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

Size: px
Start display at page:

Download "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"

Transcription

1 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, Z) t γj 1 n 0 n γ = J n } G = GSp(n, Q) + = {g M 2n (R) t gj n g = ν(g)j n, ν(g) R >0 } (2.1) g G g 1 Γ g Γ commensurable [Γ : Γ g 1 Γ g] <, [g 1 Γ g : Γ g 1 Γ g] < Γ G Hecke H(Γ, G) = H(Γ, G) C 1

2 C H(Γ, G) = a i (Γ g i Γ ) g i G, a i C i: : L(Γ, G) = { i: a i(γ g i ) g i G, a i C} C- Γ (γ, i a i(γ g i )) i a i(γ g i γ) L(Γ, G) Γ L(Γ, G) Γ ( )( ) a i (Γ γ i ) b j (Γ δ j ) = a i b j (Γ γ i δ j ) i j i,j C- H(Γ, G) L(Γ, G) Γ, Γ gγ = r Γ g i Γ gγ i=1 r Γ g i ( Γ \Γ gγ Γ g 1 Γ g\γ [Γ gγ : Γ ] < ) H(Γ, G) i=1 2.1 H(Γ, G) 2.2 g G Γ gγ diag(a 1,..., a g, d 1,..., d g ) a i d i = ν(g), a i a i+1, a g d g (ν(g) (2.1)) [An1, Theorem 3.28] ( ) ( ) A B t 2.1 G involution g = G g D t B = = C D t C t A ν(g)g 1 α α = J n αjg 1 g G Γ gγ = Γ g Γ Hecke Hecke G (p) = G GL(2n, Z[1/p]) H(Γ, G) = H p, H p = H(Γ, G (p) ) p: g G (p) ν(g) p H p 2

3 2.3 ( 1n 0 T (p) = Γ 0 p1 n ), T i (p 2 ) = Γ 1 i p1 n i p 2 1 i p1 n i Γ (0 i n) H p = C[T (p), T i (p 2 ) (1 i n)] (cf. [An1, Theorem 3.40]) Hecke Satake 3 Hecke Satake H p = G p = GSp(n, Q p ), K p = G p GL(2n, Z p ) { ϕ: G p C ϕ K p - i.e. ϕ(k 1 gk 2 ) = ϕ(g), k 1, k 2 K p ϕ } H p convolution ϕ 1 ϕ 2 (h) = ϕ 1 (g)ϕ 2 (g 1 h)dg G p C- 3.1 H p = H(Γ, G (p) ) H p, Γ gγ ch(k p gk p ) C- H p GSp T = {diag(u 1,..., u g, v 1,..., v g ) u 1 v 1 = u 2 v 2 = = u g v g } GSp ( ) 1 A B N = 0 ν t A 1 GSp A =... 1 P = T N GSp minimal parabolic subgroup GSp T Hecke : H p (T ) = {ψ : T (Q p ) C T (Z p )- } 3

4 T GL 1 n + 1 H p (T ) = C[X ± 0, X± 1,..., X± n ] ( ( 1n 0 X 0 = ch T (Z p ) 0 p1 n ( ( ) Si 0 X i = ch T (Z p ) 0 S 1 T (Z p ) i ) ) T (Z p ), ) i, S i = diag( 1,..., 1, p, 1,..., 1) T GSp N(T ) = {g GSp g 1 T g T } GSp Weyl W = N(T )/T T 3.2 W S n (Z/2Z) n S n n T t = diag(u 1,..., u n, v 1,..., v n ) n {(u 1, v 1 ), (u 2, v 2 ),..., (u n, v n )} (Z/2Z) n ε i ( i 1 0 ) u i v i W T T Hecke H p (T ) H p (T ) = C[X ± 0, X± 1,..., X± n ] W = S g (Z/2Z) n S g X 1,..., X n (Z/2Z) n ε i X 0 X 0 X i X i X 1 i X j X j (j i) H p (T ) W - H p (T ) W H p H p (T ) C- (Satake ) S : H p H p (T ), S(f)(g) = δ(t) 1/2 f(tn) dn δ(t) modulus n = Lie(N) δ(t) = det(ad n (t) p t = diag(u 1,..., u g, u 0 u 1 1,..., u 0u 1 n ) δ(t) = u n(n+1)/2 0 u 2 1u 4 2 u 2n n N 3.3 Satake C- H p H p (T ) W = C[X 0 ±, X± 1,..., X± n ] W 4

