ) compact Hermite Lagrange compact Hermite ( ) a, Σ a {0} a 3 1
014 5 4 compact compact Hermann compact Hermite ( - ) Hermann Hermann ( ) compact Hermite Lagrange compact Hermite ( ) 1 1.1. a, Σ a {0} a 3 1 (1) a = span(σ). () α, β Σ s α β := β α,β α α Σ. (3) α, β
More information1 1 1 1 1 1 2 f z 2 C 1, C 2 f 2 C 1, C 2 f(c 2 ) C 2 f(c 1 ) z C 1 f f(z) xy uv ( u v ) = ( a b c d ) ( x y ) + ( p q ) (p + b, q + d) 1 (p + a, q + c) 1 (p, q) 1 1 (b, d) (a, c) 2 3 2 3 a = d, c = b
More information5 / / $\mathrm{p}$ $\mathrm{r}$ 8 7 double 4 22 / [10][14][15] 23 P double 1 $\mathrm{m}\mathrm{p}\mathrm{f}\mathrm{u}\mathrm{n}/\mathrm{a
double $\mathrm{j}\mathrm{s}\mathrm{t}$ $\mathrm{q}$ 1505 2006 1-13 1 / (Kinji Kimura) Japan Science and Technology Agency Faculty of Science Rikkyo University 1 / / 6 1 2 3 4 5 Kronecker 6 2 21 $\mathrm{p}$
More information133 1.,,, [1] [2],,,,, $[3],[4]$,,,,,,,,, [5] [6],,,,,, [7], interface,,,, Navier-Stokes, $Petr\dot{o}$v-Galerkin [8], $(,)$ $()$,,
836 1993 132-146 132 Navier-Stokes Numerical Simulations for the Navier-Stokes Equations in Incompressible Viscous Fluid Flows (Nobuyoshi Tosaka) (Kazuhiko Kakuda) SUMMARY A coupling approach of the boundary
More information$\mathrm{v}$ ( )* $*1$ $\ovalbox{\tt\small REJECT}*2$ \searrow $\mathrm{b}$ $*3$ $*4$ ( ) [1] $*5$ $\mathrm{a}\mathrm{c}
Title 狩野本 綴術算経 について ( 数学史の研究 ) Author(s) 小川 束 Citation 数理解析研究所講究録 (2004) 1392: 60-68 Issue Date 2004-09 URL http://hdlhandlenet/2433/25859 Right Type Departmental Bulletin Paper Textversion publisher Kyoto
More informationa m 1 mod p a km 1 mod p k<s 1.6. n > 1 n 1= s m, (m, = 1 a n n a m 1 mod n a km 1 mod n k<sn a 1.7. n > 1 n 1= s m, (m, = 1 r n ν = min ord (p 1 (1 B
10 004 Journal of the Institute of Science and Engineering. Chuo University Euler n > 1 p n p ord p n n n 1= s m (m B psp = {a (Z/nZ ; a n 1 =1}, B epsp = { ( a (Z/nZ ; a n 1 a }, = n B spsp = { a (Z/nZ
More information(a) (b) (c) (d) 1: (a) (b) (c) (d) (a) (b) (c) 2: (a) (b) (c) 1(b) [1 10] 1 degree k n(k) walk path 4
1 vertex edge 1(a) 1(b) 1(c) 1(d) 2 (a) (b) (c) (d) 1: (a) (b) (c) (d) 1 2 6 1 2 6 1 2 6 3 5 3 5 3 5 4 4 (a) (b) (c) 2: (a) (b) (c) 1(b) [1 10] 1 degree k n(k) walk path 4 1: Zachary [11] [12] [13] World-Wide
More informationxia2.dvi
