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On logarithmic nonabelian Hodge theory of higher level in characteristic <span class="mathjax-formula">$p$</span>

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On logarithmic nonabelian Hodge theory of higher level in characteristic p

SACHIOOHKAWA(*)

ABSTRACT- Given a natural numbermand a log smooth integral morphismX!Sof fine log schemes of characteristicp>0with a lifting of its Frobenius pull-back X0!S modulo p2, we use indexed algebras AgpX, B(m‡1)X=S of Lorenzon-Montagnon and the sheaf D(m)X=S of log differential operators of level m of Berthelot-Montagnon to con- struct an equivalence between the category of certain indexed AgpX-modules with D(m)X=S-action and the category of certain indexed B(m‡1)X=S -modules with Higgs field.

Our result is regarded as a levelmversion of some results of Ogus-Vologodsky and Schepler.

MATHEMATICSSUBJECTCLASSIFICATION(2010). 16H05; 14F30, 32C38.

KEYWORDS. Log geometry, LogD-module, Higgs module, Cartier transform.

1. Introduction

For a projective smooth complex algebraic variety, Simpson [12] estab- lished a correspondence, which is called the Simpson correspondence nowa- days, between local systems and Higgs bundles. In [10], Ogus and Vologodsky studied an analogue of the Simpson correspondence for certain integrable connections or equivalently certain D-modules in positive characteristic. As a natural generalization of their theory, Schepler [11] studied its log version and Gros, Le Stum and QuiroÂs [4] studied its higher level version. The aim of this article is to establish the log and higher level version of the theory of Ogus- Vologodsky.

Let us recall the Ogus-Vologodsky's analogue of the Simpson correspondence in positive characteristic, which is called the global Cartier transform (see Theorem 2.8 of [10]). Let X!S be a smooth morphism of schemes of char- acteristic p>0. Let us denote by X0 the pull-back of X!S via the absolute

(*) Indirizzo dell'A.: Sachio Ohkawa, Graduate School of Mathematical Sciences, University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8914, Japan.

E-mail: ohkawa@ms.u-tokyo.ac.jp

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Frobenius FS of S. Denote the relative Frobenius morphism X!X0 by FX=S. LetTX0=S be the tangent bundle ofX0overS,STX0=S the symmetric algebra of TX0=S and Gthe nilpotent divided power envelope of the zero section of the co- tangent bundle ofX0=S, so thatOGˆG:T^ X0=S. Assume that we are given a lifting of X0!Smodulop2. Then there exists an equivalence between the category of OX-modules E with integrable connection r equipped with a horizontal OX- linear G-Higgs field u:OG!FX=SEndOX(E;r) extending the horizontal map c:STX0=S !FX=SEndOX(E;r) given by the p-curvature and the category of OX0-modulesE0 equipped with an OX0-linearG-Higgs field u:OG! EndOX0(E0).

There are two key technical results for the proof of the global Cartier transform.

One is the fact that the sheafD(0)X=S of differential operators of level 0 onXis an Azumaya algebra over its center, which is isomorphic to STX0=S via the p-cur- vature map. The other is a construction of the splitting module KX=S for this Azumaya algebra over the scalar extension OG of STX0=S. This means an iso- morphism of OX-algebras D(0)X=SSTX0=SOG! EndOG KX=S

. Then the global Cartier transform can be obtained by the Morita equivalence. Ogus-Vologodsky also constructed a splitting module over the completionS^TX0=S ofS:TX0=S under the assumption of an existence of a modp2 lifting ofFX=S and got an analogous equivalence called the local Cartier transform.

As is mentioned in the first paragraph, the theory of Ogus-Vologodsky has been generalized in (at least) two directions. First, Schepler [11] extended their theory to the case of log schemes. The difficulty for this generalization is that the Azumaya nature of the sheafD(0)X=Sof the log differential operators of level 0 is no longer true in general. Schepler overcame this difficulty by using Lor- enzon's theory of indexed modules and indexed algebras AgpX and BX=S asso- ciated to a log schemeXand its Frobenius pullbackX0!S. Roughly speaking, AgpX and BX=S are the suitable scalar extensions of the structure sheaf OX and OX0 respectively in the case of log schemes. He used the sheaf D~(0)X=S

