( ),, ( [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

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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 = 1 Tate-Shafarevich ),, p Galois Bloch- ([BK90]),. L Galois ( )., Dirichlet,, p Galois ([Ka04]). 90 ([Ka93a], [FK06]), p Galois, p Galois ( ). p Galois.,, Q(ζ n ) (n 1) Euler ), Galois., p Galois Langlands, p Galois L L, p Galois L. L, L., L Galois., l Q l Galois G Ql p, Galois ( :16K17556) 2010 Mathematics Subject Classification: 11F80 (primary), 11F85, 11S25 (secondary), p Langlands 840-8502 1 e-mail: nkentaro@cc.saga-u.ac.jp

( ),, ( [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 p ) p Langlands )., GL 2 (Q p ) p Langlands, G Qp 2 p ( ), ( ) ([Na17b]). p Langlands?. 2., 2.1., 2.1.1.? p Galois V,,. Q, L (V ), (Hodge p ). Q l, (L, ) (L, ), l = p de Rham )D dr (V ), Bloch-Kato exponential., V (V ) 1 z geom (V ) (V ) (Q ), ε geom l (V ) (V ) (Q l ) (, Q V, L Beilinson ). p Galois p Galois

., Z p [[T 1,..., T d ]] G Q G Ql T., X := Spec(Z p [[T 1,..., T d ]][1/p]) x X, T x V x p Galois (, T x X p Galois V x Spf(Z p [[T 1,..., T d ]]) ). T, T Galois, T 1 Z p [[T 1,..., T d ]]. (T ) z(t ) (T ) (Q ), ε l (T ) (T ) (Q l ), x X V x, z(t ), ε l (T ) x z(v x ), ε l (V x ) z geom (V x ) = z(v x ) (V x ) (Q ), ε geom l (V x ) = ε l (V x ) (V x ) (Q l ). 1, z(t ), ε l (T ),. 2.1.2. Bloch- d = 0, Z p Galois T. X = Spec(Q p ) = {x} 1, V x = T [1/p]., V x, Q p z geom (V x ), ε geom l (V x ) (V x ),, T Z p (T ) (V x )., Q V x L p Bloch- ([BK90]), Q l (l = p Bloch- exponential ) p Perrin-Riou ([Pe95]).,,.., Q 1 p Galois Γ := Gal(Q(ζ p )/Q), Λ := Z p [[Γ]]. Z p [[[T ]] Zp Z p [(Z p /2p) ],., V p Galois, T Galois V Z p. Λ Galois Dfm(T ) := T Zp Λ Galois g x y T Zp Λ g(x y) := gx [ḡ] 1 y (, ḡ Γ g Q(ζ p ) [ḡ] Λ ḡ ). Dfm(T ) T. Shapiro, Q p Dfm(T ) Λ HIw(Q i p, T ) := H i (Q p, Dfm(T )) lim H i (Q p (ζ p n), T ) cor

(, Dfm( ) Iw. ε Iw (T ) := ε(dfm(t )), Iw (T ) := (Dfm(T ))).,., Dfm(T ) T, T., µ p n := {x Q x pn = 1}, G Q Z p Z p (1) := lim µ p n., Kummer 1 p n n ζ p n µ p n (1 ζ p n) Z[ζ p n, 1/p] c n H 1 (Z[1/p, ζ p n], Z p (1)) H 1 (Q(ζ p n), Z p (1)). 1 p n {ζ p n} n 1 ζ p p n+1, = ζ p n c := (c n ) n 1 H 1 Iw(Z[1/p], Z p (1)) H 1 Iw(Q, Z p (1)). ([Ka93a]), Dfm(Z p (1)) z Iw (Z p (1)) Iw (Z p (1)) (, Iw (Z p (1)) Λ Frac(Λ), Iw (Z p (1)) Mazur-Wiles, Rubin Q ). 2, ([Ka04]), ( ). f(τ) := q + n 2 a n (f)q n (τ C, Im(τ) > 0, q := exp(2πiτ)) N k 2 Hecke. Q C, Q Q p a n (f) Q p, Q p {a n (f)} n 2 Q p F f., Eichler-, Deligne, G Q F f 2 V f, L L(V f, s) f L L(f, s) := n 1 a n (f) n s (Re(s) >> 0). V f, p {c n,f H 1 (Z[1/Np, ζ p n], V f ) n 1} c f H 1 Iw(Z[1/Np], V f )., Dfm(Z p (1)) z Iw (V f ) Iw (V f ) Λ Frac(Λ) (Dfm(V f ) ) ([Ka04], [Na17b])., Frac(Λ), Q,