5 [Sa] p Bruhat-Tits [Ca] H p M G p KMK KMK = i M i K, M i = p l = ν(m) i ( ) p r i1 0 Ai B i 0 p l t A 1, A i =... i p r in 3.4 M n ch(kmk) X0 l (p j X j ) r ij i j=1 H p C[X ± 0, X± 1,... X± n ] W C X 0 p 3.3 n S(ch(KMK)) p ln(n+1)/4 X0 l (p j X j ) r ij i j=1 (cf. [AS, Lemma 1]) Siege L H n = {Z M n (C) t Z = Z, Im(Z) > 0 ( )} Siegel GSp(n, R) + H n ( ) g Z = (AZ + B)(CZ + D) 1 A B H, g = G C D g GSp(n, R) + k Z H n f f k g(z) = ν(g) nk n(n+1)/2 det(cz + D) k f(g Z ) (4.1) 4.1 H n f Γ = Sp(n, Z) k Siegel 5

6 (1) γ Γ f k γ = f (2) n = 1 f cusp Fourier f(z) = ν=0 a(ν)e 2πiνz n 2 (2) (Koecher ) f Fourier f(z) = S n A 0 C(A)e 2πi Tr(AZ) (4.2) S n A 0 A f (3) det(im(z)) k/2 f(z) f cusp k M k (Γ ) cusp S k (Γ ) Siegel Hecke H(Γ, G) Γ gγ Γ γγ = r i=1 Γ γ i f k [Γ gγ ] = r f k γ i H(Γ, G) M k (Γ ) S k (Γ ) i=1 [Gu1] Siegel A = A Q Q GSp(n, A) = GSp(n, Q)GSp(n, R) + p GSp(n, Z p ) () g = γg k f M k (Γ ) GSp(n, A) φ f ( ) φ f (g) = det(ci + D) k A B f(g i1 n ), g = C D Siegel GSp(n, A) g G p f k [Γ gγ ] = φ f ch(k p gk p ) 6

7 convolution, GSp(n, A) φ, ψ φ ψ(g) = (n, A)φ(gh)ψ(h 1 ) dh GSp S k (Γ ) Petersson, Z = X + iy H n H n d Z d Z = det Y (g+1) dxdy dx dy Lebesgue d Z Sp(n, R) f, g S k (Γ ) f, g = f(z)g(z) det(y ) k d Z Γ \H n S k (Γ ) cusp Γ αγ H(G) f k Γ αγ, g = f, g k Γ αγ H(G) S k (Γ ) H(G) f S k (Γ ) Hecke X H(G) f X = λ(x) f f 3.4 p λ f : H p = C[X 0 ±, X± 1,..., X± n ] W C C[X 0 ±, X± 1,..., X± n ] C[X 0 ±, X± 1,..., X± n ] W integral λ f C[X 0 ±, X± 1,..., X± n ] C : λ f X 0, X 1,..., X n C- H p C (C ) n+1 /W 4.2 f p (n + 1) {α p,0, α p,1,..., α p,n } f Satake Siegel L Satake Satake Hecke L Weyl 7

8 4.3 (1) f {α p,0, α p,1,..., α p,n } Satake 2 L L p st(f, t) = (1 t) 1 n i=1 L p spin (f, t) = (1 α p,0t) 1 ( 1 αp,i t ) 1( 1 αp,i 1 t ) 1 n (1 α p,0 α p,i1 α p,ir t) 1 r=1 1 i 1 < <i r n (2) f s C L st (f, s) = p L spin (f, s) = p L p st(f, p s ) L p spin (f, p s ) Re(s) 0 s L st (f, s) standard L L spin (f, s) spinor L spinor L Euler L spin (t) L spin (f, t) α i X i C[X 0 ±,..., X± n ] W [t] H p [t] ( ) T (p k ) {g G p M 2n (Z p ) ν(g) p k } H p H p H n (t) = T (p k )t k 2 n 2 P n (t) H n (t) = P n (t)l spin (p n(n+1)/2 t) spinor L k=0 L Sp n ( [Yo], connected L-group ) GSp n GSpin(2n + 1, C) = ( C 1 Spin(2n + 1, C) ) /Z, (Z Spin(2n + 1, C) 2 a ( 1, a) ) Spin n 1 {±1} Spin n SO n 1 8