Journal of Differential Equations 96 (992), 70-84 Melnikov method and transversal homoclinic points in the restricted three-body problem Zhihong Xia Department of Mathematics, Harvard University Cambridge,
More information1
1 Borel1956 Groupes linéaire algébriques, Ann. of Math. 64 (1956), 20 82. Chevalley1956/58 Sur la classification des groupes de Lie algébriques, Sém. Chevalley 1956/58, E.N.S., Paris. Tits1959 Sur la classification
More information189 2 $\mathrm{p}\mathrm{a}$ (perturbation analysis ) PA (Ho&Cao [5] ) 1 FD 1 ( ) / PA $\mathrm{p}\mathrm{a}$ $\mathrm{p}\mathrm{a}$ (infinite
947 1996 188-199 188 (Hideaki Takada) (Naoto Miyoshi) (Toshiharu Hasegawa) Abstract (perturbation analysis) 1 1 1 ( ) $R$ (stochastic discrete event system) (finite difference $\mathrm{f}\mathrm{d}$ estimate
More informationExplicit form of the evolution oper TitleCummings model and quantum diagonal (Dynamical Systems and Differential Author(s) 鈴木, 達夫 Citation 数理解析研究所講究録
Explicit form of the evolution oper TitleCummings model and quantum diagonal (Dynamical Systems and Differential Author(s) 鈴木 達夫 Citation 数理解析研究所講究録 (2004) 1408: 97-109 Issue Date 2004-12 URL http://hdlhandlenet/2433/26142
More information}$ $q_{-1}=0$ OSTROWSKI (HASHIMOTO RYUTA) $\mathrm{d}\mathrm{c}$ ( ) ABSTRACT Ostrowski $x^{2}-$ $Dy^{2}=N$ $-$ - $Ax^{2}+Bx
Title 2 元 2 次不定方程式の整数解の OSTROWSKI 表現について ( 代数的整数論とその周辺 ) Author(s) 橋本 竜太 Citation 数理解析研究所講究録 (2000) 1154 155-164 Issue Date 2000-05 URL http//hdlhandlenet/2433/64118 Right Type Departmental Bulletin Paper
More informationk + (1/2) S k+(1/2) (Γ 0 (N)) N p Hecke T k+(1/2) (p 2 ) S k+1/2 (Γ 0 (N)) M > 0 2k, M S 2k (Γ 0 (M)) Hecke T 2k (p) (p M) 1.1 ( ). k 2 M N M N f S k+
1 SL 2 (R) γ(z) = az + b cz + d ( ) a b z h, γ = SL c d 2 (R) h 4 N Γ 0 (N) {( ) } a b Γ 0 (N) = SL c d 2 (Z) c 0 mod N θ(z) θ(z) = q n2 q = e 2π 1z, z h n Z Γ 0 (4) j(γ, z) ( ) a b θ(γ(z)) = j(γ, z)θ(z)
More information第5章 偏微分方程式の境界値問題
October 5, 2018 1 / 113 4 ( ) 2 / 113 Poisson 5.1 Poisson ( A.7.1) Poisson Poisson 1 (A.6 ) Γ p p N u D Γ D b 5.1.1: = Γ D Γ N 3 / 113 Poisson 5.1.1 d {2, 3} Lipschitz (A.5 ) Γ D Γ N = \ Γ D Γ p Γ N Γ
More information* (Ben T. Nohara), (Akio Arimoto) Faculty of Knowledge Engineering, Tokyo City University * 1 $\cdot\cdot
外力項付常微分方程式の周期解および漸近周期解の初期 Title値問題について ( 力学系 : 理論から応用へ 応用から理論へ ) Author(s) 野原, 勉 ; 有本, 彰雄 Citation 数理解析研究所講究録 (2011), 1742: 108-118 Issue Date 2011-05 URL http://hdl.handle.net/2433/170924 Right Type Departmental