, Iw (V f ). z Iw (V f ) ([Na17b]). p Galois., p, p, F( ), Galois T F.,, Dfm(T F ) ( [Oc06] )., Mazur Galois, F p Galois T, p T p Galois Z p [[T 1,..., T d ]]/I (I ) R univ ) T univ (T ). p Galois, T univ z(t univ ) (T univ ) (Q ), ε l (T univ ) (T univ ) (Q l ). Galois ( Galois Galois ) R = T ( (Hecke T ) ), R univ T univ., R = T T univ,. 2.1.3.?, p Galois V z geom (V ) ε geom l (V ) (L ), p Galois., (2.1.1 ) Z p [[T 1,..., T d ]] Galois T. X := Spec(Z p [[T 1,..., T d ]][1/p])., X geom := {x X V x } X geom X, x X geom z geom (V x ) ε geom l (V x ) X, Galois., Q l, l p., Grothendieck, G Ql

p V Weil-Deligne W l (V ). V W l (V ) Deligne, Langlands ([De73]), Weil-Deligne, L l (W l (V )), ε l (W l (V )), V ε geom l (V ) (V )., l p G Ql p p. G Ql (l p) p = p,, Q l, l p ( [Ya09])., p ( Q ) l = p (G Qp p ) 2. G Qp 2 p., l = p. 2.1.4. l = p ( 1) G Qp p, G Qp p,. G Qp p V, Fontaine p ([Fo82], [Fo94]) Q p D crys (V ), D dr (V )., D crys (V ) Frobenius φ : D crys (V ) D crys (V ), D dr (V ) (Hodge ) {D i dr (V )} i Z. V Q p X H í et (X Q p Q p, Q p ), D dr (V ) X de Rham H i dr (X/Q p), X Z p X, D crys (V ) X Fp := X Zp F p H i crys(x Fp /Z p ) (. p Hodge!!). ( ), Fontaine = {crys, dr} dim Qp D (V ) = dim Qp (V ) V,, de Rham., X H í et (X Q p Q p, Q p ) de Rham, X Z p,., G Qp p Galois de Rham p. G Qp p = de Rham

, l = p p (!). ε geom p {de Rham } { p } (V ) (V ), de Rham V ε geom p (V ) (V )., l p Grothendieck l = p p ([Be02]) ( l = p!)., de Rham V Weil-Deligne W p (V ), V W p (V ) L p (W p (V )), ε p (W p (V )) l p. V W p (V ), l p V W l (V ) V, l = p V W p (V ) V., l = p ε geom p (V ) L p (W p (V )), ε p (W p (V )). ε geom p (V ),, D dr (V ) Hodge. D i dr (V )/D i+1 dr (V ) {0} i V Hodge-Tate, εgeom p (V ) V Hodge-Tate., ε geom p (V ), Bloch- exponential ([BK90]) exp V : D dr (V )/DdR(V 0 ) H 1 (Q p, V ) exponential exp V : H 1 (Q p, V ) D 0 dr(v ) ([Ka93a]).,, V G Q p, H 1 (Q, V ) loc p H 1 (Q p, V ) H 1 (Q, V ) loc p H 1 (Q p, V ) exp V DdR(V 0 ),, H 1 (Q, V ) L., ε geom p (V ). ε geom p (V ) = {L p (W p (V )) + ε p (W p (V )) + Hodge Tate + exp V + exp V } (, +, ) ( ).

1 p ( [Ka93b]) Dfm(V ) (V ) (Benois-Berger[BB08], Loeffler-Venjakob- Zerbes[LVZ15]) (trianguline ) ([Na17a]), V derham V W p (V ) (, 1 )., ε p (W p (V )) Gauss. Gauss p Galois,. W p (V ) ( ). 1([Na17b]),. 1 2 p ( ), F F p, G Qp F 2 T. R univ T, T univ V ( )., (T univ ) ε p (T univ ) (T univ ),, x Spec(R univ [1/p]) T univ x V x de Rham, ε p (T univ ) x ε p (V x ) ε p (V x ) = ε geom p (V x ). ε p (T univ )., ε p (V x ) = ε geom p (V x ) W p (V ),. ε p (V x ) = ε geom p (V x ), GL 2 (Q p ) p Langlands. 4. 2.2. 2.2.1.? p 3. A Q := Ẑ Z Q Q, π GL n (A Q ). L, π L L(π, s) L Λ(π, s) := L (π, s)l(π, s), Λ(π, s) ( ) Λ(π, s) = ε(π, s)λ(π, 1 s) (, π π )., ε(π, s), Q l π ε(π l, s) ε(π, s) = l ε(π l, s)