9 standard L Spin n+1 SO n+1 SO n+1 standard spinor L spin SO n+1 2n n L L 4.1 (Böcheler [Bö]) f M k (Γ n ) ε n 1 0 ( ) s + ε n Λ(f, s) = (2π) ns π s/2 Γ Γ(s + k j)l st (f, s) 2 j=1 s- Λ(f, s) = Λ(f, s) 4.2 f M k (Γ n ) L spin (f, s) s- s nk n(n + 1) s n = 2 Andrianov ([An1]) 4.3 (Andrianov) Ψ(f, s) = Γ(s)Γ(s k + 2)(2π) 2s L spin (f, s) Ψ(f, s) Ψ(f, 2k 2 s) = ( 1) k Ψ(f, s) n = 3 Asgari-Schmidt L spin ([AS]) 5 L n M = p1 2n = diag(p,..., p) G Satake (3.4) ch(γ MΓ ) = p n(n+1)/2 X0 2 X 1 X n 9

10 (4.1) M f M k (Γ ) f k M = p nk n(n+1) f f Satake {α 0,..., α n } α0α 2 1 α n = p nk n(n+1)/2 (5.1) 5.1 ( ) 1 0 n = 1 Γ = SL(2, Z) T p Γ Γ 0 p Γ ( ) 1 0 Γ = Γ 0 p ( ) p 0 Γ = 0 1 ( ) p Γ 0 b p 1 ( ) p b Γ X 0 + X 0 X 1 C[X ± 0, X± 1 ]W f M k (Γ ) T (p)f = λ p f Satake prameter {α 0, α 1 } (5.1) α 0 + α 0 α 1 = λ p, α 2 0α 1 = p k 1 L spin (f, s) = p = p (1 α 0 p s ) 1 (1 α 0 α 1 p s ) 1 (1 λ p p s + p k 1 2s ) spinor L L L(f, s) Spin 3 = SL 2 GSpin(3, C) = GL(2, C) spinor GL(2, C) standard standard L L st (f, s) = p (1 p s ) 1 (1 α 1 p s ) 1 (1 α 1 1 p s ) 1 1 λ p t + p k 1 t 2 = (1 α 0 t)(1 α 0 α 1 t) α 2 0 = p k 1 α 1 1, α 0 (α 0 α 1 ) = p k 1, (α 0 α 1 ) 2 = p k 1 α 1 L st (f, s k + 1) = p (1 α 2 0p s ) 1 (1 α 2 0α 1 p s ) 1 (1 α 2 0α 2 1p s ) 1 = L(f, s, Sym 2 ) = ζ(2s 2k + 2) 10 n=1 a(n 2 ) n s

11 ( [Is] ) standard L 2 L accidental Spin(3, C) = SL(2, C) 2:1 SO(3, C) GL(3, C) ([Na2] : SL(2, R) 2:1 SO(2, 1) C ) SL 2 2 L standard L 5.2 Eisenstein Siegel Eisenstein E n k (Z) = ( A B C D ) Γ n \Γ n det(cz + D) k k n + 2 {( ) } Γ n A B = Γ n 0 D k n = 1 2ζ(k)Ek(z) 1 = (cz + d) k (c,d) Z 2 (0,0) Ek n(z) M k(γ n ) Ek n (Z) Hecke ( Zharkovskaya ) 5.1 Siegel Eisensetein E n k Satake α 0 = 1, α i = p k i (1 i n) n = 1 Ek 1 T p 1 + p k 1 n Zharkovskaya Siegel Φ 5.1 f M k (Γ n ) Φ(f) M k (Γ n 1 ) Φ(f)(z) = lim λ f (( )) z 0, z H 0 iλ n 1 11

