( ) 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
|
|
|
- あいぞう つちかね
- 6 years ago
- Views:
Transcription
1 ( ) 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 ( ) : Tate Weil 6 7 Z p - 2 [Iw1] 2 21 K k k 1 k K K 1
2 k(t) K K k = k K ( ) v k K ( ) v κ(v) k [κ(v) : k] deg(v) K D(K) D(K) := Zv v: f K v ord v (f) Z div : K D(K) Cl(K) P = v n vv D(K) deg(p ) := v n v deg(v) deg(p ) = 0 0 D 0 (K)( D(K)) div(k ) D 0 (K) Cl 0 (K) := D 0 (K)/div(K ) 0 0 Cl 0 (K) Cl(K) Z Cl 0 (K) K : P D(K) l(p ) := dim k {f K div(f) + P 0} {0} ( v n vv 0 v n v 0 ) P D(K) deg(p ) l(p ) + 1 K K L L k L k L k L K L L L L Cl(L) Cl(L ) Cl 0 (L) Cl 0 (L ) L/K Cl(L) Gal(L/K) N L/K : Cl(L) Cl(K) N L/K : Cl 0 (L) Cl 0 (K) L/K L K L k L/K L Cl(L) := lim Cl(M) Cl 0 (L) := lim Cl 0 (M) M M M L K 2
3 K k k Kk K k = k Kk = K k k Kk k Kk /K k Cl 0 (Kk ) Cl 0 (Kk ) = lim Cl 0 (Kk ) k k k 22 p k K K ZQ p /Z p V (K) V (K) := {f (1/p n ) K Q p /Z p v ord v (f) p n } f (1/p n ) V (K) v (ord v(f)/p n )v V (K) Cl 0 (K)[p ] k Z Q p /Z p (21) 0 k Z Q p /Z p V (K) Cl 0 (K)[p ] 0 k p k 1 p : µ p k K p- K urp (22) V (K) Gal(K urp /K) µ p (f (1/p n ) σ) σ( pn f)/ p n f ( p ) (23) Gal(K urp /K) = HomZ p (V (K) µ p ) k Z Q p /Z p = 0 (21) V (K) = Cl 0 (K)[p ] (23) (24) Gal(K urp /K) = HomZ p (Cl 0 (K)[p ] µ p ) K 0 K K/K 0 (22) Gal(K/K 0 )- (23) (24) Gal(K/K 0 )- Gal(K urp /K) Gal(K/K 0 ) 3 [We2] [SU] 3
4 31 F K F 31 (cf [SU] 692) Cl 0 (K) K Re(s) > 1 ζ K (s) := (1 κ(v) s ) 1 v: κ(v) v 32 (Hasse-Weil cf [We2] Chap VII 7 Theorem 4) K g q = F (i) 2g P K (T ) Z[T ] ζ K (s) = P K (q s ) (1 q s )(1 q 1 s ) P K (T ) ζ K (s) (ii) : ( ) 1 P K (T ) = q g T 2g P K qt (iii) P K (0) = 1 P K (1) = Cl 0 (K) 32 7 K K ur KF K 33 (cf [SU] 812) ρ K : Cl(K) Gal(K ur /K) v Frob v (v Frobenius ) dense Cl 0 (K) : ρ K0 : Cl 0 (K) = Gal(K ur /KF) L/K L (cf [SU]) L/K N L/K : Cl 0 (L) Cl 0 (K) Gal(L ur /LF) Gal(K ur /KF) ρ K0 ρ L0 4
5 4 F K KF( = K F F) F l K 1 l : (41) KF = l-nk(µ n ) Gal(KF/K) = Gal(F/F) Gal(F/F) Frobenius Gal(KF/K) Frob p F KF p- KF urp Y (K) := Gal(KF urp /KF) Gal(KF/K) Y (K) 41 (Weil) (i) g K Z p Y (K) = Z 2g p (ii) P K (T ) K ( 32 (i)) P K (T ) = det(1 FrobT : Y (K) Z p Q p ) k := Q(ζ p ) k /k Z p - k = k(µ p ) ((41) ) k urp k p- X(k) := Gal(k urp /k ) X(k) Y (K) 41 X(k) X(k) (Gal(k/Q) 1 ) X(k) Γ = Gal(k /k) Z p [[Γ]]- Λ := Z p [[T ]] Γ γ Z p [[Γ]] = Λ γ T + 1 X(k) Λ- Gal(k/Q) χ 1 f(t χ) Λ p L L p (s χ) κ : Γ Z p f(κ(γ) s 1 χ) = L p (s χ) (f(t χ) γ ) Weierstrass f(t χ) Q χ (T ) Q(T ) := Q χ (T ) Z p [T ] χ 1: 5