More information1. ( ) L L L Navier-Stokes η L/η η r L( ) r [1] r u r ( ) r Sq u (r) u q r r ζ(q) (1) ζ(q) u r (1) ( ) Kolmogorov, Obukov [2, 1] ɛ r r u r r 1 3
Kolmogorov Toward Large Deviation Statistical Mechanics of Strongly Correlated Fluctuations - Another Legacy of A. N. Kolmogorov - Hirokazu FUJISAKA Abstract Recently, spatially or temporally strongly
More information可積分測地流を持つエルミート多様体のあるクラスについて (幾何学的力学系の新展開)
1774 2012 63-77 63 Kazuyoshi Kiyoharal Department of Mathematics Okayama University 1 (Hermite-Liouville ) Hermite-Liouville (H-L) Liouville K\"ahler-Liouville (K-L $)$ Liouville Liouville ( FLiouville-St\"ackel
More informationKobe University Repository : Kernel タイトル Title 著者 Author(s) 掲載誌 巻号 ページ Citation 刊行日 Issue date 資源タイプ Resource Type 版区分 Resource Version 権利 Rights DOI
Kobe University Repository : Kernel タイトル Title 著者 Author(s) 掲載誌 巻号 ページ Citation 刊行日 Issue date 資源タイプ Resource Type 版区分 Resource Version 権利 Rights DOI 平均に対する平滑化ブートストラップ法におけるバンド幅の選択に関する一考察 (A Study about
More information(Team 2 ) (Yoichi Aoyama) Faculty of Education Shimane University (Goro Chuman) Professor Emeritus Gifu University (Naondo Jin)
教科専門科目の内容を活用する教材研究の指導方法 : TitleTeam2プロジェクト ( 数学教師に必要な数学能力形成に関する研究 ) Author(s) 青山 陽一 ; 中馬 悟朗 ; 神 直人 Citation 数理解析研究所講究録 (2009) 1657: 105-127 Issue Date 2009-07 URL http://hdlhandlenet/2433/140885 Right
More information2.3. p(n)x n = n=0 i= x = i x x 2 x 3 x..,?. p(n)x n = + x + 2 x x 3 + x + 7 x + x + n=0, n p(n) x n, ( ). p(n) (mother function)., x i = + xi +
( ) : ( ) n, n., = 2+2+,, = 2 + 2 + = 2 + + 2 = + 2 + 2,,,. ( composition.), λ = (2, 2, )... n (partition), λ = (λ, λ 2,..., λ r ), λ λ 2 λ r > 0, r λ i = n i=. r λ, l(λ)., r λ i = n i=, λ, λ., n P n,
More information42 1 ( ) 7 ( ) $\mathrm{s}17$ $-\supset$ 2 $(1610?\sim 1624)$ 8 (1622) (3 ), 4 (1627?) 5 (1628) ( ) 6 (1629) ( ) 8 (1631) (2 ) $\text{ }$ ( ) $\text{
26 [\copyright 0 $\perp$ $\perp$ 1064 1998 41-62 41 REJECT}$ $=\underline{\not\equiv!}\xi*$ $\iota_{arrow}^{-}\approx 1,$ $\ovalbox{\tt\small ffl $\mathrm{y}
More informationå‰Łçı—訋çfl»æ³Łã†¨ã…Łã‡£ã…œã…−ã……ã…†æŁ°, ㆚ㆮ2æ¬¡è©Łä¾¡å‹ƒå›²ã•† ㅋㅪㅜã…−ã……ã…†æŁ°å‹Šã†«ã‡‹ã‡‰é•£ã†®ç¢ºç”⁄訋箊
, 2 August 28 (Fri), 2016 August 28 (Fri), 2016 1 / 64 Outline 1 2 3 2 4 2 5 6 August 28 (Fri), 2016 2 / 64 fibonacci Lucas 2 August 28 (Fri), 2016 3 / 64 Dynamic Programming R.Bellman Bellman Continuum