12 f Fourier (4.2) Φ(f) Φ(f)(z) = Fourier (cf [Gu2, 3.3]). S n 1 a 0 C Φ(E n k ) = E n 1 k (( )) a 0 e 2πiaz (Zharkovskaya ) C- ψ : H p (Γ n ) H p (Γ n 1 ) (X 0, X 1,..., X n 1, X n ) (p k n X 0, X 1,..., X n 1, p n k ) f M k (Γ n ) T H p (Γ n ) Φ(f k T ) = Φ(f) k ψ(t ) [An2, Theorem 4.19] n = 2 Zharkovskaya Satake α 0 = p k 2, α 1 = p k 1, α 2 = p 2 k 3.2 W ε 2 α 0 = 1, α 1 = p k 1, α 2 = p k n L st (Ek n, s) = ζ(s) ζ(s k + i)ζ(s + k i) i=1 [An1] A.N. Andrianov Euler prodcts associated with Siegel modular forms of degree two, Russ. Math. Surveys 29, 3, (1974). [An2] A.N. Andrianov Indroduction to Siegel modura forms and Dirichlet series, Universitext. Springer, New York (2009). [AS] M. Asgari and R. Schmidt, Siegel modular forms and representations. Manuscripta Math. 104, no. 2, (2001). 12

13 [Bö] S. Böcherer Über die Funktionalgelichung automprpher L-Funktionen zur Siegelschen Modulgruppe. J. reine angew. Math. 362, (1985). [Ca] P. Cartier, Representations of p-adic groups: a survey. Automorphic forms, representations and L-functions, Part 1, pp , Proc. Sympos. Pure Math., 33, Amer. Math. Soc., Providence, R.I. (1979). [Fr] E. Freitag, Siegelsche Modulfunktionen, Grundl. Math. Wiss Springer-Verlag, Berlin. [vg] G. van der Geer, Siegel modular forms and their applications. The of modular forms, , Universitext, Springer, Berlin, (2008) [Gu1], GL 2, [Gu2], Siegel Eisensetein Fourier, [Is], L, 16 L (2009), p3-36. [Na1], L, 16 L (2009), p [Na2], Accidental, [Sa] I. Satake, Theory of spherical functions on reductive groups over p-adic fields, Publ. Math. I.H.E.S. 18, 5-69 (1963). [Yo], Functoriality Principle, 13

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

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,

More information

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+

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)

More information

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

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

More information

(ii) (iii) z a = z a =2 z a =6 sin z z a dz. cosh z z a dz. e z dz. (, a b > 6.) (z a)(z b) 52.. (a) dz, ( a = /6.), (b) z =6 az (c) z a =2 53. f n (z

(ii) (iii) z a = z a =2 z a =6 sin z z a dz. cosh z z a dz. e z dz. (, a b > 6.) (z a)(z b) 52.. (a) dz, ( a = /6.), (b) z =6 az (c) z a =2 53. f n (z B 4 24 7 9 ( ) :,..,,.,. 4 4. f(z): D C: D a C, 2πi C f(z) dz = f(a). z a a C, ( ). (ii), a D, a U a,r D f. f(z) = A n (z a) n, z U a,r, n= A n := 2πi C f(ζ) dζ, n =,,..., (ζ a) n+, C a D. (iii) U a,r

More information

Macdonald, ,,, Macdonald. Macdonald,,,,,.,, Gauss,,.,, Lauricella A, B, C, D, Gelfand, A,., Heckman Opdam.,,,.,,., intersection,. Macdona

Macdonald, ,,, 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 information

I. (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, ( ) 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 information

0. I II I II (1) linear type: GL( ), Sp( ), O( ), (2) loop type: loop current Kac-Moody affine, hyperbolic (3) diffeo t

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

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

, 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

D = [a, b] [c, d] D ij P ij (ξ ij, η ij ) f S(f,, {P ij }) S(f,, {P ij }) = = k m i=1 j=1 m n f(ξ ij, η ij )(x i x i 1 )(y j y j 1 ) = i=1 j

D = [a, b] [c, d] D ij P ij (ξ ij, η ij ) f S(f,, {P ij }) S(f,, {P ij }) = = k m i=1 j=1 m n f(ξ ij, η ij )(x i x i 1 )(y j y j 1 ) = i=1 j 6 6.. [, b] [, d] ij P ij ξ ij, η ij f Sf,, {P ij } Sf,, {P ij } k m i j m fξ ij, η ij i i j j i j i m i j k i i j j m i i j j k i i j j kb d {P ij } lim Sf,, {P ij} kb d f, k [, b] [, d] f, d kb d 6..