6 42 ( ) (i) X(k) µ- 0 (Ferrero-Washington) Λ- Z p - X(k) = Z λ k p (ii) X(k) Λ char Λ (X(k) )( Z p [T ]) char Λ (X(k) ) = Q(T ) 42 (i) 41 (i) X(k) λ- λ k 2 2g Z p - µ (ii) : 43 (cf [Wa] p292) Λ- M Γ γ T + 1( Λ) M µ- 0 char Λ (M) = det((t + 1) γ : M Z p Q p ) ( T M ) (ii) Q(T ) = det((t + 1) γ : X(k) Z p Q p ) 41 (ii) p L Z p - (1) KF/K (2) Gal(KF/K) = Gal(F/F) = Ẑ ( Λ ) (3) Frob Gal(KF/K) (4) P K (T ) p 1 n Q(µ n ) 42 ([Ho] [Ku] ) Q p
7 51 [DK] [AG] Chap V VII k ( ): {k } {k projective smooth } C/k K(C) K {K } { generic point } projective smooth C/k projective smooth K C K g C M/k C M := C Spec(k) Spec(M) M K(C M ) K k M Weil C/k Jac(C) k g M/k functorial Jac(C)(M) = Cl 0 (K(C M )) k /k (51) Jac(C)(k ) = Cl 0 (Kk ) (Kk = K k k ) k /k Gal(k /k) Gal(Kk /K) Gal(Kk /K) = Gal(k /k) (51) p k k Jac(C)[p n ] := Jac(C)(k)[p n ] Jac(C)[p n ] = (Z/p n ) 2g Jac(C)[p ] = (Q p /Z p ) 2g Weil Gal(k/k)- (52) Jac(C)[p n ] Jac(C)[p n ] µ p n (Weil pairing) p n p n+1 p (53) Jac(C)[p ] T p (Jac(C)) µ p n T p (Jac(C)) Jac(C) (p-)tate T p (Jac(C)) := lim n Jac(C)[p n ] ( p ) T p (Jac(C)) = Z 2g p 7
8 (53) Gal(k/k)- (54) T p (Jac(C)) = Hom(Jac(C)[p ] µ p ) (24) (51) (54) 51 Kk p- Kk urp Gal(Kk/K) = Gal(k/k)- Gal(Kk urp /Kk) = T p (Jac(C)) 52 Weil F K K C F p V p := T p (Jac(C)) Z p Q p V p Gal(F/F) Weil (Weil cf [We1]) P K (T ) 32 (i) P K (T ) = det(1 FrobT : V p ) 53 ζ K (s) = exp( n C(F(n)) q ns ) n ( F = q F(n) [F(n) : F] = n ) : C(F(n)) = 1 + q n Tr(Frob n : V p ) (Frob n Gal(F/F(n)) ) 41 : 51 Gal(KF/K) = Gal(F/F)- Gal(KF urp /KF) = T p (Jac(C)) 41 (i) T p (Jac(C)) = Z 2g p (ii) Weil pairing 32 (ii) (52) p T p (Jac(C)) T p (Jac(C)) lim n µ p n < >: V p V p Q p (1) 8
9 Q p (1) := (lim µ p n) n Z p Q p Frob q 1 x y V p < Frobx Froby >= q < x y > det(1 FrobT : V p ) = (qt ) 2g det(frob : V p ) 1 det(1 Frob(qT ) 1 : V p ) < > (55) det(frob : V p ) = q g p L p L 6 Z p - 61 Riemann-Hurwitz K L k g(k) g(l) 61 (Riemann-Hurwitz cf [Iw1] p 311 [DK] 814) L/K tame 2g(L) 2 = [L : K](2g(K) 2) + (e(v ) 1) e(v ) L/K v v :L 4 k = Q(ζ p ) Z p - λ - (X(k) λ- λ k ) ( 2 ) k CM λ - CM λ - Riemann-Hurwitz ( [Ki] [Iw5] p- ) 62 p- K k p k K K p- ( ) 62 (Grothendieck cf [NSW] Theorem 1012) Gal( K/K) 2g x 1 x 2 x 2g [x 1 x 2 ][x 3 x 4 ] [x 2g 1 x 2g ] = 1 pro-p 9
