Broadhurst-Kreimer Brown ( D3) 1 Broadhurst-Kreimer Zagier Gangl- -Zagi
|
|
- みりあ ほうねん
- 5 years ago
- Views:
Transcription
1 Broadhurst-Kreimer Brown ( D3) 1 Broadhurst-Kreimer Zagier Gangl- -Zagier GKZ Brown Brown Lie Brown ,, Broadhurst-Kreimer ( 97). Broadhurst-Kreimer, Zagier ( 94),., SL 2 (Z), Broadhurst-Kreimer.,., Gangl,, Zagier GKZ,, Brown (exceptional element)., Lie 1
2 ., Brown. Brown, Q (totally odd MZV), Lie, Lie,., Brown. Brown,, ( ). Brown, - -Zagier( 06) (linearized double shuffle space) Lie., 1 Broadhurst-Kreimer,. 2,, Brown, - -Zagier. Brown, 3 Brown, Gangl- -Zagier ( GKZ ). 4, Lie, Lie Brown., Brown, 2, 3. 1 Broadhurst-Kreimer, Zagier [23]., Broadhurst- Kreimer[5]., Broadhurst-Kreimer. 1. n = ( 1,..., n ), ζ() = ζ( 1,..., n ) = m 1 > >m n >0 1. m 1 1 m n n wt() = n, dep() = n., 1 > 1., Zagier. 2
3 Zagier Q Z, {d } 0 1/(1 t 2 t 3 ) = d t., Z (n) dim Q Z? = d. Zagier, d ([21, 8] ), {ζ( 1,..., n ) i {2, 3}} Z ([2, 3], Hoffman ).,, Q Galois Gronthendiec-Teichmüller. (, [6].) Broadhurst-Kreimer,., n ( 1) Q Z (n) : := ζ() wt() =, dep() n Q, Z (n) 0 := Q. n,. Broadhurst-Kreimer, Z (n) /Z(n 1) ( ). E(s), O(s), S(s) : E(s) = s2 s3, O(s) = 1 s2 1 s, S(s) = s 12 2 (1 s 4 )(1 s 6 ). {d,n },n 0.,n 0 d,n s t n = 1 + E(s)t 1 O(s)t + S(s)t 2 S(s)t (Broadhurst-Kreimer vector space ver. ) > n > 0, d,n =? dim Q Z (n) /Z(n 1). d,n n\
4 2, (bigraded algebra) (algebra generator). (graded algebra) Z, augumentation I. Z := Z (n), Z := Z, I = Z. >n>0 0 1 Z (filtered algebra) {0} = Z (0) Z (1)... Z (n) Z ( Z (n) := 0 Z (n) )., T := I/I 2, (cotangent space) T,., M ( :[15, p.14]): M :=,n>0,n>0 M (n), M(n) := T (n) /T (n 1) (n) = Z /(Z(n 1) + Z (n) I 2 ). {D,n },n>0. ( ) D,n 1 1 = 1 s t n 1 O(s)t + S(s)t 2 S(s)t (Broadhurst-Kreimer algebra generator ver. ) > n > 0 (, (, n) (2, 1)), D?,n = dim Q M (n). D,n n\ : D,n log, D,n n = 2, 3, 4,. ( :[12]) M (n) D,2 s s 8 = (1 s 2 )(1 s 6 ), D,3 s s 11 (1 + s 2 s 4 ) = (1 s 2 )(1 s 4 )(1 s 6 ), >0 >0 D,4 s = s12 (1 + 2s 4 + s 6 + s 8 + 2s 10 + s 14 s 16 ). (1 s 2 )(1 s 6 )(1 s 8 )(1 s 12 ) >0 ( 4 ) 4
5 n\ ζ(2) ζ(3) ζ(5) ζ(7) ζ(9) ζ(11) ζ(13) 2 ζ(3, 5) ζ(3, 7) ζ(3, 9) 3 ζ(3, 3, 5) 4 ζ(4, 4, 2, 2) ζ(15) ζ(17) ζ(19) ζ(3,11) ζ(5,9) ζ(3, 3, 3, 5) ζ(3,3,9) ζ(3,5,7) ζ(3,13) ζ(5,11) ζ(3,3,3,7) ζ(3,3,5,5) ζ(4,4,2,6) ζ(3,3,11),ζ(3,5,9) ζ(3,7,7),ζ(5,5,7) ζ(3,15) ζ(5,13) ζ(3,3,3,9),ζ(3,3,5,7) ζ(3,5,5,5),ζ(3,5,3,7) ζ(4,8,4,2) ζ(3,3,13),ζ(3,5,11) ζ(3,7,9),ζ(5,5,9) ζ(5,7,7) ζ(3,5,5) ζ(3,3,7) ζ(3,17) ζ(5,15) ζ(7,13) 2 - -Zagier, (double shuffle relations) Broadhurst-Kreimer - -Zagier [13].,., dim M (n) (linearized double shuffle space),. 2.1,.,. [1] [13] ( [1] ).,,.,, : r + s = (r > s 1), ζ(r)ζ(s) = ζ(r, s) + ζ(s, r) + ζ(), (1) ζ(r)ζ(s) = (( ) ( )) i 1 i 1 + ζ(i, j). r 1 s 1 i+j= i,j 1 ( a,b>0 = a>b>0 + b>a>0 + a=b>0 ) ( ). 5
6 , s = 1,,., ζ(1) := 0 ζ(1, r) := ζ(r, 1) ζ(r + 1)., ( ) (Hoffman [11], [1, 1.4] ). x, y Q ( ) H, H 1, H 0 : H := Q x, y H 1 := Q + Hy H 0 := Q + xhy. H 0. Q- Z : H 0 R Z(x 1 1 y x n 1 y) = ζ( 1,..., n ) 1., Z(1) = 1. H 0. : Q- : H 1 H 1 H 1 z := x 1 y, w, w H 1, z w z l w = z (w z l w ) + z l (z w w ) + z +l (w w ),., 1. H 1 H 1 = Q z 1, z 2,.... H 0., Hoffman[11] (i.e. Z(w w ) = Z(w)Z(w )). : Q- x : H H H w, w H u, v {x, y}, uw x vw = u(w x vw ) + v(uw x w ),., 1 x., x H 0, (i.e. Z(w x w ) = Z(w)Z(w )). : Q Z H 1 R[T ]. {, x}, H 1, H 0., Q Z : H 1 R[T ], ([1, 1.4.3]): Z H 0 = Z, Z (y) = T., H 1 = H 0 [y], w H 1 w = w 0 + w 1 y + w n y n (w 0, w 1,..., w n H 0 )., Z (w) = Z(w 0 ) + Z(w 1 )T + + Z(w n )T n. 1 x = dt/t, y = dt/(1 t) 0 1 ( ). 6
7 4. ( [13]) w 0 H 0, w 1 H 1 Z (w 0 w 1 w 0 x w 1 ) = 0., T Z reg = Z T =0. Z reg(w 0 w 1 w 0 x w 1 ) = 0. Proof.. R ρ : R[T ] R[T ]( [1, 1.4.6]). ρ(exp(t u)) = exp ( ( 1) n n ζ(n)un) exp(t u). n>1, Z x = ρ Z ( ). w 1 H 1 w 0 H 0, ρ R.. 0 = Z(w 0 )Z x (w 1 ) Z(w 0 )ρ(z (w 1 )) = Z x (w 0 x w 1 ) ρ(z (w 0 w 1 )) = Z x (w 0 w 1 w 0 x w 1 ). 5. y n w 1 H 1, Z reg(w 1 ) Z x reg(w 1 ) (mod Z (n 1) + Z (n) I 2 ). Proof. w 1, : w 1 = v 0 + v 1 y + + v n y n (v i H 0 ). v i y n i., ρ(t i ) Q[ζ() 2] T i, i, ρ(z (w 1 )) = Z reg(w 1 ) + Z(v 1 )ρ(t ) + + Z(v n )ρ(t n ) Z reg(w 1 ) mod Z (n 1) + Z (n) I 2 : Z x reg(w 1 ) = Z x (w 1 ) T =0 = ρ(z (w 1 )) T =0 Z reg(w 1 ) (mod Z (n 1) + Z (n) I 2 ). ( : i 2, ρ(t i ), v i 0 i 2 ρ(z (w 1 )) T =0 Z reg(w 1 )., 2 (ρ(t i ) (i 2) ), ρ(z (w 1 )) T =0 = Z reg(w 1 ).) 7