(, ). z(t ) (T ). S p. Q S l S Q Galois, Galois G Q,S := Gal(Q S /Q). T ( )Z p [[T 1,..., T d ]] G Q,S, T, T (1) := T Zp Z p (1)(T Tate ). T S (T )(G Q,S Galois ), l S T GQl l (T )., Galois Galois Poitou-Tate, S (T (1)) l S l (T ) R S (T ).,. T, T (1), z S (T ) S (T ), ε l (T ) l (T )., z S (T (1)) = l S ε l (T ) z S (T ) T ([Ka93b],[FK06])., z S (T ) z S (T (1)), p V z geom (V ) L L(V (1), s) s = 0.,., z(t ) ε p (T )., L L (π, s) (Hodge ) ε p (V ) Hodge-Tate. 2.2.2. 1 S = {p}, G Q,S Z p (1) Dfm(Z p (1))., z Iw S (Z p (1)) Iw S (Z p (1)), ([Ka93b]). 2.2.3. ( 2) ε Iw p (Z p (1)) Iw p (Z p (1)) 2, 2. 2.1.2 f, S := {l N} {p}., 2.1.2 z S Iw(V f) Iw S (V f), 1 Dfm(V f ) GQ p ε Iw p (V f ) Iw p (V f ) p ([Na17b]). 2 f z Iw S (V f )

3. GL 2 (Q p ) p Langlands GL 2 (Q p ) p Langlands, G Qp 2 p GL 2 (Q p ) p Banach., (Frobenius )Weil-Deligne 2 GL 2 (Q p ) GL 2 (Q p ) Langlands p., C, p Langlands G Qp GL 2 (Q p ) p., p Langlands. Breuil([Br03a],[Br03b], [Br04]), Colmez([Co10]) (φ, Γ) ([Fo91]) Galois GL 2 (Q p ), Berger-Breuil([BBr10]), Kisin([Ki10]), Pasukunas([Pa13]), Colmez- Dospinescu-Paskunas([CDP14])., Colmez G Qp 2 p ( ) GL 2 (Q p ) p Banach ( ) ( ). p, p. Emerton([Em11]) Kisin([Ki09]), p, G Q 2 p Galois V Fontaine-Mazur (Wiles -, ). GL 2 (Q p ) p Langlands 1. Emerton Kisin Fontaine-Mazur,,, (φ, Γ) (Colmez )., Colmez, GL 2 (Q p ) p Langlands! Colmez, 2 w := ( 0 1 1 0 ) GL 2 (Q p ), ( Langlands ),. 1 2! w. (φ, Γ), G Qp 2 p T, B GL 2 (Q p ) Π(T )

(, T ). Π(T ) w GL 2 (Q p ) p Langlands.. V G Qp 2 p, Π(V ) GL 2 (Q p ) Banach. Π(V ) Π(V ) := Hom cont F (Π(V ), F ) (F Π(V ) Q p ), x Π(V ), y Π(V ) [x, y] := x(y) F. Π(V ) y, x Π(V ) GL 2 (Q p ) g [g x, y] F. Π(V ) Π(V ) alg. Colmez Π(V ) alg {0} V de Rham regular (, V Hodge-Tate (, 2 ) k 2 > k 1 regular ). Colmez Emerton([Em11]),, GL 2 (Q p ) ( ) Π(V ) alg π LL (W p (V )) F Sym k 2 k 1 1 (F 2 ) F det k 1 (, π LL (W p (V )) Langlands W p (V ) GL 2 (Q p ) ( F ) ) ( Langlands )., GL 2 (Q p ) p Langlands ( ), Emerton W p (V ) ( π LL (W p (V )) supercuspidal ), ( ). 4. 2 1. (G Qp 2 p T ) ε p (T ), ε geom p (V ),. 4.1. ε p (T ) (w ) Kirillov (GL 2 (Q p ) smooth Q p ), GL 2 (Q p ) smooth π ( ε p (π) ), w GL 2 (Q p ) π., G Qp 2 p T, Banach Π(T ) w T ε p (T ) (T ).

, Dfm(T ) ε Iw p (T ) Iw (T ) ( ε p (T ) (T ) ). Dfm(T ) Iw (T ) HIw 1 (Q p, T ), HIw 1 (Q p, T ) Π(T ).,, V = T 2 p ( ) p 0 ( T ). g p := 0 1 ( ) 1/p 0, Π(V ) δ. Π(V ) Π(V ) 0 1/p g p (Π(V ) ) gp=1, g p δ (Π(V ) ) gp=δ. w. γ Γ w : (Π(V ) ) g p=1 ( ) χ(γ) 0 0 1 (Π(T ) ) g p=δ GL 2 (Q p ) (χ : Γ Z p p ), (Π(V ) ) g p=1 (Π(V ) ) g p=δ Λ[1/p] ( (Π(V ) ) g p=δ )., Colmez, Λ[1/p] (Π(V ) ) gp=1 H 1 Iw(Q p, V ), (Π(V ) ) gp=δ H 1 Iw(Q p, V (1)) (!)., w w : H 1 Iw(Q p, V ) H 1 Iw(Q p, V (1))., ε Iw p (V ) Iw (V ), Dfm(V ) Tate {, } Tate : H 1 Iw(Q p, V ) H 1 Iw(Q p, V (1)) Λ[1/p] 2 H 1 Iw (Q p, V ) (H 1 Iw (Q p, V ) 2 Λ[1/p] ) 2 H 1 Iw(Q p, V ) Λ[1/p] : x 1 x 2 {x 1, w x 2 } Tate. 4.2. ε geom p (V ) ( Langlands ) V regular 2 de Rham. 2.1.4. ε geom p (V ) (V ) 4.1 ε p (V ) (V ). V Weil-Deligne W p (V ) ( π LL (W p (V )) supercuspidal ),., ε geom p (V ), x H Iw (Q p, V ) α : H 1 iw(q p, V ) sp H 1 (Q p, V ) exp V D 0 dr(v )