10 Z p - p- [Wi] [NSW] Chap X 7 Z p - [Iw4] 12 [Wa] Z p - F p F F F 1 p µ p F(µ p ) Gal(F(µ p )/F) Z p F(µ p )/F F Gal(F /F) = Z p F F p- F /F n F n K Z p - K K K := KF K F Γ := Gal(K /K) Γ = Gal(F /F) = Z p K /K n K n K n = KF n K n F n 72 p-part A(K) := Cl 0 (K)[p ] K p- K urp F /F p- K K urp KF K urp = K A(K) = Gal(K urp /K ) L/K A(L) Gal(L urp /L ) N L/K A(K) Gal(K urp /K ) A n := A(K n ) X(K) := lim A n n 10
11 X(K) Γ Z p - Z p [[Γ]] Γ γ (71) Z p [[Γ]] Λ γ T + 1 X(K) Λ := Z p [[T ]]- ( 4 ) 71 Λ- (72) X(K) = Gal(K urp /K ) (Γ Gal(K urp /K ) ) K /K 72 ω n (T ) := (1 + T ) pn 1 Λ A n = X(K)/ωn X(K) A n X(K) Λ- λ µ ν- λ K µ K ν K n A n = p λ Kn+µ K p n +ν K Proof (72) ω n X(K) M n M n /K n K urp K n K urp n K urp K urp n M n M n /K n K urp n M n K urp n = M n X(K)/ω n X(K) = Gal(K urp n /K ) = A n K urp 73 Z p - X(K) λ K µ K X(K) = Z λ K p λ K 2g (g K ) µ K = 0 X(K) Λ- Frob Γ Γ = Gal(F /F) Frobenius (71) Γ Frob 1 (Hyp): Cl 0 (K)[p] = (Z/p) 2g 74 K (Hyp) X(K) Γ Frob 1 Λ- char Λ (X(K)) = q g P K (T + 1) P K (T ) 32 (i) 75 C K Cl 0 (K)[p] = Jac(C)(F)[p] (Hyp) Jac(C)(F)[p] = Jac(C)[p] Weil-pairing F µ p K F /F KF KF (Hyp) (F Jac(C)[p] F(Jac(C)[p]) ) 11
12 74 C K K (Hyp) 76 (Hyp) Jac(C)(F )[p ] = Jac(C)[p ] Proof Gal(F(Jac[p ])/F) GL 2g (Z p ) GL 2g (Z/p) pro-p F p- F F(Jac[p ]) (Hyp) F µ p F µ p (24) (51) (54) (72) 76 (73) X(K) = T p (Jac(C)) 76 Jac(C)[p ] Gal(F/F) Gal(F /F) (73) Gal(F /F)- Γ Frob 1 X(K)( = T p (Jac(C))) µ 0 char(x(k)) = det((t + 1) Frob 1 : T p (Jac(C)) Z p Q p ) ( 43) det((t + 1) Frob 1 ) = det( Frob 1 ) det(1 Frob(T + 1)) 52 (55) 77 Jac(C)(F )[p ] = Jac(C)[p ] (Hyp) 74 K F := F(Jac(C)[p ]) p G Gal(F /F) = Z p G F Z p F Gal(F /F ) = Z p Gal(F /F ) = G X(K) = X(KF ) G G p X(KF ) G X(KF ) = Z 2g p 2g Z p - 73 X(K) char Λ (X(K)) Z p [T ] q g P K (T + 1) K = KF q = F 79 A := Cl 0 (K )[p ] A = lim A n n (Hyp) A = (Qp /Z p ) 2g (24) (72) : lim n A n = Hom(lim A n µ p ) n 12
13 References [AG] Cornell G and Silverman J H eds: Arithmetic Geometry Springer-Verlag New York (1986) [DK] : (1998) [Ho] Horie K: CM fields with all roots of unity Compositio Math 74 (1990) 1 14 [Iw1] : (1973) [Iw2] : 15 (1963) 65 67; Collected Papers [40] [Iw3] Iwasawa K: Analogies between number fields and function fields Some Recent Advances in the Basic Sciences Vol 2 (1969) pp ; Collected Papers [47] [Iw4] Iwasawa K: On Z l -extensions of algebraic number fields Ann of Math (2) 98 (1973) ; Collected Papers [52] [Iw5] Iwasawa K: Riemann-Hurwitz formula and p-adic Galois representations for number fields Tohoku Math J (2) 33 (1981) ; Collected Papers [58] [Iw6] : (1993) [Ki] Kida Y: l-extensions of CM-fields and cyclotomic invariants J Number Theory 12 (1980) [Ku] Kurihara M: On the ideal class groups of the maximal real subfields of number fields with all roots of unity J European Math Soc 1 (1999) [NSW] Neukirch J Schmidt A Wingberg K: Cohomology of number fields Grundlehren der Mathematischen Wissenschaften 323 (2000) [SU] : (1998) [Wa] Washington LC: Introduction to cyclotomic fields 2nd edition GTM 83 Springer-Verlag New York (1997) [We1] Weil A: Courbes algébriques et variétés Abéliennes Hermann Paris (1971) [We2] Weil A: Basic Number Theory 3rd edition Grundlehren der Mathematischen Wissenschaften 144 Springer-Verlag New York-Berlin (1974) [Wi] Wingberg K: On the maximal unramified p-extension of an algebraic number field J Reine Angew Math 440 (1993) yhachi@mathgakushuinacjp 13
非可換Lubin-Tate理論の一般化に向けて
Lubin-Tate 2012 9 18 ( ) Lubin-Tate 2012 9 18 1 / 27 ( ) Lubin-Tate 2012 9 18 2 / 27 Lubin-Tate p 1 1 ( ) Lubin-Tate 2012 9 18 2 / 27 Lubin-Tate p 1 1 Lubin-Tate GL n n 1 Lubin-Tate ( ) Lubin-Tate 2012
0. I II I II (1) linear type: GL( ), Sp( ), O( ), (2) loop type: loop current Kac-Moody affine, hyperbolic (3) diffeo t
e-mail: [email protected] 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
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
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,
2 Riemann Im(s) > 0 ζ(s) s R(s) = 2 Riemann [Riemann]) ζ(s) ζ(2) = π2 6 *3 Kummer s = 2n, n N ζ( 2) = 2 2, ζ( 4) =.3 2 3, ζ( 6) = ζ( 8)
(Florian Sprung) p 2 p * 9 3 p ζ Mazur Wiles 4 5 6 2 3 5 2006 http://www.icm2006.org/video/ eighth session [ ] Coates [Coates] 2 735 Euler n n 2 = p p 2 p 2 = π2 6 859 Riemann ζ(s) = n n s = p p s s ζ(s)
17 Θ Hodge Θ Hodge Kummer Hodge Hodge
Teichmüller ( ) 2015 11 0 3 1 4 2 6 3 Teichmüller 8 4 Diophantus 11 5 13 6 15 7 19 8 21 9 25 10 28 11 31 12 34 13 36 14 41 15 43 16 47 1 17 Θ 50 18 55 19 57 20 Hodge 59 21 63 22 67 23 Θ Hodge 69 24 Kummer
2.1 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,
医系の統計入門第 2 版 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 第 2 版 1 刷発行時のものです.