AgpX OX D(0)X=S in place ofD(0)X=Sand proved the Azumaya nature of D~(0)X=S over its center. Schepler also generalized the splitting module KX=Sof Ogus-Vologodsky and got the log global Cartier transform. Second, in [4], Gros, Le Stum and QuiroÂs extended some results in [10] to the case of Berthelot's ring of differ- ential operators of higher level [2]. They proved the Azumaya nature of the sheaf D(m)X=S of differential operators of levelm, constructed a splitting module forD(m)X=S overS^TX0=S (hereX0denotes the pull-back ofX!Sby the (m‡1)-st iterate of the absolute Frobenius FS :S!S) under the assumption of an existence of a good lifting of the (m‡1)-st relative Frobenius morphism FX=S modp2, which they call a strong lifting, and proved the local Cartier transform of higher level. They also constructed (but informally) a global splitting module by a gluing argument. But their construction is different from that of Ogus- Vologodsky. It should be remarked here that the sheaf D~(0)X=S used by Schepler (or more generally the sheafD~(m)X=S of log differential operators of higher level) was introduced by Montagnon [9]. She established there the foundations of log

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differential operators of higher level and especially obtained the log version of Berthelot's Frobenius descent by using the indexed algebras AgpX and B(m)X=S, where the latter denotes the higher level version of Lorenzon's BX=S.

The purpose of this paper is to generalize Schepler's log global Cartier transform to the case of higher level by using the indexed algebras AgpX and

B(m‡1)X=S of Lorenzon and Montagnon. Our construction is a natural general-

ization of Ogus-Vologodsky and Schepler, but we also need some log differ- ential calculus of higher level which is based on Montagnon's result. We also prove the compatibility of the log global Cartier transform with Montagnon's log Frobenius descent.

Let us describe the content of each section. We work with a log smooth morphismX!Sof fine log schemes in positive characteristic. LetFX=Sdenote the (m‡1)-st relative FrobeniusX!X0. In the second section, we review the theory of indexed modules. In the third section, we construct the log version of the higher curvature map b:TX0=S!FX=SD(m)X=S, which we call the pm‡1-curvature map, in Definition 3.10 after reviewing the theory of log differential operators of levelm. In the fourth section, after reviewing the construction and some basic results of in- dexed algebras associated to the log structure, we study the Azumaya nature of D~(m)X=S. We prove thatB(m‡1)X=S OX0 S:TX0=Sis identified with the center ofD~(m)X=Svia the pm‡1-curvature map (see Theorem 4.16) and D~(m)X=S is an Azumaya algebra over B(m‡1)X=S OX0 S:TX0=S (see Corollary 4.2-). We also prove the log Cartier descent theorem of higher level as an application (see Theorem 4.26). In the fifth section, we construct the splitting module K(m);AX=S forD~(m)X=S overB(m‡1)X=S OX0 G^:TX0=S under the assumption of an existence of a modp2lifting ofX0!S(see (18)) and get the log global Cartier transform of higher level by using the indexed variant of the Morita equivalence (see Theorem 5.19). In the final section, we consider the compatibility of the log global Cartier transform with Montagnon's log Frobenius descent. Our new ingredient is to prove the behavior of the splitting moduleK(m);AX=S with respect to the Frobenius descent functor of Montagnon (see Theorem 6.10).

As a consequence of Theorem 6.10, we obtain the expected compatibility (see Theorem 6.8).

2. Indexed Azumaya Algebra

In this section, we give a review of the theory of indexed modules and indexed Azumaya algebras developed by ([5], see also [11]) which we will use to construct the log global Cartier transform of higher level. The general theory of indexed modules can be developed on a ringed topos but, for simplicity, we only consider the case of the ringed topos associated to the eÂtale site of a scheme and its structure sheaf. Also, we try to describe several notions more concretely than those given in [5] and [11]. We fix throughout this section a schemeXand an eÂtale sheaf of abelian groupsI.

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2.1 ±Indexed module

Let us recall some notions on indexed modules.

DEFINITION2.1. (1) AnI-indexed sheaf onXis a sheaf of sets overI, namely, a map of sheaves F ! I. We denote the mapF ! I bypF. AnI-indexed sheaf of abelian groups onXis anI-indexed sheafF ! I onXequipped with an addition mapF IF ! FoverI, a unit mapI ! FoverIand an inverse mapF ! Fover I satisfying the usual axioms of abelian groups.