8 2.2, M Q., M n n.,,,,., M (n). Z (n) /(Z(n 1) +Z (n) I 2 ) :, (1), M (2).. F2 (x 1, x 2 ) := Zreg(z 1 z 2 )x x 2 1 2,, F x 2 (x 1, x 2 ) := 1, 2 >0 1, 2 >0 Z x reg(z 1 z 2 )x x F 2 (x 1, x 2 ) = ζ(2) 2 +ζ(2, 1)x 1+( ζ(2, 1) ζ(3))x 2 +ζ(2, 2)x 1 x 2 +( ζ(3, 1) ζ(4))x (i) F 2 (x 1, x 2 ) = F x 2 (x 1, x 2 ), (ii) 0 F 2 (x 1, x 2 ) + F 2 (x 2, x 1 ) 1, 2 >0 F x 2 (x 1 + x 2, x 2 ) + F x 2 (x 1 + x 2, x 1 ) (mod Z (1) + Z (2) I 2 ). Proof. 5., (1)., 0 Zreg(z 1 z 2 )x x Zreg(z 1 z 2 + z 2 z 1 )x x 2 1 2, 0 1, 2 >0 = 1, 2 >0 = i,j>0 Z x reg(z 1 i+j= i,j>0 x z 2 )x x , 2 >0 (( ) ( )) i 1 i 1 + Z x reg(z i z j )x x Z x reg(z i z j ) ( (x 1 + x 2 ) i 1 x j (x 1 + x 2 ) i 1 x j 1 1 ). 8
9 6, mod Z (1) + Z (2) I 2, Q f(x 1, x 2 ) : 0 = f(x 1, x 2 ) + f(x 2, x 1 ) = f(x 1 + x 2, x 2 ) + f(x 1 + x 2, x 1 ). (2) (2), Q[x 1, x 2 ] DSh 2, d Q DSh 2 (d). 7. 2, DSh 2 := {f(x 1, x 2 ) Q[x 1, x 2 ] f satisfy (2)}. dim M (2) dim DSh 2 ( 2). Proof. DSh 2 ( 2), q 1,..., q g (g = dim DSh 2 ( 2)). 6, F2 (x 1, x 2 ) M (2) DSh 2, ζ i M (2), (F 2 (x 1, x 2 ) 2 ) = ζ 1 q ζ g q g. ζ 1,..., ζ g,. Remar. - -Zagier, dim DSh 2 ( 2) = D,2., Broadhurst-Kreimer n = 2 2.,, DSh n Broadhurst-Kreimer. n :. n 2, Q[x 1,..., x n ] sh (n) l Z[GL n (Q)] (1 l n 1) : f(x 1,..., x n ) (n) sh l := f(x σ 1 (1),..., x σ 1 (n)). σ S n σ(1)<...<σ(l) σ(l+1)<...<σ(n) ( ),., w 1,..., w n, ([18] ): w 1 w l x w l+1 w n = w σ 1 (1) w σ 1 (n). (3) σ S n σ(1)<...<σ(l) σ(l+1)<...<σ(n), f (x 1,..., x n ) := f(x x n,..., x n 1 + x n, x n ). n ( {, x}): Fn(x 1,..., x n ) := Zreg(z 1 z n )x x n 1 n. ( 1,..., n) N n 2, D,n Broadhurst- Kreimer. 9
10 8. n > 1 l {1,..., n 1},. (i) Fn Fn x (mod Z (n 1) + Z (n) I 2 ), (ii) 0 Fn (n) sh l (Fn x ) (n) sh l (mod Z (n 1) + Z (n) I 2 ). Proof. 5., 0 Z reg(z 1 z l z l+1 z n ) (mod Z (n) I 2 ) Z reg(z 1 z l x z l+1 z n ) (mod Z (n 1) + Z (n) I 2 ), (3) Fn (n) sh l 0.,, z 1 z l x z l+1 z n.,, 0 = (Fl x ) (x 1,..., x l ) (Fn l) x (x l+1,..., x n ) = (Fn x ) (x 1,..., x n ) (n) sh l ( :[13], [12, Proposition 9]). 9. n n > 1, DSh n := {f Q[x 1,..., x n ] f sh (n) l, d DSh n (d). 7,. 10. ( - -Zagier [13]) > n > 1, dim M (n) = f sh (n) l = 0 (1 l n 1)}. dim DSh n ( n). Remar. dim DSh n ( n) D,n, Broadhurst-Kreimer., DSh n (d). DSh n (d), Goncharov [10] GL n (Z), - [14] B d > 0 n > 0, DSh n (d) = {0} ([13, Prop. 17]). d > 0,. [ ] d dim DSh 2 (d) = = D d+2,2 ([10],[13, Prop. 18]), 6 [ ] d 2 1 dim DSh 3 (d) = = D d+3,3 ([10, 14])
11 3 Gangl- -Zagier Broadhurst-Kreimer (Zagier [23, 8], [24, 3] ), dim Q Z (2)? = 2 1 dim S (SL 2 (Z)) ( : even)., (GKZ ).,.,, GKZ. 3.1,, ( Gangl- -Zagier[7] ). F (X, Y ) GL 2 (Z), Z[GL 2 (Z)] : F (X, Y ) ( a b c d ) = F (ax + by, cx + dy )., GL 2 (Z). ( ) ( ) S =, T =, ε = ( ) ( 0 1, δ = , F (X, Y ) ε = F (Y, X), F (X, Y ) δ = F ( X, Y )., W : W := er(1 T t T ) (= {P (X, Y ) Q[X, Y ] P (X, Y ) (1 T t T ) = 0})., d W (d). PGL 2 (Z), (1 T t T )S = (1 + S) (1 + T S + (T S) 2 ). PSL 2 (Z) S T, P W G = P (1 + S) = P (1 + T S + (T S) 2 ), G SL 2 (Z), G 0., P (1 + S) = 0.,, W = er(1 + S) er(1 + T S + (T S) 2 )., ε(t S)ε = (T S) 2 P ε = P δ W. W ε ±1 W ± ( t T = εt ε): W ± = er(1 T T ε). : P W P δ = P,. ). 11
12 , W = er(1 + S) er(1 + T S + (T S) 2 )., f(z), n-th r n (f) r n (f) = 0 f(it)t n dt ( : f L- r n (f) = n!/(2π) n+1 L(n + 1, f)), : P f (X, Y ) = i 0 f(z)(x zy ) 2 dz. (f ), P f (X, Y ) γ = γ 1 (i ) f(z)(x zy ) 2 dz, SL γ 1 (0) 2 (Z) S, T S, P f (X, Y ) (1 + S) = Pf (X, Y ) (1 + T S + (T S) 2 ) = 0. P f (X, Y ), Q., P f (X, Y ) (1 + S) = 0 rn (f) = ( 1) n r 2 n (f). P f (X, Y ), P f (X, Y ) ( ) HP 1 (SL 2(Z), V Q C), SL 2 (Z)., V 2 ; V = Q[X, Y ] ( 2). f S (SL 2 (Z)), Z[SL 2 (Z)]- φ f : SL 2 (Z) V Q C φ f (γ) = γ 1 (i ) f(z)(x zy ) 2 dz, φ i f HP 1 (SL 2(Z), V Q C). ( φ f (γ 1 γ 2 ) = φ f (γ 1 ) γ2 + φ f (γ 2 ).) φ f, φ f (S) = P f (X, Y ) W ( 2), S 2 = (T S) 3 = 1 (PSL 2 (Z) ) φ f (S) W. ( [17, 19].) 12. (Eichler- -Manin [16]), r + : S (SL 2 (Z)) W + ( 2) Q C, f P f (X, Y ) (1 + δ), r : S (SL 2 (Z)) W ( 2) Q C, f P f (X, Y ) (1 δ) 1. Remar. W (d) Q(X d Y d )., W (d) = 12
13 W,0 (d) Q(X d Y d ), W,0 (d) d W,0. W,0 = d>0 W,0 (d). 3.2 GKZ Gangl- -Zagier[7] GKZ.,. 13. (Gangl- -Zagier [7]) P (X, Y ) W ( 2), q r,s. P (X + Y, Y ) = ( ) 2 q r,s X r 1 Y s 1. r 1,. r+s= r,s odd r+s= r,s 1 q r,s ζ(r, s) 0 (mod Qζ()). 1. X 2 Y 8 3X 4 Y 6 + 3X 6 Y 4 X 8 Y 2 W (10). GKZ-, 14ζ(9, 3) + 75ζ(7, 5) + 84ζ(5, 7) 0 (mod Qζ(12)). 13. D, Z, Z r,s (r+s =, r, s 1) Q,. Z r,s + Z s,r + Z = (( ) ( )) i 1 i 1 + Z i,j. (4) r 1 s 1 i+j= ( i+j= i, j 1.), D = Z, Z r,s r + s = Q. (relation (4)) 14. a r,s,. (i) D,. a r,s Z r,s 0 (mod QZ ). r+s= (ii) 2 H(X, Y ) er(1 ε, V ),. H(X, Y ) ( t T 1) = ( ) 2 a r,s X r 1 Y s 1. r 1 r+s= 13