医系の統計入門第 2 版 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. http://www.morikita.co.jp/books/mid/009192 このサンプルページの内容は, 第 2 版 1 刷発行時のものです. i 2 t 1. 2. 3 2 3. 6 4. 7 5. n 2 ν 6. 2 7. 2003 ii 2 2013 10 iii 1987
16 B
16 B (1) 3 (2) (3) 5 ( ) 3 : 2 3 : 3 : () 3 19 ( ) 2 ax 2 + bx + c = 0 (a 0) x = b ± b 2 4ac 2a 3, 4 5 1824 5 Contents 1. 1 2. 7 3. 13 4. 18 5. 22 6. 25 7. 27 8. 31 9. 37 10. 46 11. 50 12. 56 i 1 1. 1.1..
.5.1. G K O E, O E T, G K Aut OE (T ) (T, ρ). ρ, (T, ρ) T. Aut OE (T ), En OE (F ) p..5.. G K E, E V, G K GL E (V ) (V, ρ). ρ, (V, ρ) V. GL E (V ), En
p 1. 1.1., 01 8 3, 57,,.. 1.., Gal(Q p /Q p ), 1. Wach,,. 1.3. Part I,,. Part II, Part III. 1.4.., Paé. Part 1. p.. p p.1. p Q p p (Q p p )... E Q p, E p Z p E, O E. O E E. E Q p, O E. v p : E Q Q E, v
v v = v 1 v 2 v 3 (1) R = (R ij ) (2) R (R 1 ) ij = R ji (3) 3 R ij R ik = δ jk (4) i=1 δ ij Kronecker δ ij = { 1 (i = j) 0 (i
1. 1 1.1 1.1.1 1.1.1.1 v v = v 1 v 2 v 3 (1) R = (R ij ) (2) R (R 1 ) ij = R ji (3) R ij R ik = δ jk (4) δ ij Kronecker δ ij = { 1 (i = j) 0 (i j) (5) 1 1.1. v1.1 2011/04/10 1. 1 2 v i = R ij v j (6) [
, 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
Mazur [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
Part () () Γ Part ,
Contents a 6 6 6 6 6 6 6 7 7. 8.. 8.. 8.3. 8 Part. 9. 9.. 9.. 3. 3.. 3.. 3 4. 5 4.. 5 4.. 9 4.3. 3 Part. 6 5. () 6 5.. () 7 5.. 9 5.3. Γ 3 6. 3 6.. 3 6.. 3 6.3. 33 Part 3. 34 7. 34 7.. 34 7.. 34 8. 35
( ),, ( [Ka93b],[FK06]).,. p Galois L, Langlands p p Galois (, ) p., Breuil, Colmez([Co10]), Q p Galois G Qp 2 p ( ) GL 2 (Q p ) p Banach ( ) (GL 2 (Q
2017 : msjmeeting-2017sep-00f006 p Langlands ( ) 1. Q, Q p Q Galois G Q p (p Galois ). p Galois ( p Galois ), L Selmer Tate-Shafarevich, Galois. Dirichlet ( Dedekind s = 0 ) Birch-Swinnerton-Dyer ( L s
[AI] G. Anderson, Y. Ihara, Pro-l branched cov erings of P1 and higher circular l-units, Part 1 Ann. of Math. 128 (1988), 271-293 ; Part 2, Intern. J. Math. 1 (1990), 119-148. [B] G. V. Belyi, On Galois
meiji_resume_1.PDF
β β β (q 1,q,..., q n ; p 1, p,..., p n ) H(q 1,q,..., q n ; p 1, p,..., p n ) Hψ = εψ ε k = k +1/ ε k = k(k 1) (x, y, z; p x, p y, p z ) (r; p r ), (θ; p θ ), (ϕ; p ϕ ) ε k = 1/ k p i dq i E total = E
II (Percolation) ( 3-4 ) 1. [ ],,,,,,,. 2. [ ],.. 3. [ ],. 4. [ ] [ ] G. Grimmett Percolation Springer-Verlag New-York [ ] 3
II (Percolation) 12 9 27 ( 3-4 ) 1 [ ] 2 [ ] 3 [ ] 4 [ ] 1992 5 [ ] G Grimmett Percolation Springer-Verlag New-York 1989 6 [ ] 3 1 3 p H 2 3 2 FKG BK Russo 2 p H = p T (=: p c ) 3 2 Kesten p c =1/2 ( )
TOP URL 1
TOP URL http://amonphys.web.fc.com/ 3.............................. 3.............................. 4.3 4................... 5.4........................ 6.5........................ 8.6...........................7