(2) AnI-indexedOX-module is anI-indexed sheaf of abelian groups equipped with a scalar multiplication map OX F ! F over I satisfying the usual asso- ciativity, distributivity and unitarity conditions, where OX F is regarded as a sheaf overI via the compositeOX F ! F ! I.

(3) AnI-indexedOX-algebra is anI-indexedOX-module Aequipped with an OX-bilinear multiplication mapp:A A ! A over the addition map I I ! I and a global section 1A of Aover the zero section 0:e! I satisfying the usual associativity and unitarity conditions. We say an I-indexed OX-algebra A is commutative if the multiplication map p satisfies psˆp where s is the iso- morphismA A ! A Adefined by (a;b)7!(b;a).

(4) For an I-indexed OX-algebraA, anI-indexedA-algebra is anI-indexed OX-algebraBequipped with a morphismA ! BofI-indexedOX-algebras.

REMARK2.2. LetAbe anI-indexed sheaf onX. For an eÂtale openUofXand a sectioni2 I(U), we denote byAithe pullbackhUIAwherehU is an eÂtale sheaf onXrepresented byUandhU ! Iis the sectioni. We callAithe fiber ofA ! Iat i2 I(U). Note thatAiis naturally considered as an eÂtale sheaf onU, and more- over, if A is an I-indexed OX-module, then Ai has an OU-module structure naturally induced by theI-indexedOX-module structure onA. IfAis anI-indexed OX-algebra, the multiplication mappofAis equivalent to the following data: for each eÂtale open U of X and sections i;j2 I(U), a morphism of OU-modules pij:AiOUAj! Ai‡j functorial with respect toi;jsatisfying the obvious condi- tions of associativity and unitarity.

Now we recall the definition ofJ-indexedA-modules.

DEFINITION2.3. LetAbe anI-indexedOX-algebra. LetJ be an eÂtale sheaf of I-sets, that is, an eÂtale sheaf of sets on X equipped with an I-action map I J ! J;(i;j)7!i‡j. AJ-indexed leftA-module is aJ-indexedOX-moduleE equipped with anOX-bilinear mapr:A E ! Eover theI-action mapI J ! J satisfying the usual associativity and unitarity conditions. We can similarly define the notion ofJ-indexed rightA-module.

REMARK2.4. LetAbe anI-indexedOX-algebra andJ be an eÂtale sheaf ofI- sets on X. Let E be a J-indexed left A-module. Then the structure morphism

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r:A E ! E over I J ! J is equivalent to the following data: for each eÂtale open U of X, and each section (i;j)2 I J, a morphism of OU-modules rij:AiOUEj! Ei‡j;ae7!aefunctorial with respect toi;jsatisfying the ob- vious conditions of associativity and unitarity.

Next we recall the definition of tensor products and internal hom objects as an indexed module.

DEFINITION2.5. LetAbe anI-indexedOX-algebra andJ,Kbe eÂtale sheaves of I-sets onX.

(1) LetEbe aJ-indexed rightA-module andFaK-indexed leftA-module. Let J IKbe theI-setJ K=, whereis the equivalence relation generated by the relation (i‡j;k)(j;i‡k) for i2 I;j2 J;k2 K. Then we define aJ IK- indexed sheaf of abelian groups E AF (the tensor product of E andF) as the object representing the functor which sends J IK-indexed sheaf of abelian groups M to the set of biadditive A-balanced morphisms E F ! Mover the natural projectionJ K ! J IK. Concretely this is the eÂtale sheaf onXasso- ciated to the presheaf

U7 ! G

l2J IK(U)

M

(j;k)ˆl

Ej(U)OX(U)Fk(U)

!

=R

endowed with the natural projection toJ IK, whereRis theOX(U)-submodule generated by

xay xay

x2 E(U); y2 F(U) anda2 A(U) satisfying (pE(x)‡pA(a);pF(y))ˆl

. When A is commutative, thenE AF naturally forms aJ IK-indexedA-module.

(2) For aK-indexed leftA-module F andW2HomI(J;K), we define theJ- indexedA-moduleF(W) by the eÂtale sheafF K;WJwith the second projection and theA-action via the action onF.