More information

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

More information

prime number theorem

prime number theorem For Tutor MeBio ζ Eite by kamei MeBio 7.8.3 : Bernoulli Bernoulli 4 Bernoulli....................................................................................... 4 Bernoulli............................................................................

More information

等質空間の幾何学入門

等質空間の幾何学入門 2006/12/04 08 [email protected] i, 2006/12/04 08. 2006, 4.,,.,,.,.,.,,.,,,.,.,,.,,,.,. ii 1 1 1.1 :................................... 1 1.2........................................ 2 1.3......................................

More information

2 1 κ c(t) = (x(t), y(t)) ( ) det(c (t), c x (t)) = det (t) x (t) y (t) y = x (t)y (t) x (t)y (t), (t) c (t) = (x (t)) 2 + (y (t)) 2. c (t) =

2 1 κ c(t) = (x(t), y(t)) ( ) det(c (t), c x (t)) = det (t) x (t) y (t) y = x (t)y (t) x (t)y (t), (t) c (t) = (x (t)) 2 + (y (t)) 2. c (t) = 1 1 1.1 I R 1.1.1 c : I R 2 (i) c C (ii) t I c (t) (0, 0) c (t) c(i) c c(t) 1.1.2 (1) (2) (3) (1) r > 0 c : R R 2 : t (r cos t, r sin t) (2) C f : I R c : I R 2 : t (t, f(t)) (3) y = x c : R R 2 : t (t,

More information

Z: Q: R: C: 3. Green Cauchy

Z: Q: R: C: 3. Green Cauchy 7 Z: Q: R: C: 3. Green.............................. 3.............................. 5.3................................. 6.4 Cauchy..................... 6.5 Taylor..........................6...............................

More information

非可換Lubin-Tate理論の一般化に向けて

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

More information

x (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 (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

1. R n Ω ε G ε 0 Ω ε B n 2 Ωε = with Bu = 0 on Ω ε i=1 x 2 i ε +0 B Bu = u (Dirichlet, D Ω ε ), Bu = u ν (Neumann, N Ω ε ), Ω ε G ( ) / 25

1. R n Ω ε G ε 0 Ω ε B n 2 Ωε = with Bu = 0 on Ω ε i=1 x 2 i ε +0 B Bu = u (Dirichlet, D Ω ε ), Bu = u ν (Neumann, N Ω ε ), Ω ε G ( ) / 25 .. IV 2012 10 4 ( ) 2012 10 4 1 / 25 1. R n Ω ε G ε 0 Ω ε B n 2 Ωε = with Bu = 0 on Ω ε i=1 x 2 i ε +0 B Bu = u (Dirichlet, D Ω ε ), Bu = u ν (Neumann, N Ω ε ), Ω ε G ( ) 2012 10 4 2 / 25 1. Ω ε B ε t

More information

Z: Q: R: C:

Z: 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

( ) 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- ( 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 information

meiji_resume_1.PDF

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

More information

( ),.,,., C A (2008, ). 1,, (M, g) (Riemannian symmetric space), : p M, s p : M M :.,.,.,, (, ).,, (M, g) p M, s p : M M p, : (1) p s p, (

( ),.,,., C A (2008, ). 1,, (M, g) (Riemannian symmetric space), : p M, s p : M M :.,.,.,, (, ).,, (M, g) p M, s p : M M p, : (1) p s p, ( ( ),.,,., C A (2008, ). 1,,. 1.1. (M, g) (Riemannian symmetric space), : p M, s p : M M :.,.,.,, (, ).,,. 1.2. (M, g) p M, s p : M M p, : (1) p s p, (2) s 2 p = id ( id ), (3) s p ( )., p ( s p (p) = p),,

More information

(2 X Poisso P (λ ϕ X (t = E[e itx ] = k= itk λk e k! e λ = (e it λ k e λ = e eitλ e λ = e λ(eit 1. k! k= 6.7 X N(, 1 ϕ X (t = e 1 2 t2 : Cauchy ϕ X (t