14 Proof. er(1 ε, V ) H r,s (X, Y ) = ( 2 r 1) (X r 1 Y s 1 +X s 1 Y r 1 ) (r+s = ), H r,s ( t T 1)., ( 2 r 1) X r 1 (X+Y ) s 1 = ( 2 )( i 1 ) i+j= i 1 r 1 X i 1 Y j 1, Z r,s + Z s,r (( ) ( )) i 1 i 1 + Z i,j (mod QZ ) r 1 s 1 i+j=. D (4),. 15. q r,s q r,s = q s,r (r, s : even).,. (i) D,. q r,s Z r,s 3 q r,s Z r,s (mod QZ ). r+s= r,s even r+s= r,s odd (ii) P (X, Y ) W ( 2),. P (X, Y ) ( ) 2 T = q r,s X r 1 Y s 1. r 1 r+s= Proof. (ii) (i). P (X, Y ) = ( 2 r+s= r 1) pr,s X r 1 Y s 1 W ( 2), Q(X, Y ) = P (X, Y ) T. Q (1 ε) = P (T T ε) = P, q r,s q s,r = { pr,s r, s : odd, 0 r, s : even. (5), Q δ Q = Q ev + Q od, Q ev er(1 δ, V ), Q od er(1 + δ, V ). Q od (5), (i.e. Q od er(1 ε, V )). Q ev (5), Q ev = ( ) 2 (p r,s + q s,r )X r 1 Y s 1 = P + Q ev ε (6) r 1 r+s=., Q ev ε Q ev = Q ev,+ + Q ev,, Q ev,± er(1 ε), (6) 2Q ev, = P., 14, (i) F, F 2Q ev,+ 2Q od ( )., 2Q ev, t T = P t T = P T ε = Q ε = Q ev,+ + Q ev, Q od, (Q ev,+ Q ev, Q od ) t T = Q S t T = P T S t T = P S = P = 2Q ev,, (2Q ev,+ 2Q od ) t T = Q ev,+ 3Q ev, Q od, (2Q ev,+ 2Q od ) ( t T 1) = Q od 3Q ev. 14
15 15, Z r,s ζ(r, s), 15 (i), q r,s = q s,r ζ(r)ζ(s) (r + s =, r, s even) ζ() ( )., GKZ ( 13). 4 Brown DSh DSh := n>0 DSh n = DSh n (d)., DSh 1 := d>0 Qx2d 1. 2, Broadhurst-Kreimer DSh n ( n) D,n. Brown [4], DSh Lie.,. d,n>0 4.1, DSh Lie., DSh., Brown ( [4] ). Q-. : Q[y 0,..., y r ] Q Q[y 0,..., y s ] Q[y 0,..., y r+s ] f(y 0,..., y r ) g(y 0,..., y s ) f g(y 0,..., y r+s ), f g(y 0,..., y r+s ) = s deg f+r ( 1) s f(y i, y i+1,..., y i+r )g(y 0,..., y }{{} i, y i+r+1,..., y r+s )+ }{{} i+1 s i i=0 i=1, : f(y i+r,..., y i+1, y i )g(y 0,..., y }{{ i 1, y } i+r,..., y r+s ). }{{} i s i+1 {f, g} = f g(0, x 1,..., x r+s ) g f(0, x 1,..., x r+s ) 16. (Goncharov-Racinet-Brown) DSh {, }, Lie (bigraded Lie algebra). 15
16 , {, }, Jacobi, f i DSh ni (d i ), {f 1, f 2 } DSh n1 +n 2 (d 1 + d 2 )., {x 2n 1 1, x 2n 2 1 } = (x 2n 1 = x 2n x 2n 2 2 x 2n 2 1 x 2n 1 ( x 2n 2 2 (x 2 x 1 ) ) 2n 2 + (x 2 x 1 ) ( 2n 1 x 2n 2 1 x 2n ) (1 T + T ε), (7) ) + x 2n 1 ( 2 (x2 x 1 ) 2n 2 ) x 2n Brown Lie DSh, Lie. DSh (DSh/{DSh, DSh} = DSh ab ), DSh Lie A. A := Lie Q [x 2 1, x 4 1, x 6 1,...]. Lie A n ( x 2m 1 (m = 1, 2,...) n 1 ), d A A n (d).. A n (d) DSh n (d). (8) 2. n = 2 : A 2 (4) = {0}, A 2 (6) = Q{x 2 1, x 4 1}, A 2 (8) = Q{x 2 1, x 6 1}, A 2 (10) = Q{x 2 1, x 8 1} + Q{x 4 1, x 6 1}, A 2 (12) = Q{x 2 1, x 10 1 } + Q{x 4 1, x 8 1}. Lie A Lie., A ( -, Schneps[20]) d > 0, a n1,n 2 a n1,n 2 {x 2n 1 1, x 2n 2 1 } = 0 2n 1 +2n 2 =d n 1 >n 2 >0, a n1,n 2 (X 2n 1 Y 2n 2 X 2n 2 Y 2n 1 ) W,0 (d). 2n 1 +2n 2 =d n 1 >n 2 >0 Proof. (7). 0 W,0 DSh 1 DSh 1 A 2 0., DSh 1 DSh 1 n 1,n 2 >0 Q(x2n 1 1 x 2n 2 2 x 2n 2 1 x 2n 1 2 ). 3. 1, (X 2 Y 8 X 8 Y 2 ) 3(X 4 Y 6 X 6 Y 4 ) W (10)., (7) {x 2 1, x 8 1} 3{x 4 1, x 6 1} = 0. 16
17 dim A 4 (8) = 0, dim DSh 4 (8) = 1., A DSh, Brown [4], A DSh Lie,.. p(x, Y ) W,0. p(x, Y ) XY (X Y ). p 0 (X, Y ), p 1 (X, Y ) : p 0 (X, Y ) = p(x, Y )/XY (X Y ), p 1 (X, Y ) = p(x, Y )/XY. 18. p(x, Y ) W,0, e p (y 0,..., y 4 ) := ( p1 (y σ(4) y σ(3), y σ(2) y σ(1) ) + (y σ(0) y σ(1) )p 0 (y σ(2) y σ(3), y σ(4) y σ(3) ) ), σ Z/5Z e p (x 1,..., x 4 ) := e p (0, x 1,..., x 4 ). σ. 19. (Brown[4]) d > 0,. e : W,0 (d) DSh 4 (d 2) p(x, Y ) e p (x 1,..., x 4 ). DSh DSh 1 Lie, 19 Brown (Brown exceptional element, ), DSh Brown., Brown DSh Lie,. 20. DSh. H 1 (DSh, Q) = DSh 1 e(w,0 ) H 2 (DSh, Q) = W,0 H i (DSh, Q) = 0 (i 3). Remar. Brown 20, 19 DSh 4 DSh Lie W, DSh? = A W ( W := Lie Q (e(w,0 )) ),, DSh 17 A 2., 20, DSh n ( n), D,n ( [4] ). 17
18 4.3 Brown, , A,. 21. >n>0 ( 1 ) dim An( n)? = 1 s t n 1 1 O(s)t + S(s)t 2. (9), ζ( 1,..., n ) x x n 1 n, A 3 ζ(2l 1 + 1,..., 2l n + 1) (l i 1)( ) Z A 3., (9). Brown.,., n Z O (n). O (n) n (mod 2),. O (n) O (n 1) := ζ() Z (n) i 3 : odd Q. = O (n 2) O (n 3) = O (n 4). ζ(2) Z (ζ(2))., Z,n odd,, n, n 1, (ζ(2)). Z odd,n = O (n) /(Z(n 1) O (n) + (ζ(2)) O (n) ). 22. (Brown ). 1 + >n>0 dim Z odd,n s t n? = 1 1 O(s)t + S(s)t 2., 21, 22,. n = 2 ( ) : 21, [ ] 2 dim A 2 ( 2) = ( : even) 6 3, 1 M (n)., ( 19). 18