13 0 1 1 4 11 4 12 5 13 6 2 10 21 10 22 14 3 20 31 20 32 25 33 28 4 31 41 32 42 34 43 38 5 41 51 41 52 43 53 54 6 57 61 57 62 60 70 0 Gauss a, b, c x, y f(x, y) = ax 2 + bxy + cy 2 = x y a b/2 b/2 c x
18 I ( ) (1) I-1,I-2,I-3 (2) (3) I-1 ( ) (100 ) θ ϕ θ ϕ m m l l θ ϕ θ ϕ 2 g (1) (2) 0 (3) θ ϕ (4) (3) θ(t) = A 1 cos(ω 1 t + α 1 ) + A 2 cos(ω 2 t + α
18 I ( ) (1) I-1,I-2,I-3 (2) (3) I-1 ( ) (100 ) θ ϕ θ ϕ m m l l θ ϕ θ ϕ 2 g (1) (2) 0 (3) θ ϕ (4) (3) θ(t) = A 1 cos(ω 1 t + α 1 ) + A 2 cos(ω 2 t + α 2 ), ϕ(t) = B 1 cos(ω 1 t + α 1 ) + B 2 cos(ω 2 t
k + (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)
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
2016 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
006 11 8 0 3 1 5 1.1..................... 5 1......................... 6 1.3.................... 6 1.4.................. 8 1.5................... 8 1.6................... 10 1.6.1......................
1.2 (Kleppe, cf. [6]). C S 3 P 3 3 S 3. χ(p 3, I C (3)) 1 C, C P 3 ( ) 3 S 3( S 3 S 3 ). V 3 del Pezzo (cf. 2.1), S V, del Pezzo 1.1, V 3 del Pe
3 del Pezzo (Hirokazu Nasu) 1 [10]. 3 V C C, V Hilbert scheme Hilb V [C]. C V C S V S. C S S V, C V. Hilbert schemes Hilb V Hilb S [S] [C] ( χ(s, N S/V ) χ(c, N C/S )), Hilb V [C] (generically non-reduced)
構造と連続体の力学基礎
II 37 Wabash Avenue Bridge, Illinois 州 Winnipeg にある歩道橋 Esplanade Riel 橋6 6 斜張橋である必要は多分無いと思われる すぐ横に道路用桁橋有り しかも塔基部のレストランは 8 年には営業していなかった 9 9. 9.. () 97 [3] [5] k 9. m w(t) f (t) = f (t) + mg k w(t) Newton
4. ϵ(ν, T ) = c 4 u(ν, T ) ϵ(ν, T ) T ν π4 Planck dx = 0 e x 1 15 U(T ) x 3 U(T ) = σt 4 Stefan-Boltzmann σ 2π5 k 4 15c 2 h 3 = W m 2 K 4 5.
A 1. Boltzmann Planck u(ν, T )dν = 8πh ν 3 c 3 kt 1 dν h 6.63 10 34 J s Planck k 1.38 10 23 J K 1 Boltzmann u(ν, T ) T ν e hν c = 3 10 8 m s 1 2. Planck λ = c/ν Rayleigh-Jeans u(ν, T )dν = 8πν2 kt dν c
24 I ( ) 1. R 3 (i) C : x 2 + y 2 1 = 0 (ii) C : y = ± 1 x 2 ( 1 x 1) (iii) C : x = cos t, y = sin t (0 t 2π) 1.1. γ : [a, b] R n ; t γ(t) = (x
24 I 1.1.. ( ) 1. R 3 (i) C : x 2 + y 2 1 = 0 (ii) C : y = ± 1 x 2 ( 1 x 1) (iii) C : x = cos t, y = sin t (0 t 2π) 1.1. γ : [a, b] R n ; t γ(t) = (x 1 (t), x 2 (t),, x n (t)) ( ) ( ), γ : (i) x 1 (t),
1 9 v.0.1 c (2016/10/07) Minoru Suzuki T µ 1 (7.108) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1)
1 9 v..1 c (216/1/7) Minoru Suzuki 1 1 9.1 9.1.1 T µ 1 (7.18) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1) E E µ = E f(e ) E µ (9.1) µ (9.2) µ 1 e β(e µ) 1 f(e )
http://www.ike-dyn.ritsumei.ac.jp/ hyoo/wave.html 1 1, 5 3 1.1 1..................................... 3 1.2 5.1................................... 4 1.3.......................... 5 1.4 5.2, 5.3....................