More informationSEISMIC HAZARD ESTIMATION BASED ON ACTIVE FAULT DATA AND HISTORICAL EARTHQUAKE DATA By Hiroyuki KAMEDA and Toshihiko OKUMURA A method is presented for using historical earthquake data and active fault
More informationuntitled
2 : n =1, 2,, 10000 0.5125 0.51 0.5075 0.505 0.5025 0.5 0.4975 0.495 0 2000 4000 6000 8000 10000 2 weak law of large numbers 1. X 1,X 2,,X n 2. µ = E(X i ),i=1, 2,,n 3. σi 2 = V (X i ) σ 2,i=1, 2,,n ɛ>0
More information$\mathfrak{u}_{1}$ $\frac{\epsilon_{1} }{1-\mathcal{E}_{1}^{J}}<\frac{\vee 1\prime}{2}$ $\frac{1}{1-\epsilon_{1} }\frac{1}{1-\epsilon_{\sim} }$ $\frac
$\vee$ 1017 1997 92-103 92 $\cdot\mathrm{r}\backslash$ $GL_{n}(\mathbb{C}$ \S1 1995 Milnor Introduction to algebraic $\mathrm{k}$-theory $narrow \infty$ $GL_{n}(\mathbb{C}$ $\mathit{1}\mathrm{t}i_{n}(\mathbb{c}$
More informationTitle KETpicによる曲面描画と教育利用 ( 数式処理と教育教育における数式処理システムの効果的利用に関する研究 ) : 数学 Author(s) 金子, 真隆 ; 阿部, 孝之 ; 関口, 昌由 ; 山下, 哲 ; 高遠, Citation 数理解析研究所講究録 (2009), 1624:
Title KETpicによる曲面描画と教育利用 ( 数式処理と教育教育における数式処理システムの効果的利用に関する研究 ) : 数学 Author(s) 金子, 真隆 ; 阿部, 孝之 ; 関口, 昌由 ; 山下, 哲 ; 高遠, Citation 数理解析研究所講究録 (2009), 1624: 1-10 Issue Date 2009-01 URL http://hdl.handle.net/2433/140279
More informationZ: Q: R: C: sin 6 5 ζ a, b
Z: Q: R: C: 3 3 7 4 sin 6 5 ζ 9 6 6............................... 6............................... 6.3......................... 4 7 6 8 8 9 3 33 a, b a bc c b a a b 5 3 5 3 5 5 3 a a a a p > p p p, 3,
More informationHohenegger & Schär, a cm b Kitoh et. al., Gigerenzer et. al. Susan et. al.
Study on characteristics of inhabitants acceptance of weather information with a probability Motohiro HONMA *, Kyoko ARAI **, Kento MATSUMOTO *** and Yasushi SUZUKI *** Abstract In this study, we performed
More information2 A A 3 A 2. A [2] A A A A 4 [3]
1 2 A A 1. ([1]3 3[ ]) 2 A A 3 A 2. A [2] A A A A 4 [3] Xi 1 1 2 1 () () 1 n () 1 n 0 i i = 1 1 S = S +! X S ( ) 02 n 1 2 Xi 1 0 2 ( ) ( 2) n ( 2) n 0 i i = 1 2 S = S +! X 0 k Xip 1 (1-p) 1 ( ) n n k Pr
More informationi Version 1.1, (2012/02/22 24),.,..,.,,. R-space,, ( R- space),, Kahler (Kähler C-space)., R-space,., R-space, Hermite,.
R-space ( ) Version 1.1 (2012/02/29) i Version 1.1, (2012/02/22 24),.,..,.,,. R-space,, ( R- space),, Kahler (Kähler C-space)., R-space,., R-space, Hermite,. ii 1 Lie 1 1.1 Killing................................