19 . A Lie, Poincaré-Birhoff-Witt ([22, p226]) ( ) dim An ( n) 1 1 s = 1 s t n 1 s(st + 1) >n>0, t 2 dim A 2 ( 2) = [( 4)/4] ( : even)., 17, A 2 ( 2) dim W,0 ( 2) = dim S (SL 2 (Z)) = [( 4)/4] [( 2)/6], 12,17 (8), A 2 = DSh 2 : [ ] [ ] 4 2 dim A 2 ( 2) = dim S (SL 2 (Z)) = = dim DSh 2 ( 2). 4 6 n = 3 ( ) : Brown [4], Goncharov A 3 = DSh 3., A 3 (12), (Jacobi ){x 2 1, {x 2 1, x 8 1} 3{x 4 1, x 6 1}} = 0. n = 2 ( ) : 22,. dim Q Z odd,2? = 2 2 dim S (SL 2 (Z))., Z odd,2 = ζ(2i + 1, 2i 1) 1 i /2 1 Q/ π Q, GKZ ( 13) dim S (SL 2 (Z)),. dim Q Z odd,2 2 2 dim S (SL 2 (Z)). n = 3 ( ) : 22, dim Q Z,3 odd s =? O(s) 3 2O(s)S(s). >0, 15 ( )., 1 GKZ ζ(3)., 14(ζ(3, 9, 3) + 2ζ(9, 3, 3)) + 75(ζ(3, 7, 5) + ζ(7, 3, 5) + ζ(7, 5, 3)) + 84(ζ(3, 5, 7) + ζ(5, 3, 7) + ζ(5, 7, 3)) 0 (mod Z (2) 15 ). 36ζ(5, 5, 5) + 6ζ(5, 7, 3) + 15ζ(7, 5, 3) 14ζ(9, 3, 3) 0 (mod Z (2) 15 ),., ( GKZ ), 3 d=12 dim S d(sl 2 (Z)),. 19
20 [1] T. Araawa, M. Kaneo,, MI 23. [2] F. Brown, Mixed Tate motives over Z, Ann. of Math. 175(2) (2012), [3] F. Brown, On the decomposition of motivic multiple zeta values, Galois-Teichmüller theory and Arithmetic Geometry, Advanced Studies in Pure Mathematics. [4] F. Brown, Depth-graded motivic multiple zeta values, arxiv: [5] D. Broadhurst, D. Kreimer, Association of multiple zeta values with positive nots via Feynman diagrams up to 9 loops, Phys. Lett. B 393, no. 3-4 (1997), [6] H. Furusho, The Multiple Zeta Value Algebra And The Stable Derivation Algebra, RIMS-oyurou 1200, Algebraic number theory and related topics, (2001), [7] H. Gangle, M. Kaneo, D. Zagier, Double zeta values and modular forms, Automorphic forms and Zeta functions, Proceedings of the conference in memory of Tsuneo Araawa, World Scientific, (2006), [8] P. Deligne, A.B. Goncharov, Groupes fondamentaux motiviques de Tate mixte, Ann. Sci. Ećole Norm. Sup. 38 (2005), 1 56 [9] A. B. Goncharov, Multiple polylogarithms, cyclotomy and modular complexes, Math. Res. Lett., 5 (1998), [10] A. B. Goncharov, The dihedral Lie algebras and Galois symmetries of π (l) 1 (P 1 ({0, } µ N )), Due Math. J. 110(3) (2001), [11] M. Hoffman, The algebra of multiple harmonic series, J. of Algebra, 194 (1997), [12] K. Ihara, Derivation and double shuffle relations for multiple zeta values, RIMS 1549 (2007), [13] K. Ihara, M. Kaneo, D. Zagier, Derivation and double shuffle relations for multiple zeta values, Compositio Math. 142 (2006),
21 [14] K. Ihara, H. Ochiai, Symmetry on linear relations for multiple zeta values, Nagoya Math. J. 189 (2008), [15] C. Kassel, Quantum groups, Graduate Texts in Mathematics, 155. Springer-Verlag, New Yor, [16] W. Kohnen, D. Zagier, Modular forms with rational periods, Modular forms (Durham, 1983), , Ellis Horwood [17] S. Lang, Introduction to modular forms. Grundlehren der mathematischen Wissenschaften, No Springer-Verlag, Berlin-New Yor, [18] C. Reutenauer, Free Lie algebras (Oxford Science Publications, Oxford, 1993). [19] G. Shimura, Introduction to the arithmetic theory of automorphic functions. Kanô Memorial Lectures, No. 1. Publications of the Mathematical Society of Japan, No. 11. Iwanami Shoten, Publishers, Toyo; Princeton University Press, Princeton, N.J., [20] L. Schneps, On the Poisson Bracet on the Free Lie Algebra in two Generators, Journal of Lie Theory 16(1) (2006), [21] T. Terasoma, Mixed Tate motives and multiple zeta values, Invent. Math. 149(2) (2002), [22] C. Weibel, An introduction to homological algebra, Cambridge Studies in Advanced Mathematics, 38. Cambridge University Press, [23] D. Zagier, Values of zeta functions and their applications, First European Congress of Mathematics, Vol. II (Paris, 1992), Progr. Math., 120, Birhäuser, Basel (1994), [24] D. Zagier, Periods of modular forms, traces of Hece operators, and multiple zeta values, in Hoei-eishii to L-ansuu no enyuu (= Research on Automorphic Forms and L-Functions), RIMS Koyurou 843 (1993),
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 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 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[Oc, Proposition 2.1, Theorem 2.4] K X (a) l (b) l (a) (b) X [M3] Huber adic 1 Huber ([Hu1], [Hu2], [Hu3]) adic 1.1 adic A I I A {I n } 0 adic 2
On the action of the Weil group on the l-adic cohomology of rigid spaces over local fields (Yoichi Mieda) Graduate School of Mathematical Sciences, The University of Tokyo 0 l Galois K F F q l q K, F K,
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 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 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 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 information平成 30 年度 ( 第 40 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 30 ~8 年月 72 月日開催 30 日 [6] 1 4 A 1 A 2 A 3 l P 3 P 2 P 1 B 1 B 2 B 3 m 1 l 3 A 1, A 2, A 3 m 3 B 1,