(2 X Poisso P (λ ϕ X (t = E[e itx ] = k= itk λk e k! e λ = (e it λ k e λ = e eitλ e λ = e λ(eit 1. k! k= 6.7 X N(, 1 ϕ X (t = e 1 2 t2 : Cauchy ϕ X (t 6 6.1 6.1 (1 Z ( X = e Z, Y = Im Z ( Z = X + iy, i = 1 (2 Z E[ e Z ] < E[ Im Z ] < Z E[Z] = E[e Z] + ie[im Z] 6.2 Z E[Z] E[ Z ] : E[ Z ] < e Z Z, Im Z Z E[Z] α = E[Z], Z = Z Z 1 {Z } E[Z] = α = α [ α ]

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) (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 information

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

More information

SUSY DWs

SUSY DWs @ 2013 1 25 Supersymmetric Domain Walls Eric A. Bergshoeff, Axel Kleinschmidt, and Fabio Riccioni Phys. Rev. D86 (2012) 085043 (arxiv:1206.5697) ( ) Contents 1 2 SUSY Domain Walls Wess-Zumino Embedding

More information

z 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 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 information

Note.tex 2008/09/19( )

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..................................

More information

Jacobi, Stieltjes, Gauss : :

Jacobi, Stieltjes, Gauss : : Jacobi, Stieltjes, Gauss : : 28 2 0 894 T. J. Stieltjes [St94a] Recherches sur les fractions continues Stieltjes 0 f(u)du, z + u f(u) > 0, z C z + + a a 2 z + a 3 +..., a p > 0 (a) Vitali (a) Stieltjes

More information

25 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 information

II 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.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 information

G 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

G 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

IA [email protected] Last updated: January,......................................................................................................................................................................................

More information

36 3 D f(z) D z f(z) z Taylor z D C f(z) z C C f (z) C f(z) f (z) f(z) D C D D z C C 3.: f(z) 3. f (z) f 2 (z) D D D D D f (z) f 2 (z) D D f (z) f 2 (

36 3 D f(z) D z f(z) z Taylor z D C f(z) z C C f (z) C f(z) f (z) f(z) D C D D z C C 3.: f(z) 3. f (z) f 2 (z) D D D D D f (z) f 2 (z) D D f (z) f 2 ( 3 3. D f(z) D D D D D D D D f(z) D f (z) f (z) f(z) D (i) (ii) (iii) f(z) = ( ) n z n = z + z 2 z 3 + n= z < z < z > f (z) = e t(+z) dt Re z> Re z> [ ] f (z) = e t(+z) = (Rez> ) +z +z t= z < f(z) Taylor

More information

Part () () Γ Part ,

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

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,,.

,. 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 information

A

A A 2563 15 4 21 1 3 1.1................................................ 3 1.2............................................. 3 2 3 2.1......................................... 3 2.2............................................

More information

第5章 偏微分方程式の境界値問題

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

App. of Leb. Integral Theory (S. Hiraba) Lebesgue (X, F, µ) (measure space)., X, 2 X, F 2 X σ (σ-field), i.e., (1) F, (2) A F = A c F, (3)

App. of Leb. Integral Theory (S. Hiraba) Lebesgue (X, F, µ) (measure space)., X, 2 X, F 2 X σ (σ-field), i.e., (1) F, (2) A F = A c F, (3) Lebesgue (Applications of Lebesgue Integral Theory) (Seiji HIABA) 1 1 1.1 1 Lebesgue........................ 1 1.2 2 Fubini...................... 2 2 L p 5 2.1 Banach, Hilbert..............................

More information

(τ τ ) τ, σ ( ) w = τ iσ, w = τ + iσ (w ) w, w ( ) τ, σ τ = (w + w), σ = i (w w) w, w w = τ w τ + σ w σ = τ + i σ w = τ w τ + σ w σ = τ i σ g ab w, w

(τ τ ) τ, σ ( ) w = τ iσ, w = τ + iσ (w ) w, w ( ) τ, σ τ = (w + w), σ = i (w w) w, w w = τ w τ + σ w σ = τ + i σ w = τ w τ + σ w σ = τ i σ g ab w, w S = 4π dτ dσ gg ij i X µ j X ν η µν η µν g ij g ij = g ij = ( 0 0 ) τ, σ (+, +) τ τ = iτ ds ds = dτ + dσ ds = dτ + dσ δ ij ( ) a =, a = τ b = σ g ij δ ab g g ( +, +,... ) S = 4π S = 4π ( i) = i 4π dτ dσ

More information

2000年度『数学展望 I』講義録

2000年度『数学展望 I』講義録 2000 I I IV I II 2000 I I IV I-IV. i ii 3.10 (http://www.math.nagoya-u.ac.jp/ kanai/) 2000 A....1 B....4 C....10 D....13 E....17 Brouwer A....21 B....26 C....33 D....39 E. Sperner...45 F....48 A....53

More information

20 4 20 i 1 1 1.1............................ 1 1.2............................ 4 2 11 2.1................... 11 2.2......................... 11 2.3....................... 19 3 25 3.1.............................