(3) LetEbe aJ-indexed leftA-module andF aK-indexed leftA-module. We define the internal hom object ofEandF, which we denote byHomA(E;F), as the eÂtale sheaf onX

U7 ! G

W2HomI…J;K†(U)

HomA EjU;FjU(W)

endowed with the natural projection toHomI(J;K), where HomAdenotes the set of homomorphism of J-indexed A-modules. When A is commutative, then HomA(E;F) naturally forms a HomI(J;K)-indexed A-module. Also, we denote HomA(E;E) simply byEndA(E).

Finally we recall the local freeness and faithful flatness as an I-indexed A- module.

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DEFINITION2.6. LetAbe anI-indexedOX-algebra and letBbe aJ-indexed A-algebra.

(1) We say that anI-indexedA-moduleEis locally free of rankkif eÂtale locally onXthere exist sectionsn1;. . .;nkofI ˆ HomI(I;I) such thatEis isomorphic to Lk

iˆ1A(ni), whereA(ni) are as in Definition 2.5 (2).

(2) We say thatBis faithfully flat overAif the functorE 7! E ABis exact and faithful.

2.2 ±Indexed Azumaya algebra

The following proposition due to Schepler (see [11]) is an index version of the Morita equivalence.

PROPOSITION2.7. LetAbe a commutativeI-indexedOX-algebra. LetJ be an eÂtale sheaf of I-sets on X and M be a locally free I-indexedA-module of finite rank. We denoteEndA(M)byEwhich is anI-indexedOX-algebra in natural way.

Then the functor E7 !MAE is an equivalence of categories between the category ofJ-indexedA-modules and the category ofJ-indexed leftE-modules.

PROOF. The quasi-inverse ofE7 !MAEis given byF7 ! HomA(M;F). For

more details, see Theorem 2.2 of [11]. p

Now let us recall the notion on indexed Azumaya algebra.

DEFINITION2.8. Let Abe a commutative I-indexedOX-algebra andE anI- indexedA-algebra. Then, for a commutativeI-indexedA-algebraB,Esplits overB with splitting module M if there exists anI-indexed locally freeB-module M of finite rank such thatE AB  EndB(M).Eis an Azumaya algebra overAof rankr2 if there exists a faithfully flatI-indexedA-algebraBsuch thatEsplits overBwith splitting moduleMof rankr.

If we know thatEis an Azumaya algebra overA, then we can find a splitting module forEoverAin certain case by the following proposition.

PROPOSITION 2.9. Let A be a commutative I-indexed OX-algebra and E an Azumaya algebra over Aof rank r2. If there exists a locally freeI-indexedA- module M of rank r with a structure ofI-indexed leftE-module compatible with the given I-indexed A-module structure, then E splits over A with splitting module M.

PROOF. See Corollary 2.5 of [11]. p

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3. Thepm‡1-curvature map

From this section, we are mainly concerned with log schemes. Our aim of this section is to construct thepm‡1-curvature map for a log smooth morphismX!S of fine log schemes defined over a field of positive characteristic, which generalizes the classicalp-curvature map.

3.1 ±Logarithmic differential operators of higher level

In this subsection, we briefly recall the log version of Berthelot's theory of differential operators of higher level which is studied by Montagnon. For more details, see [2] and [9].

Let us start with basics on log schemes [5]. A pre-log structure on a schemeXis a pair (MX;aX) whereMX is a sheaf of monoids on the eÂtale site ofXandaX is a homomorphism from MX to the multiplicative monoid OX. A pre-log structure (MX;aX) is a log structure ifaXinduces an isomorphism fromaX1 OX

toOX. A log scheme is a pair of a schemeXand a log structure (MX;aX). We usually denote a log scheme by a single letter such asX and the log structure ofXbyMX. For a schemeX, the natural forgetful functor from the category of log structures onXto that of pre-log structures onXhas a left adjoint functor (see (1.3) of [5]). We denote by (MaX;aaX) the log structure defined by the image of a pre-log structure (MX;aX) under this left adjoint functor. We call (MaX;aa) the log structure associated to (MX;aX). A monoidP is integral if the natural map fromPto the groupPgpas- sociated to P is injective. It is fine if it is finitely generated and integral. A log schemeXis fine if, eÂtale locally onX, there exists a fine monoidPwith a morphism PX ! MX of monoids such that the log structure of X is isomorphic to the log structure associated to a pre-log structurePX ! MX ! OX. HerePX denotes the constant eÂtale sheaf onX defined by P. Fine log schemes form a category in an obvious way. This category has all finite projective limits (see (2.8) of [5]). A morphism of log schemesf :X!Yis strict if the natural morphismfMY ! MX

induced by f is an isomorphism, wherefMY denotes the log structure onXas- sociated to a pre-log structuref 1MY ! MX ! OX. It is an exact closed immer- sion if it is strict and the underlying morphism of schemes is a closed immersion.