[6] 1 4 A 1 A 2 A 3 l P 3 P 2 P 1 B 1 B 2 B 3 m 1 l 3 A 1, A 2, A 3 m 3 B 1, B 2, B 3 A i 1 B i+1 A i+1 B i 1 P i i = 1, 2, 3 3 3 P 1, P 2, P 3 1 *1 19 3 27 B 2 P m l (*) l P P l m m 1 P l m + m *1 A N
More information平成 15 年度 ( 第 25 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 ~8 15 月年 78 日開催月 4 日 ) X 2 = 1 ( ) f 1 (X 1,..., X n ) = 0,..., f r (X 1,..., X n ) = 0 X = (
1 1.1 X 2 = 1 ( ) f 1 (X 1,..., X n ) = 0,..., f r (X 1,..., X n ) = 0 X = (X 1,..., X n ) ( ) X 1,..., X n f 1,..., f r A T X + XA XBR 1 B T X + C T QC = O X 1.2 X 1,..., X n X i X j X j X i = 0, P i
More information,. 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,
More informationmeiji_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
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 informationφ 4 Minimal subtraction scheme 2-loop ε 2008 (University of Tokyo) (Atsuo Kuniba) version 21/Apr/ Formulas Γ( n + ɛ) = ( 1)n (1 n! ɛ + ψ(n + 1)
φ 4 Minimal subtraction scheme 2-loop ε 28 University of Tokyo Atsuo Kuniba version 2/Apr/28 Formulas Γ n + ɛ = n n! ɛ + ψn + + Oɛ n =,, 2, ψn + = + 2 + + γ, 2 n ψ = γ =.5772... Euler const, log + ax 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. Mac Lane [ML98]. 1 2 (strict monoidal category) S 1 R 3 A S 1 [0, 1] C 2 C End C (1) C 4 1 U q (sl 2 ) Drinfeld double. 6 2
2014 6 30. 2014 3 1 6 (Hopf algebra) (group) Andruskiewitsch-Santos [AFS09] 1980 Drinfeld (quantum group) Lie Lie (ribbon Hopf algebra) (ribbon category) Turaev [Tur94] Kassel [Kas95] (PD) x12005i@math.nagoya-u.ac.jp
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 informationD-brane K 1, 2 ( ) 1 K D-brane K K D-brane Witten [1] D-brane K K K K D-brane D-brane K RR BPS D-brane
D-brane K 1, 2 E-mail: sugimoto@yukawa.kyoto-u.ac.jp (2004 12 16 ) 1 K D-brane K K D-brane Witten [1] D-brane K K K K D-brane D-brane K RR BPS D-brane D-brane RR D-brane K D-brane K D-brane K K [2, 3]
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 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(2) Fisher α (α) α Fisher α ( α) 0 Levi Civita (1) ( 1) e m (e) (m) ([1], [2], [13]) Poincaré e m Poincaré e m Kähler-like 2 Kähler-like
() 10 9 30 1 Fisher α (α) α Fisher α ( α) 0 Levi Civita (1) ( 1) e m (e) (m) ([1], [], [13]) Poincaré e m Poincaré e m Kähler-like Kähler-like Kähler M g M X, Y, Z (.1) Xg(Y, Z) = g( X Y, Z) + g(y, XZ)
More informationmain.dvi
SGC - 70 2, 3 23 ɛ-δ 2.12.8 3 2.92.13 4 2 3 1 2.1 2.102.12 [8][14] [1],[2] [4][7] 2 [4] 1 2009 8 1 1 1.1... 1 1.2... 4 1.3 1... 8 1.4 2... 9 1.5... 12 1.6 1... 16 1.7... 18 1.8... 21 1.9... 23 2 27 2.1
More informationA11 (1993,1994) 29 A12 (1994) 29 A13 Trefethen and Bau Numerical Linear Algebra (1997) 29 A14 (1999) 30 A15 (2003) 30 A16 (2004) 30 A17 (2007) 30 A18
2013 8 29y, 2016 10 29 1 2 2 Jordan 3 21 3 3 Jordan (1) 3 31 Jordan 4 32 Jordan 4 33 Jordan 6 34 Jordan 8 35 9 4 Jordan (2) 10 41 x 11 42 x 12 43 16 44 19 441 19 442 20 443 25 45 25 5 Jordan 26 A 26 A1
More informationnewmain.dvi
数論 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/008142 このサンプルページの内容は, 第 2 版 1 刷発行当時のものです. Daniel DUVERNEY: THÉORIE DES NOMBRES c Dunod, Paris, 1998, This book is published
More informationx, y x 3 y xy 3 x 2 y + xy 2 x 3 + y 3 = x 3 y xy 3 x 2 y + xy 2 x 3 + y 3 = 15 xy (x y) (x + y) xy (x y) (x y) ( x 2 + xy + y 2) = 15 (x y)
x, y x 3 y xy 3 x 2 y + xy 2 x 3 + y 3 = 15 1 1977 x 3 y xy 3 x 2 y + xy 2 x 3 + y 3 = 15 xy (x y) (x + y) xy (x y) (x y) ( x 2 + xy + y 2) = 15 (x y) ( x 2 y + xy 2 x 2 2xy y 2) = 15 (x y) (x + y) (xy
More information1 Abstract 2 3 n a ax 2 + bx + c = 0 (a 0) (1) ( x + b ) 2 = b2 4ac 2a 4a 2 D = b 2 4ac > 0 (1) 2 D = 0 D < 0 x + b 2a = ± b2 4ac 2a b ± b 2
1 Abstract n 1 1.1 a ax + bx + c = 0 (a 0) (1) ( x + b ) = b 4ac a 4a D = b 4ac > 0 (1) D = 0 D < 0 x + b a = ± b 4ac a b ± b 4ac a b a b ± 4ac b i a D (1) ax + bx + c D 0 () () (015 8 1 ) 1. D = b 4ac
More information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
More informationMacdonald, ,,, Macdonald. Macdonald,,,,,.,, Gauss,,.,, Lauricella A, B, C, D, Gelfand, A,., Heckman Opdam.,,,.,,., intersection,. Macdona
Macdonald, 2015.9.1 9.2.,,, Macdonald. Macdonald,,,,,.,, Gauss,,.,, Lauricella A, B, C, D, Gelfand, A,., Heckman Opdam.,,,.,,., intersection,. Macdonald,, q., Heckman Opdam q,, Macdonald., 1 ,,. Macdonald,
More informationDynkin Serre Weyl
Dynkin Naoya Enomoto 2003.3. paper Dynkin Introduction Dynkin Lie Lie paper 1 0 Introduction 3 I ( ) Lie Dynkin 4 1 ( ) Lie 4 1.1 Lie ( )................................ 4 1.2 Killing form...........................................