More informationsakigake1.dvi
(Zin ARAI) arai@cris.hokudai.ac.jp http://www.cris.hokudai.ac.jp/arai/ 1 dynamical systems ( mechanics ) dynamical systems 3 G X Ψ:G X X, (g, x) Ψ(g, x) =:Ψ g (x) Ψ id (x) =x, Ψ gh (x) =Ψ h (Ψ g (x)) (
More information( ) ( ) (B) ( , )
() 2006 2 6 () 2006 2 6 2 7 7 (B) ( 574009, ) 2006 4 .,.. Introduction. [6], I. Simon (), J.-E. Pin. min-plus ().,,,. min-plus. (min-plus ). a, b R,, { a b := min(a, b), a b := a + b.. (R,, ) (, ). ( min-plus
More informationChern-Simons Jones 3 Chern-Simons 1 - Chern-Simons - Jones J(K; q) [1] Jones q 1 J (K + ; q) qj (K ; q) = (q 1/2 q
Chern-Simons E-mail: fuji@th.phys.nagoya-u.ac.jp Jones 3 Chern-Simons - Chern-Simons - Jones J(K; q) []Jones q J (K + ; q) qj (K ; q) = (q /2 q /2 )J (K 0 ; q), () J( ; q) =. (2) K Figure : K +, K, K 0
More information1 4 1 ( ) ( ) ( ) ( ) () 1 4 2
7 1995, 2017 7 21 1 2 2 3 3 4 4 6 (1).................................... 6 (2)..................................... 6 (3) t................. 9 5 11 (1)......................................... 11 (2)
More information( ) (, ) arxiv: hgm OpenXM search. d n A = (a ij ). A i a i Z d, Z d. i a ij > 0. β N 0 A = N 0 a N 0 a n Z A (β; p) = Au=β,u N n 0 A
( ) (, ) arxiv: 1510.02269 hgm OpenXM search. d n A = (a ij ). A i a i Z d, Z d. i a ij > 0. β N 0 A = N 0 a 1 + + N 0 a n Z A (β; p) = Au=β,u N n 0 A-. u! = n i=1 u i!, p u = n i=1 pu i i. Z = Z A Au
More informationリカレンスプロット : 時系列の視覚化を越えて (マクロ経済動学の非線形数理)
1768 2011 150-162 150 : Recurrence plots: Beyond visualization of time series Yoshito Hirata Institute of Industrial Science, The University of Tokyo voshito@sat. t.u\cdot tokvo.ac.ip 1 1. 1987 (Eckmann
More informationZ[i] Z[i] π 4,1 (x) π 4,3 (x) 1 x (x ) 2 log x π m,a (x) 1 x ϕ(m) log x 1.1 ( ). π(x) x (a, m) = 1 π m,a (x) x modm a 1 π m,a (x) 1 ϕ(m) π(x)
3 3 22 Z[i] Z[i] π 4, (x) π 4,3 (x) x (x ) 2 log x π m,a (x) x ϕ(m) log x. ( ). π(x) x (a, m) = π m,a (x) x modm a π m,a (x) ϕ(m) π(x) ϕ(m) x log x ϕ(m) m f(x) g(x) (x α) lim f(x)/g(x) = x α mod m (a,
More informationTitle Compactification theorems in dimens Topology and Related Problems) Author(s) 木村, 孝 Citation 数理解析研究所講究録 (1996), 953: Issue Date URL
Title Compactification theorems in dimens Topology and Related Problems Authors 木村 孝 Citation 数理解析研究所講究録 1996 953 73-92 Issue Date 1996-06 URL http//hdlhandlenet/2433/60394 Right Type Departmental Bulletin
More information一般相対性理論に関するリーマン計量の変形について
1896 2014 137-149 137 ( ) 1 $(N^{4}, g)$ $N$ 4 $g$ $(3, 1)$ $R_{ab}- \frac{1}{2}rg_{ab}=t_{ab}$ (1) $R_{ab}$ $g$ $R$ $g$ ( ) $T_{ab}$ $T$ $R_{ab}- \frac{1}{2}rg_{ab}=0$ 4 $R_{ab}=0$ $\mathbb{r}^{3,1}$
More information