One can define a log smooth (resp. log eÂtale) morphism of fine log schemes in terms of local infinitesimal liftings in the category of fine log schemes (see Subsection 3 of [5]). Let (X;MX)!(S;MS) be a morphism of log schemes. Then we define the module of log differentialsV1(X;MX)=(S;MS)by the quotientV1X=S OXZMgpX

=N.

Here V1X=S is the module of differentials of the underlying morphism of schemes X!SandN is theOX-submodule locally generated by the sections of the form (daX(a);0) (0;aX(a)a) witha2 MX and (0;1a) witha2Im(fMS! MX).

From now on, we simply denote the module of log differentials ofX!SbyV1X=S. If X!S is a log smooth morphism of fine log schemes, then its module of log dif- ferentialsV1X=S is a locally freeOX-module of finite rank.

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From now on, all log schemes are assumed to be defined overZ(p). Let us recall the definition of them-PD structure.

DEFINITION3.1. LetX be a log scheme andIa quasi-coherent ideal ofOX. A divided power structure of levelm(m-PD structure) onIis a divided power ideal (J;g) ofOX such that

I(pm)‡pIJI

and the divided power structuregonJis compatible with the unique one onpZ(p). HereI(pm)denotes the ideal ofOXgenerated bypm-th powers of all sections ofI. If (J;g) is an m-PD structure on I, we call (I;J;g) an m-PD ideal of OX and call (X;I;J;g) anm-PD log scheme.

Let (X;I;J;g) be anm-PD log scheme. For each natural numberk, we define the map I! OX; f7!ffkg(m) by ffkg(m):ˆfrgq(fpm) where kˆpmq‡r and 0r<pm. These maps satisfy the following formulas (see p. 13 of [9]).

PROPOSITION 3.2. Let(X;I;J;g) be an m-PD log scheme and k;l be positive integers.

(1) For any x2I;xf0g(m)ˆ1;xf1g(m)ˆx, and xfkg(m) 2I:Moreover if kpm, then xfkg(m) 2J:

(2) For any x2I and a2 OX,(ax)fkg(m)ˆakxfkg(m). (3) For any x;y2I,(x‡y)fkg(m)= P

k0‡k00ˆk

kk0 xfk0g(m)yfk00g(m): (4) For any x2I, qk!xfkg(m)ˆxk.

(5) For any x2I,(xfkg(m))flg(m)ˆ qkl!

(qk!)lql!xfklg(m).

In the following, we sometimes denote an element ffkg(m) simply by ffkg, if there will be no confusions. For a while, we fix an m-PD fine log scheme (S;a;b;g) (i.e. S is a fine log scheme) on which p is locally nilpotent and a log smooth morphism X!S of fine log schemes. We assume that g extends to X (for definition, see [2] DeÂfinition 1.3.2(1)). Note that g always extends to X in the case bˆ(p) (see [2] DeÂfinition 1.3.2(1)), which is the case of our interest.

To recall the sheaf of log differential operators of higher level, we need the log m-PD envelope. The construction of the logm-PD envelope is the same as the classical case of level 0, which we explain now: Let i:X,!Y be an immersion of fine log schemes overS. EÂtale locally onX, we have a factorizationiˆgi0with an exact closed immersion i0:X,!Z and a log eÂtale morphism g:Z!Y. Let i00:X,!Dbe the usualm-PD envelope ofi0(for definition, see [2]), and endowD with the inverse image log structure of Z. Then, since i00 satisfies the obvious universal property, it descents to the exact closed immersionX,!PX;(m)(Y) with

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the m-PD structure globally on X. PX;(m)(Y) is called the logm-PD envelope of i:X,!Y.

Let us consider the diagonal immersionX!XSX. We simply denote its log m-PD envelope byPX=S;(m)and the defining ideal ofX,!PX=S;(m)byI. Then there exists the m-PD-adic filtration Ifng

n2N associated toI (for definition, see [3]

DeÂfinition A.3) which satisfies the following property.