More informationK 2 X = 4 MWG(f), X P 2 F, υ 0 : X P 2 2,, {f λ : X λ P 1 } λ Λ NS(X λ ), (υ 0 ) λ : X λ P 2 ( 1) X 6, f λ K X + F, f ( 1), n, n 1 (cf [10]) X, f : X
2 E 8 1, E 8, [6], II II, E 8, 2, E 8,,, 2 [14],, X/C, f : X P 1 2 3, f, (O), f X NS(X), (O) T ( 1), NS(X), T [15] : MWG(f) NS(X)/T, MWL(f) 0 (T ) NS(X), MWL(f) MWL(f) 0, : {f λ : X λ P 1 } λ Λ NS(X λ
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 information2 2 MATHEMATICS.PDF 200-2-0 3 2 (p n ), ( ) 7 3 4 6 5 20 6 GL 2 (Z) SL 2 (Z) 27 7 29 8 SL 2 (Z) 35 9 2 40 0 2 46 48 2 2 5 3 2 2 58 4 2 6 5 2 65 6 2 67 7 2 69 2 , a 0 + a + a 2 +... b b 2 b 3 () + b n a
More informationD 24 D D D
5 Paper I.R. 2001 5 Paper HP Paper 5 3 5.1................................................... 3 5.2.................................................... 4 5.3.......................................... 6
More informationR C Gunning, Lectures on Riemann Surfaces, Princeton Math Notes, Princeton Univ Press 1966,, (4),,, Gunning, Schwarz Schwarz Schwarz, {z; x}, [z; x] =
Schwarz 1, x z = z(x) {z; x} {z; x} = z z 1 2 z z, = d/dx (1) a 0, b {az; x} = {z; x}, {z + b; x} = {z; x} {1/z; x} = {z; x} (2) ad bc 0 a, b, c, d 2 { az + b cz + d ; x } = {z; x} (3) z(x) = (ax + b)/(cx
More information20 6 4 1 4 1.1 1.................................... 4 1.1.1.................................... 4 1.1.2 1................................ 5 1.2................................... 7 1.2.1....................................
More informationX 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
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 informationDonaldson Seiberg-Witten [GNY] f U U C 1 f(z)dz = Res f(a) 2πi C a U U α = f(z)dz dα = 0 U f U U P 1 α 0 a P 1 Res a α = 0. P 1 Donaldson Seib
( ) Donaldson Seiberg-Witten Witten Göttsche [GNY] L. Göttsche, H. Nakajima and K. Yoshioka, Donaldson = Seiberg-Witten from Mochizuki s formula and instanton counting, Publ. of RIMS, to appear Donaldson
More informationZ: Q: R: C:
0 Z: Q: R: C: 3 4 4 4................................ 4 4.................................. 7 5 3 5...................... 3 5......................... 40 5.3 snz) z)........................... 4 6 46 x
More informationコホモロジー的AGT対応とK群類似
AGT K ( ) Encounter with Mathematics October 29, 2016 AGT L. F. Alday, D. Gaiotto, Y. Tachikawa, Liouville Correlation Functions from Four-dimensional Gauge Theories, Lett. Math. Phys. 91 (2010), arxiv:0906.3219.
More informationIII 1 (X, d) d U d X (X, d). 1. (X, d).. (i) d(x, y) d(z, y) d(x, z) (ii) d(x, y) d(z, w) d(x, z) + d(y, w) 2. (X, d). F X.. (1), X F, (2) F 1, F 2 F
III 1 (X, d) d U d X (X, d). 1. (X, d).. (i) d(x, y) d(z, y) d(x, z) (ii) d(x, y) d(z, w) d(x, z) + d(y, w) 2. (X, d). F X.. (1), X F, (2) F 1, F 2 F F 1 F 2 F, (3) F λ F λ F λ F. 3., A λ λ A λ. B λ λ
More information,2,4
2005 12 2006 1,2,4 iii 1 Hilbert 14 1 1.............................................. 1 2............................................... 2 3............................................... 3 4.............................................
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 information( 9 1 ) 1 2 1.1................................... 2 1.2................................................. 3 1.3............................................... 4 1.4...........................................
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 informationII No.01 [n/2] [1]H n (x) H n (x) = ( 1) r n! r!(n 2r)! (2x)n 2r. r=0 [2]H n (x) n,, H n ( x) = ( 1) n H n (x). [3] H n (x) = ( 1) n dn x2 e dx n e x2
II No.1 [n/] [1]H n x) H n x) = 1) r n! r!n r)! x)n r r= []H n x) n,, H n x) = 1) n H n x) [3] H n x) = 1) n dn x e dx n e x [4] H n+1 x) = xh n x) nh n 1 x) ) d dx x H n x) = H n+1 x) d dx H nx) = nh
More information20 9 19 1 3 11 1 3 111 3 112 1 4 12 6 121 6 122 7 13 7 131 8 132 10 133 10 134 12 14 13 141 13 142 13 143 15 144 16 145 17 15 19 151 1 19 152 20 2 21 21 21 211 21 212 1 23 213 1 23 214 25 215 31 22 33
More information2/14 2 () (O O) O O (O O) id γ γ id O O γ O O O γ η id id η I O O O O I γ O. O(n) n *5 γ η γ S M, N M N (M N)(n) ( ) M(k) Sk Ind S n S i1 S ik N(i 1 )
1/14 * 1. Vassiliev Hopf P = k P k Kontsevich Bar-Natan P k (g,n) k=g 1+n, n>0, g 0 H 1 g ( S 1 H F(Com) ) ((g, n)) Sn. Com F Feynman ()S 1 H S n ()Kontsevich ( - - Lie ) 1 *2 () [LV12] Koszul 1.1 S F
More information液晶の物理1:連続体理論(弾性,粘性)
The Physics of Liquid Crystals P. G. de Gennes and J. Prost (Oxford University Press, 1993) Liquid crystals are beautiful and mysterious; I am fond of them for both reasons. My hope is that some readers
More information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
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 information1. A0 A B A0 A : A1,...,A5 B : B1,...,B
1. A0 A B A0 A : A1,...,A5 B : B1,...,B12 2. 3. 4. 5. A0 A, B Z Z m, n Z m n m, n A m, n B m=n (1) A, B (2) A B = A B = Z/ π : Z Z/ (3) A B Z/ (4) Z/ A, B (5) f : Z Z f(n) = n f = g π g : Z/ Z A, B (6)
More information2010 ( )
2010 (2010 1 8 2010 1 13 ( 1 29 ( 17:00 2 3 ( e-mail (1 3 (2 (3 (1 (4 2010 1 2 3 4 5 6 7 8 9 10 11 Hesselholt, Lars 12 13 i 1 ( 2 3 Cohen-Macaulay Auslander-Reiten [1] [2] 5 [1], :,, 2002 [2] I Assem,
More informationS I. dy fx x fx y fx + C 3 C dy fx 4 x, y dy v C xt y C v e kt k > xt yt gt [ v dt dt v e kt xt v e kt + C k x v + C C k xt v k 3 r r + dr e kt S dt d
S I.. http://ayapin.film.s.dendai.ac.jp/~matuda /TeX/lecture.html PDF PS.................................... 3.3.................... 9.4................5.............. 3 5. Laplace................. 5....