all.dvi
72 9 Hooke,,,. Hooke. 9.1 Hooke 1 Hooke. 1, 1 Hooke. σ, ε, Young. σ ε (9.1), Young. τ γ G τ Gγ (9.2) X 1, X 2. Poisson, Poisson ν. ν ε 22 (9.) ε 11 F F X 2 X 1 9.1: Poisson 9.1. Hooke 7 Young Poisson G
図 : CGC 回転面. 左の図は 正の場合の平行曲面として得られる平均曲率 一定回転面 ダラネーアンデュロイド 上 とノドイド 下, 中の図は その平行正 CGC 回転面 右の図は負 CGC 回転面 ミンディング曲面と呼 ばれる 図 2: 回転面でない位相的な円柱面 螺旋対称性を持つ. ダラネー
[email protected] (K ) Nick Schmitt (Tübingen ) [6] R 3 K CGC [], R 3 CGC, R 3 CGC CGC CGC CGC 2, [2]. CGC CGC [6] C 3 CGC [4] CGC. 図 : CGC 回転面. 左の図は 正の場合の平行曲面として得られる平均曲率 一定回転面 ダラネーアンデュロイド 上
S K(S) = T K(T ) T S K n (1.1) n {}}{ n K n (1.1) 0 K 0 0 K Q p K Z/pZ L K (1) L K L K (2) K L L K [L : K] 1.1.
() 1.1.. 1. 1.1. (1) L K (i) 0 K 1 K (ii) x, y K x + y K, x y K (iii) x, y K xy K (iv) x K \ {0} x 1 K K L L K ( 0 L 1 L ) L K L/K (2) K M L M K L 1.1. C C 1.2. R K = {a + b 3 i a, b Q} Q( 2, 3) = Q( 2
KENZOU
KENZOU 2008 8 2 3 2 3 2 2 4 2 4............................................... 2 4.2............................... 3 4.2........................................... 4 4.3..............................
n ξ n,i, i = 1,, n S n ξ n,i n 0 R 1,.. σ 1 σ i .10.14.15 0 1 0 1 1 3.14 3.18 3.19 3.14 3.14,. ii 1 1 1.1..................................... 1 1............................... 3 1.3.........................
微分積分 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 初版 1 刷発行時のものです.
微分積分 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. ttp://www.morikita.co.jp/books/mid/00571 このサンプルページの内容は, 初版 1 刷発行時のものです. i ii 014 10 iii [note] 1 3 iv 4 5 3 6 4 x 0 sin x x 1 5 6 z = f(x, y) 1 y = f(x)
数学Ⅱ演習(足助・09夏)
II I 9/4/4 9/4/2 z C z z z z, z 2 z, w C zw z w 3 z, w C z + w z + w 4 t R t C t t t t t z z z 2 z C re z z + z z z, im z 2 2 3 z C e z + z + 2 z2 + 3! z3 + z!, I 4 x R e x cos x + sin x 2 z, w C e z+w
H.Haken Synergetics 2nd (1978)
27 3 27 ) Ising Landau Synergetics Fokker-Planck F-P Landau F-P Gizburg-Landau G-L G-L Bénard/ Hopfield H.Haken Synergetics 2nd (1978) (1) Ising m T T C 1: m h Hamiltonian H = J ij S i S j h i S
X G P G (X) G BG [X, BG] S 2 2 2 S 2 2 S 2 = { (x 1, x 2, x 3 ) R 3 x 2 1 + x 2 2 + x 2 3 = 1 } R 3 S 2 S 2 v x S 2 x x v(x) T x S 2 T x S 2 S 2 x T x S 2 = { ξ R 3 x ξ } R 3 T x S 2 S 2 x x T x S 2
I A A441 : April 21, 2014 Version : Kawahira, Tomoki TA (Kondo, Hirotaka ) Google
I4 - : April, 4 Version :. Kwhir, Tomoki TA (Kondo, Hirotk) Google http://www.mth.ngoy-u.c.jp/~kwhir/courses/4s-biseki.html pdf 4 4 4 4 8 e 5 5 9 etc. 5 6 6 6 9 n etc. 6 6 6 3 6 3 7 7 etc 7 4 7 7 8 5 59
Note.tex 2008/09/19( )
1 20 9 19 2 1 5 1.1........................ 5 1.2............................. 8 2 9 2.1............................. 9 2.2.............................. 10 3 13 3.1.............................. 13 3.2..................................