If xis a local section ofIfng; then xfkg is inIfnkg: …1†

LetPX=S;(m)denote the structure sheaf ofPX=S;(m). For each natural numbern, we denote by PnX=S;(m) the quotient sheaf PX=S;(m)Ifn‡1g and by PnX=S;(m) the closed subscheme ofPX=S;(m) defined byIfn‡1g. We have a sequence of surjective homo- morphisms of sheaves

! PnX=S;(m) ! PnX=S;(m)1 ! ! P1X=S;(m)! P0X=S;(m):

Let p0 and p1 (resp. pn0 and pn1) denote the first and second projection PX=S;(m)!X(resp.PnX=S;(m)!X) respectively.

DEFINITION3.3. Letn;mbe natural numbers. The sheaf of differential opera- tors of levelmof ordernis defined by

D(m)X=S;n:ˆ HomOX(pn0PnX=S;(m);OX):

The sheaf of differential operators of levelmis defined by D(m)X=S:ˆ [

n2N

D(m)X=S;n:

REMARK3.4. Since, for any m0m, an m-PD ideal can be considered as an m0-PD ideal,

D(m)X=S m0 naturally forms an inductive system.

D(m)X=S has the (non commutative) ring structure as follows. By using the uni- versality of m-PD envelope, we obtain the canonical homomorphism of OX-alge- bras

dn;nm 0:Pn‡nX=S;(m)0 ! PnX=S;(m)OXPnX=S;(m)0

for each natural numbern;n0, which is induced by the projectionXSXSX! XSX to the first and the third factors (for precise definition ofdn;nm 0, see Sub- section 2.3.2 of [9]). For each F2 D(m)X=S;n andC2 D(m)X=S;n0, we define the product FC2 D(m)X=S;n‡n0by

Pn‡nX=S;(m)0 ƒƒƒ!dn;n

0

m PnX=S;(m)OXPnX=S;(m)0 ƒƒƒ!idC PnX=S;(m)ƒ!F OX:

This is well-defined andD(m)X=Sforms a sheaf of non commutativeOX-algebras onX.

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REMARK3.5. LetEbe anOX-module. Then a logm-PD stratification onEis a family ofPnX=S;(m)-linear isomorphismsen :pn0 E ! pn1 Esatisfying the usual cocycle conditions. As is the same with the classical case, giving a D(m)X=S-action on E extending itsOX-module structure is equivalent to giving a logm-PD stratification onE.

Finally we recall the local description of D(m)X=S. Letjdenote the logm-PD en- velopeX,!PX=S;(m)of the diagonalX!XSX. We have an exact sequence

0!j 1(1‡I)ƒ!l j 1MPX=S;(m) ƒ!j MX !0;

…2†

where l is the restriction of the log structure j 1(aPX=S;(m)1 ):j 1(PX=S;(m) )! j 1(MPX=S;(m)). For any sectiona2 MX,p0(a) andp1(a) have the same image inMX. Thus, from the exact sequence (2), there exists a unique sectionm(m)(a)2j 1(1‡I) such that p1(a)ˆp0(a)l m(m)(a)

. Log smoothness ofX!Simplies that, eÂtale locally onX, there is a logarithmic system of coordinatesm1;. . .;mr2 MgpX, that is, a system of sections such that the setfdlogm1;. . .;dlogmrgforms a basis of the log differential module V1X=S of X over S. We define h(m)i :ˆm(m)(mi) 1 and hfkg(m):ˆQr

i:ˆ1hfki ig(m)for each multi-indexk2Nr.

PROPOSITION-DEFINITION 3.6. We regard PnX=S;(m) as an OX-module via pn0. Then the setfhfkg(m)jkj ngforms a local basis ofPnX=S;(m)overOX. We denote the dual basis of

hfkg(m)jkj n by

@hki(m)jkj n . We also denote hfkg(m) (resp.

@hki(m))byhfkg (resp.@hki)simply, if there will be no confusions.

PROOF. See Proposition 2.2.1 of [9]. p

PROPOSITION 3.7. Let X!S be a log smooth morphism of fine log schemes.

Assume that we are given a logarithmic system of coordinates m1;. . .;mr2 MgpX. (1) D(m)X=S is locally generated by

@heii; @hpeii;. . .; @hpmeii1ir as an OX- algebra.

(2) We have

@hk0i@hk00iˆ kX0‡k00

kˆsupfk0;k00g

k!