More information1 = = = (set) (element) a A a A a A a A a A {2, 5, (0, 1)}, [ 1, 1] = {x; 1 x 1}. (proposition) A = {x; P (x)} P (x) x x a A a A Remark. (i) {2, 0, 0,
2005 4 1 1 2 2 6 3 8 4 11 5 14 6 18 7 20 8 22 9 24 10 26 11 27 http://matcmadison.edu/alehnen/weblogic/logset.htm 1 1 = = = (set) (element) a A a A a A a A a A {2, 5, (0, 1)}, [ 1, 1] = {x; 1 x 1}. (proposition)
More informationBasic Math. 1 0 [ N Z Q Q c R C] 1, 2, 3,... natural numbers, N Def.(Definition) N (1) 1 N, (2) n N = n +1 N, (3) N (1), (2), n N n N (element). n/ N.
Basic Mathematics 16 4 16 3-4 (10:40-12:10) 0 1 1 2 2 2 3 (mapping) 5 4 ε-δ (ε-δ Logic) 6 5 (Potency) 9 6 (Equivalence Relation and Order) 13 7 Zorn (Axiom of Choice, Zorn s Lemma) 14 8 (Set and Topology)
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 information( ) (, ) ( )
( ) (, ) ( ) 1 2 2 2 2.1......................... 2 2.2.............................. 3 2.3............................... 4 2.4.............................. 5 2.5.............................. 6 2.6..........................
More informationλ n numbering Num(λ) Young numbering T i j T ij Young T (content) cont T (row word) word T µ n S n µ C(µ) 0.2. Young λ, µ n Kostka K µλ K µλ def = #{T
0 2 8 8 6 3 0 0 Young Young [F] 0.. Young λ n λ n λ = (λ,, λ l ) λ λ 2 λ l λ = ( m, 2 m 2, ) λ = n, l(λ) = l {λ n n 0} P λ = (λ, ), µ = (µ, ) n λ µ k k k λ i µ i λ µ λ = µ k i= i= i < k λ i = µ i λ k >
More information25 7 18 1 1 1.1 v.s............................. 1 1.1.1.................................. 1 1.1.2................................. 1 1.1.3.................................. 3 1.2................... 3
More informationArmstrong culture Web
2004 5 10 M.A. Armstrong, Groups and Symmetry, Springer-Verlag, NewYork, 1988 (2000) (1989) (2001) (2002) 1 Armstrong culture Web 1 3 1.1................................. 3 1.2.................................
More informationI 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
More information等質空間の幾何学入門
2006/12/04 08 tamaru@math.sci.hiroshima-u.ac.jp i, 2006/12/04 08. 2006, 4.,,.,,.,.,.,,.,,,.,.,,.,,,.,. ii 1 1 1.1 :................................... 1 1.2........................................ 2 1.3......................................
More information30
3 ............................................2 2...........................................2....................................2.2...................................2.3..............................
More information163 KdV KP Lax pair L, B L L L 1/2 W 1 LW = ( / x W t 1, t 2, t 3, ψ t n ψ/ t n = B nψ (KdV B n = L n/2 KP B n = L n KdV KP Lax W Lax τ KP L ψ τ τ Cha
63 KdV KP Lax pair L, B L L L / W LW / x W t, t, t 3, ψ t n / B nψ KdV B n L n/ KP B n L n KdV KP Lax W Lax τ KP L ψ τ τ Chapter 7 An Introduction to the Sato Theory Masayui OIKAWA, Faculty of Engneering,
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 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 information8.1 Fubini 8.2 Fubini 9 (0%) 10 (50%) Carathéodory 10.3 Fubini 1 Introduction 1 (1) (2) {f n (x)} n=1 [a, b] K > 0 n, x f n (x) K < ( ) x [a
% 100% 1 Introduction 2 (100%) 2.1 2.2 2.3 3 (100%) 3.1 3.2 σ- 4 (100%) 4.1 4.2 5 (100%) 5.1 5.2 5.3 6 (100%) 7 (40%) 8 Fubini (90%) 2007.11.5 1 8.1 Fubini 8.2 Fubini 9 (0%) 10 (50%) 10.1 10.2 Carathéodory
More informationI
I 6 4 10 1 1 1.1............... 1 1................ 1 1.3.................... 1.4............... 1.4.1.............. 1.4................. 1.4.3........... 3 1.4.4.. 3 1.5.......... 3 1.5.1..............
More information1 filename=mathformula tex 1 ax 2 + bx + c = 0, x = b ± b 2 4ac, (1.1) 2a x 1 + x 2 = b a, x 1x 2 = c a, (1.2) ax 2 + 2b x + c = 0, x = b ± b 2
filename=mathformula58.tex ax + bx + c =, x = b ± b 4ac, (.) a x + x = b a, x x = c a, (.) ax + b x + c =, x = b ± b ac. a (.3). sin(a ± B) = sin A cos B ± cos A sin B, (.) cos(a ± B) = cos A cos B sin
More informationn ( (
1 2 27 6 1 1 m-mat@mathscihiroshima-uacjp 2 http://wwwmathscihiroshima-uacjp/~m-mat/teach/teachhtml 2 1 3 11 3 111 3 112 4 113 n 4 114 5 115 5 12 7 121 7 122 9 123 11 124 11 125 12 126 2 2 13 127 15 128
More informationMilnor 1 ( ), IX,. [KN].,. 2 : (1),. (2). 1 ; 1950, Milnor[M1, M2]. Milnor,,. ([Hil, HM, IO, St] ).,.,,, ( 2 5 )., Milnor ( 4.1)..,,., [CEGS],. Ω m, P
Milnor 1 ( ), IX,. [KN].,. 2 : (1),. (2). 1 ; 1950, Milnor[M1, M2]. Milnor,,. ([Hil, HM, IO, St] ).,.,,, ( 2 5 )., Milnor ( 4.1)..,,., [CEGS],. Ω m, PC ( 4 5 )., 5, Milnor Milnor., ( 6 )., (I) Z modulo
More informationI. (CREMONA ) : Cremona [C],., modular form f E f. 1., modular X H 1 (X, Q). modular symbol M-symbol, ( ) modular symbol., notation. H = { z = x
I. (CREMONA ) : Cremona [C],., modular form f E f. 1., modular X H 1 (X, Q). modular symbol M-symbol, ( ). 1.1. modular symbol., notation. H = z = x iy C y > 0, cusp H = H Q., Γ = PSL 2 (Z), G Γ [Γ : G]
More informationC p (.2 C p [[T ]] Bernoull B n,χ C p p q p 2 q = p p = 2 q = 4 ω Techmüller a Z p ω(a a ( mod q φ(q ω(a Z p a pz p ω(a = 0 Z p φ Euler Techmüller ω Q
p- L- [Iwa] [Iwa2] -Leopoldt [KL] p- L-. Kummer Remann ζ(s Bernoull B n (. ζ( n = B n n, ( n Z p a = Kummer [Kum] ( Kummer p m n 0 ( mod p m n a m n ( mod (p p a ( p m B m m ( pn B n n ( mod pa Z p Kummer
More informationi
009 I 1 8 5 i 0 1 0.1..................................... 1 0.................................................. 1 0.3................................. 0.4........................................... 3
More information006 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......................