compact 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
N/m f x x L dl U 1 du = T ds pdv + fdl (2.1)
23 2 2.1 10 5 6 N/m 2 2.1.1 f x x L dl U 1 du = T ds pdv + fdl (2.1) 24 2 dv = 0 dl ( ) U f = T L p,t ( ) S L p,t (2.2) 2 ( ) ( ) S f = L T p,t p,l (2.3) ( ) U f = L p,t + T ( ) f T p,l (2.4) 1 f e ( U/
Shunsuke Kobayashi 1 [6] [11] [7] u t = D 2 u 1 x 2 + f(u, v) + s L u(t, x)dx, L x (0.L), t > 0, Neumann 0 v t = D 2 v 2 + g(u, v), x (0, L), t > 0. x
Shunsuke Kobayashi [6] [] [7] u t = D 2 u x 2 + fu, v + s L ut, xdx, L x 0.L, t > 0, Neumann 0 v t = D 2 v 2 + gu, v, x 0, L, t > 0. x2 u u v t, 0 = t, L = 0, x x. v t, 0 = t, L = 0.2 x x ut, x R vt, x
i 18 2H 2 + O 2 2H 2 + ( ) 3K
i 18 2H 2 + O 2 2H 2 + ( ) 3K ii 1 1 1.1.................................. 1 1.2........................................ 3 1.3......................................... 3 1.4....................................
,. Black-Scholes u t t, x c u 0 t, x x u t t, x c u t, x x u t t, x + σ x u t, x + rx ut, x rux, t 0 x x,,.,. Step 3, 7,,, Step 6., Step 4,. Step 5,,.
9 α ν β Ξ ξ Γ γ o δ Π π ε ρ ζ Σ σ η τ Θ θ Υ υ ι Φ φ κ χ Λ λ Ψ ψ µ Ω ω Def, Prop, Th, Lem, Note, Remark, Ex,, Proof, R, N, Q, C [a, b {x R : a x b} : a, b {x R : a < x < b} : [a, b {x R : a x < b} : a,
0. Intro ( K CohFT etc CohFT 5.IKKT 6.
E-mail: [email protected] 0. Intro ( K 1. 2. CohFT etc 3. 4. CohFT 5.IKKT 6. 1 µ, ν : d (x 0,x 1,,x d 1 ) t = x 0 ( t τ ) x i i, j, :, α, β, SO(D) ( x µ g µν x µ µ g µν x ν (1) g µν g µν vector x µ,y
数学の基礎訓練I
I 9 6 13 1 1 1.1............... 1 1................ 1 1.3.................... 1.4............... 1.4.1.............. 1.4................. 3 1.4.3........... 3 1.4.4.. 3 1.5.......... 3 1.5.1..............
No δs δs = r + δr r = δr (3) δs δs = r r = δr + u(r + δr, t) u(r, t) (4) δr = (δx, δy, δz) u i (r + δr, t) u i (r, t) = u i x j δx j (5) δs 2
No.2 1 2 2 δs δs = r + δr r = δr (3) δs δs = r r = δr + u(r + δr, t) u(r, t) (4) δr = (δx, δy, δz) u i (r + δr, t) u i (r, t) = u i δx j (5) δs 2 = δx i δx i + 2 u i δx i δx j = δs 2 + 2s ij δx i δx j