(k0‡k00 k)!(k k0)!(k k00)!

qk0!qk00! qk! @hki: In particular,@hki@hk0iˆ@hk0i@hkiholds.

(3) For any x2 OX, we have

@hki:xˆX

ik

ki @hk ii(x)@hii inD(m)X=S:

(4) The natural mapD(m)X=S! D(mX=S0) sends@hki(m)toqq!0!@hki(m0), where kˆpmq‡r , k0ˆpm0q0‡r0with0r<pmand0r0<pm0.

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PROOF. (1) See Proposition 2.3.1 of [9]. (2) See Lemme 2.3.4 of [9]. (3) See (2.5)

of [9]. (4) See (2.6) of [9]. p

We prove the following lemma needed later.

LEMMA3.8. Let X!S be a log smooth morphism of fine log schemes defined overZ=pZ. For any k2Nr, l2Nand1ir, we have

@hpm‡1ki@hle

iiˆ@hpm‡1k‡leii:

PROOF. We may assume 1lpm‡1. Whenkiˆ0, the assertion follows easily from Proposition 3.7 (2). Thus we may also assumeki1. By Proposition 3.7 (2), we have

(|) @hpm‡1ki@hle

iiˆXl

sˆ0

(pm‡1ki‡s)!

(l s)!s!(pm‡1ki l‡s)!

(pki)!ql!

(pki‡qs)!@hpm‡1k‡seii: We put

A:ˆ (pm‡1ki‡s)!

(l s)!s!(pm‡1ki l‡s)!2Z andB:ˆ (pki)!ql! (pki‡qs)!2Q:

First, we consider the casesˆl. Then, we have ABˆ(pm‡1ki‡l)!

l!(pm‡1ki)!

(pki)!ql! (pki‡ql)!

ˆYl

jˆ1

1‡pm‡1ki j

Yql

jˆ1

1‡pki

j 1

:

Since 1‡pm‡1j ki21‡pZ(p) if 1jpm‡1 1,1‡ppm‡1m‡1kiˆ1‡ki if jˆpm‡1, (1‡pkji) 121‡pZ(p) if 1jp 1 and (1‡pkpi) 1ˆ(1‡ki) 1 if jˆp, we have AB21‡pZ(p) and thus AB1 mod p. Next, we consider the case 0sl 1;lˆpm‡1. Then, we have

Bˆ (pki)!ql! (pki‡qs)!ˆYqs

jˆ1

1

(pki‡j)p!2pZ(p):

HenceAB2pZ(p). We thus haveAB0 modp. Finally, we consider the case 0sl 1;0lpm‡1 1. Then, we have

BˆYqs

jˆ1

1

(pki‡j)ql!2Z(p):

Let v:Q !Z denote the normalized p-adic valuation. For any n2N, it is

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known that (p 1)v(n!)ˆn s(n), wheres(n):ˆP

jajifnˆP

jajpj. Thus, we have

(p 1)v(A)ˆs(l s)‡s(s)‡s(pm‡1ki l‡s) s(pm‡1ki‡s)

ˆs(l s)‡s(pm‡1ki l‡s) s(pm‡1ki)

>0:

Hence AB2pZ(p). We thus have AB0 modp. The assertion follows from

these calculations and (|). p

3.2 ±The pm‡1-curvature map

Throughout this subsection, all the log schemes are assumed to be defined over Z=pZ. Let us introduce some notations. For a log scheme X, FX denotes the (m‡1)-st iterate of its absolute Frobenius. For a morphism X!S of fine log schemes, we consider the following commutative diagram:

whereX00is the fiber product in the category of fine log schemes, and the morphism X!X0(denoted byFX=Sand called the ((m‡1)-st) relative Frobenius morphism) is uniquely determined by the requirement that the morphismFX=Sis purely in- separable and X0!X00 is log eÂtale (see Proposition 4.10 of [5]). We denote the compositionX0!X00!XbypX=S or simply byp. We also denoteX0byX(m‡1), if there is a risk of confusion.

First we prove the log levelmversion of Mochizuki's theorem which is used to construct thepm‡1-curvature map (see also Proposition 3.2 of [4] and Proposition A.7 of [11]).