More information

x () g(x) = f(t) dt f(x), F (x) 3x () g(x) g (x) f(x), F (x) (3) h(x) = x 3x tf(t) dt.9 = {(x, y) ; x, y, x + y } f(x, y) = xy( x y). h (x) f(x), F (x

x () g(x) = f(t) dt f(x), F (x) 3x () g(x) g (x) f(x), F (x) (3) h(x) = x 3x tf(t) dt.9 = {(x, y) ; x, y, x + y } f(x, y) = xy( x y). h (x) f(x), F (x [ ] IC. f(x) = e x () f(x) f (x) () lim f(x) lim f(x) x + x (3) lim f(x) lim f(x) x + x (4) y = f(x) ( ) ( s46). < a < () a () lim a log xdx a log xdx ( ) n (3) lim log k log n n n k=.3 z = log(x + y ),

More information

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

More information

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.   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)

More information

cubic zeta 1ifting (Tomoyoshi IBUKIYAMA) (Department of Math., Graduate School of Sci., Osaka Univ. 1 \Re $\Phi^{\mathrm{J}}$ 1

cubic 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 information

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.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 )

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.   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 information

R 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

R 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: [email protected]) 1 1 ( 5 ) 2 ( Q ) Spec

More information

A 2008 10 (2010 4 ) 1 1 1.1................................. 1 1.2..................................... 1 1.3............................ 3 1.3.1............................. 3 1.3.2..................................

More information

213 March 25, 213, Rev.1.5 4........................ 4........................ 6 1 8 1.1............................... 8 1.2....................... 9 2 14 2.1..................... 14 2.2............................

More information

TOP URL 1

TOP URL   1 TOP URL http://amonphys.web.fc.com/ 3.............................. 3.............................. 4.3 4................... 5.4........................ 6.5........................ 8.6...........................7

More information

SO(2)

SO(2) TOP URL http://amonphys.web.fc2.com/ 1 12 3 12.1.................................. 3 12.2.......................... 4 12.3............................. 5 12.4 SO(2).................................. 6

More information

0. Intro ( K CohFT etc CohFT 5.IKKT 6.

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

More information

1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2

1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2 2005 9/8-11 2 2.2 ( 2-5) γ ( ) γ cos θ 2πr πρhr 2 g h = 2γ cos θ ρgr (2.1) γ = ρgrh (2.2) 2 cos θ θ cos θ = 1 (2.2) γ = 1 ρgrh (2.) 2 2. p p ρgh p ( ) p p = p ρgh (2.) h p p = 2γ r 1 1 (Berry,1975) 2-6

More information

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 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

More information

(yx4) 1887-1945 741936 50 1995 1 31 http://kenboushoten.web.fc.com/ OCR TeX 50 yx4 e-mail: [email protected] i Jacobi 1751 1 3 Euler Fagnano 187 9 0 Abel iii 1 1...................................

More information

211 [email protected] 1 R *1 n n R n *2 R n = {(x 1,..., x n ) x 1,..., x n R}. R R 2 R 3 R n R n R n D D R n *3 ) (x 1,..., x n ) f(x 1,..., x n ) f D *4 n 2 n = 1 ( ) 1 f D R n f : D R 1.1. (x,

More information

構造と連続体の力学基礎

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

More information

TOP URL 1

TOP URL   1 TOP URL http://amonphys.web.fc.com/ 1 19 3 19.1................... 3 19.............................. 4 19.3............................... 6 19.4.............................. 8 19.5.............................

More information

φ 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 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 information

20 6 4 1 4 1.1 1.................................... 4 1.1.1.................................... 4 1.1.2 1................................ 5 1.2................................... 7 1.2.1....................................

More information