More informationA
A 2563 15 4 21 1 3 1.1................................................ 3 1.2............................................. 3 2 3 2.1......................................... 3 2.2............................................
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 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 informationx (x, ) x y (, y) iy x y z = x + iy (x, y) (r, θ) r = x + y, θ = tan ( y ), π < θ π x r = z, θ = arg z z = x + iy = r cos θ + ir sin θ = r(cos θ + i s
... x, y z = x + iy x z y z x = Rez, y = Imz z = x + iy x iy z z () z + z = (z + z )() z z = (z z )(3) z z = ( z z )(4)z z = z z = x + y z = x + iy ()Rez = (z + z), Imz = (z z) i () z z z + z z + z.. z
More information変 位 変位とは 物体中のある点が変形後に 別の点に異動したときの位置の変化で あり ベクトル量である 変位には 物体の変形の他に剛体運動 剛体変位 が含まれている 剛体変位 P(x, y, z) 平行移動と回転 P! (x + u, y + v, z + w) Q(x + d x, y + dy,
変 位 変位とは 物体中のある点が変形後に 別の点に異動したときの位置の変化で あり ベクトル量である 変位には 物体の変形の他に剛体運動 剛体変位 が含まれている 剛体変位 P(x, y, z) 平行移動と回転 P! (x + u, y + v, z + w) Q(x + d x, y + dy, z + dz) Q! (x + d x + u + du, y + dy + v + dv, z +
More information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..............
More information(Bessel) (Legendre).. (Hankel). (Laplace) V = (x, y, z) n (r, θ, ϕ) r n f n (θ, ϕ). f n (θ, ϕ) n f n (θ, ϕ) z = cos θ z θ ϕ n ν. P ν (z), Q ν (z) (Fou
(Bessel) (Legendre).. (Hankel). (Laplace) V = (x, y, z) n (r, θ, ϕ) r n f n (θ, ϕ). f n (θ, ϕ) n f n (θ, ϕ) z = cos θ z θ ϕ n ν. P ν (z), Q ν (z) (Fourier) (Fourier Bessel).. V ρ(x, y, z) V = 4πGρ G :.
More informationI A A441 : April 15, 2013 Version : 1.1 I Kawahira, Tomoki TA (Shigehiro, Yoshida )
I013 00-1 : April 15, 013 Version : 1.1 I Kawahira, Tomoki TA (Shigehiro, Yoshida) http://www.math.nagoya-u.ac.jp/~kawahira/courses/13s-tenbou.html pdf * 4 15 4 5 13 e πi = 1 5 0 5 7 3 4 6 3 6 10 6 17
More informationA bound of the number of reduced Arakelov divisors of a number field (joint work with Ryusuke Yoshimitsu) Takao Watanabe Department of Mathematics Osa
A bound of the number of reduced Arakelov divisors of a number field (joint work with Ryusuke Yoshimitsu) Takao Watanabe Department of Mathematics Osaka University , Schoof Algorithmic Number Theory, MSRI
More information( )/2 hara/lectures/lectures-j.html 2, {H} {T } S = {H, T } {(H, H), (H, T )} {(H, T ), (T, T )} {(H, H), (T, T )} {1
( )/2 http://www2.math.kyushu-u.ac.jp/ hara/lectures/lectures-j.html 1 2011 ( )/2 2 2011 4 1 2 1.1 1 2 1 2 3 4 5 1.1.1 sample space S S = {H, T } H T T H S = {(H, H), (H, T ), (T, H), (T, T )} (T, H) S
More informationz f(z) f(z) x, y, u, v, r, θ r > 0 z = x + iy, f = u + iv C γ D f(z) f(z) D f(z) f(z) z, Rm z, z 1.1 z = x + iy = re iθ = r (cos θ + i sin θ) z = x iy
z fz fz x, y, u, v, r, θ r > z = x + iy, f = u + iv γ D fz fz D fz fz z, Rm z, z. z = x + iy = re iθ = r cos θ + i sin θ z = x iy = re iθ = r cos θ i sin θ x = z + z = Re z, y = z z = Im z i r = z = z
More information1 1, 2016 D B. 1.1,.,,. (1). (2). (3) Milnor., (1) (2)., (3). 1.2,.,, ( )..,.,,. 1.3, webpage,.,,.
1 1, 2016 D B. 1.1,.,,. (1). (2). (3) Milnor., (1) (2)., (3). 1.2,.,, ( )..,.,,. 1.3, 2015. webpage,.,,. 2 1 (1),, ( ). (2),,. (3),.,, : Hashinaga, T., Tamaru, H.: Three-dimensional solvsolitons and the
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 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 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 information³ÎΨÏÀ
2017 12 12 Makoto Nakashima 2017 12 12 1 / 22 2.1. C, D π- C, D. A 1, A 2 C A 1 A 2 C A 3, A 4 D A 1 A 2 D Makoto Nakashima 2017 12 12 2 / 22 . (,, L p - ). Makoto Nakashima 2017 12 12 3 / 22 . (,, L p
More informationBlack-Scholes [1] Nelson [2] Schrödinger 1 Black Scholes [1] Black-Scholes Nelson [2][3][4] Schrödinger Nelson Parisi Wu [5] Nelson Parisi-W
003 7 14 Black-Scholes [1] Nelson [] Schrödinger 1 Black Scholes [1] Black-Scholes Nelson [][3][4] Schrödinger Nelson Parisi Wu [5] Nelson Parisi-Wu Nelson e-mail: takatoshi-tasaki@nifty.com kabutaro@mocha.freemail.ne.jp
More informationGauss Fuchs rigid rigid rigid Nicholas Katz Rigid local systems [6] Fuchs Katz Crawley- Boevey[1] [7] Katz rigid rigid Katz middle convolu
rigidity 2014.9.1-2014.9.2 Fuchs 1 Introduction y + p(x)y + q(x)y = 0, y 2 p(x), q(x) p(x) q(x) Fuchs 19 Fuchs 83 Gauss Fuchs rigid rigid rigid 7 1970 1996 Nicholas Katz Rigid local systems [6] Fuchs Katz
More informationPart () () 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
More information) ] [ h m x + y + + V x) φ = Eφ 1) z E = i h t 13) x << 1) N n n= = N N + 1) 14) N n n= = N N + 1)N + 1) 6 15) N n 3 n= = 1 4 N N + 1) 16) N n 4
1. k λ ν ω T v p v g k = π λ ω = πν = π T v p = λν = ω k v g = dω dk 1) ) 3) 4). p = hk = h λ 5) E = hν = hω 6) h = h π 7) h =6.6618 1 34 J sec) hc=197.3 MeV fm = 197.3 kev pm= 197.3 ev nm = 1.97 1 3 ev
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: , 2.0, 3.0, 2.0, (%) ( 2.
2017 1 2 1.1...................................... 2 1.2......................................... 4 1.3........................................... 10 1.4................................. 14 1.5..........................................
More informationG H J(g, τ G g G J(g, τ τ J(g 1 g, τ = J(g 1, g τj(g, τ J J(1, τ = 1 k g = ( a b c d J(g, τ = (cτ + dk G = SL (R SL (R G G α, β C α = α iθ (θ R
1 1.1 SL (R 1.1.1 SL (R H SL (R SL (R H H H = {z = x + iy C; x, y R, y > 0}, SL (R = {g M (R; dt(g = 1}, gτ = aτ + b a b g = SL (R cτ + d c d 1.1. Γ H H SL (R f(τ f(gτ G SL (R G H J(g, τ τ g G Hol f(τ
More information