α(x) ε p (W p (V )) 2, ε geom p (V ) ε p (W p (V )) + α(x) ε p (V ) x H Iw (Q p, V ) w : H 1 Iw (Q p, V ) H 1 Iw (Q p, V (1)) β : H 1 Iw(Q p, V (1)) sp H 1 (Q p, V (1)) exp V (1) D 0 dr(v (1)) β(w x) ( Hodge-Tate, ). ε p (V ) β(w x), ε p (V ) = ε geom p (V ), ε p (W p (V )) + α(x)? β(w x). 4.1.1 x (Π(V ) ) g p=1, w x (Π(V ) ) g p=δ Π(V ). Colmez Kirillov (B Π(V ) alg Q p ), Q p y α, y β Π(V ) alg, x (Π(V ) ) g p=1, x (Π(V ) ) g p=δ ( ) α(x) [x, y α ], β(x ) [x, y β ]. y α, y β,, Langlands Π(V ) alg π LL (W p (V )) F Sym k 2 k 1 1 (F 2 ) det k 1 π LL (W p (V )) Kirillov w y β y α ε p (π LL (W p (V ))). w y β ε p (π LL (W p (V ))) + y α GL 2 (Q p ) Langlands ε p (π LL (W p (V ))) = ε p (W p (V )), w y β ε p (W p (V )) + y α. ε p (V ) β(w x) [w x, y β ] [x, w y β ] ε p (W p (V )) + [x, y α ] ε p (W p (V )) + α(x) ε geom p (V )

ε p (V ) ε geom p (V ). Langlands ε p (V ) = ε geom p (V ), ε p (V ) = ε geom p (V )( V ),, Π(V ) alg w, Π(V ) alg smooth π LL (W p (V ))., ε p (V ) = ε geom p (V ) Langlands! 5. 1 ε p (V ) = ε geom p (V ) Langlands GL 2 (Q p ) p Langlands = G Qp 2. G Q 2, Emerton ([Em11]). ([CEGGPS16a], [CEGGPS16b], [GN17] ), p Langlands, = G Q 2. [BB08] D. Benois, L. Berger, Théorie d Iwasawa des représentations cristallines. II, Comment. Math. Helv. 83 (2008), no. 3, 603-677. [BBr10] L. Berger, C. Breuil, Sur quelques représentations potentiellement cristallines de GL 2 (Q p ), Astérisque 330, 2010, 155-211. [Be02] L. Berger, Représentations p-adiques et équations différentielles, Invent. Math. 148 (2002), 219-284. [BK90] S. Bloch, K. Kato, L-functions and Tamagawa numbers of motives. The Grothendieck Festschrift, Vol. I, 333-400, Progr. Math. 86, Birkhäuser Boston, Boston, MA 1990. [Br03a] C. Breuil, Sur quelques représentations modulaires et p-adiques de GL 2 (Q p ). I, Compositio Math. 138 (2003), 165-188. [Br03b] C. Breuil, Sur quelques représentations modulaires et p-adiques de GL 2 (Q p ). II, J. Inst. Math. Jussieu 2 (2003), 1-36. [Br04] C. Breuil, Invariant L et série spéciale p-adique, Ann. Scient. de l E.N.S. 37 (2004), 559-610. [CEGGPS16a] A. Caraiani, M. Emerton, T. Gee, D. Geraghty, V. Paskunas, S. Shin, Paching and the p-adic local Langlands correspondence, Cambridge Journal of Mathematics 4 (2016), no. 2, 197-287. [CEGGPS16b] A. Caraiani, M. Emerton, T. Gee, D. Geraghty, V. Paskunas, S. Shin, Patching and the p-adic Langlands program for GL 2 (Q p ), preprint. [Co10] P. Colmez, Représentations de GL 2 (Q p ) et (φ, Γ)-modules, Astérisque 330 (2010), 281-509.

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