THEOREM3.9. Let X!S be a log smooth morphism of fine log schemes. Let PX=S;(m)(resp. Y) be the log m-PD envelope (resp. the log formal neighborhood) of the diagonal immersion X !XSX andI (resp. I) its defining ideal. LetPX=S;(m) denote the structure sheaf of PX=S;(m). Then there is an isomorphism ofOX-modules

a:FX=SV1X0=S!I=Ifpm‡1‡1g‡IPX=S;(m) such that, for anyj2I with imagev2I=I2V1X=S,

a(1pv)ˆjfpm‡1g: …3†

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PROOF. First we show that the mapa0:I!I=IPX=S;(m) defined by I ! I=IPX=S;(m)

j 7 ! jfpm‡1g

isFX-linear and zero onI2. Ifjandtare local sections ofI, by Proposition 3.2 (3) we have

(j‡t)fpm‡1gˆjfpm‡1g‡tfpm‡1g‡ X

i‡jˆpm‡1 i;j>0

pm‡1 i

jfigtfjg:

Since 0<i;j<pm‡1, we have qi;qj <p, where qi;qj are as in Subsection 1.3.

Therefore qi! and qj! are invertible. From Proposition 3.2 (4) we have jfigtfjg ˆ(qi!qj!) 1jitj2IPX=S;(m). It follows that the last term in the sum is in IPX=S;(m)and we see the additivity ofa0. Similarly, the fact thata0isFX-linear and zero onI2follows from Proposition 3.2 (2), (5). We thus obtain theOX-linear map

a:FX=SV1X0=SFXV1X=S !I=Ifpm‡1‡1g‡IPX=S;(m)

which satisfies (3). Let us show thatais an isomorphism. Since the assertion is eÂtale local on X, we may assume that we have a logarithmic system of coordinates m1;. . .;mr2 MgpX. Then the left hand side is isomorphic toLr

iˆ1OX…1pdlogmi†.

On the other hand, by Proposition-Definition 3.6,I=Ifpm‡1‡1g is freely generated by n

hfigj1 jij pm‡1o

as an OX-module and the image of IPX=S;(m) under the mapIPX=S;(m)!I=Ifpm‡1‡1g is generated byfhjhfigj0 jij pm‡1 1;1jrg as an OX-module. Actually I=(Ifpm‡1‡1g‡IPX=S;(m)) is freely generated by nhfpi m‡1g1iro

as an OX-module. So the right hand side is isomorphic to Lr

iˆ1OXhfpi m‡1g and, by construction,a sends 1pdlogmi tohfpi m‡1g. This com-

pletes the proof. p

Letadenote the map defined by the composite PnX=S;(m) ! OX ! PnX=S;(m);

where the first map is the natural projection and the second one is the structural morphismpn0 . Now, we are ready to define thepm‡1-curvature map.

DEFINITION3.10. LetX!Sbe a log smooth morphism of fine log schemes. Let TX0=S:ˆ HomOX0(V1X0=S;OX0) denote the log tangent bundle onX0. We define the mapb:TX0=S!FX=SD(m)X=Sby sendingD2 TX0Sto the composition of maps

PX=S;(m)pm‡1 ƒƒƒƒƒƒy7!y a(y)!I=Ifpm‡1g!I=Ifpm‡1‡1g‡IPX;m

 FX=SV1X0=S ƒƒƒƒƒ!F

X=S D

OX; where the second map is the natural projection and the third one is the isomorphism in Theorem 3.9. We call it thepm‡1-curvature map.

The local description of thepm‡1-curvature map is the following.

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PROPOSITION3.11. Let X!S be a log smooth morphism of fine log schemes.

Assume that we are given a logarithmic system of coordinates m1;. . .;mr2 MgpX . Letnj0i1iro

denote the dual basis ofpdlogmi1ir

. Thenbsendsj0i to@hpm‡1eii.

PROOF. We calculate thatb(j0i) sendshfkgto 1 ifkˆpm‡1eiand 0 otherwise by

construction ofb, thereby completing the proof. p

REMARK3.12. Whenm is equal to 0, ourpm‡1-curvature map is the usual p- curvature map ([10] Proposition 1.7). If the log structure ofX is trivial, then our pm‡1-curvature map coincides with thepm-curvature map studied in [4] section 3.

4. Azumaya algebra property

The goal of this section is the Azumaya algebra property of the indexed version of the sheaf of log differential operators D~(m)X=Sˆ AgpX OXD(m)X=S defined by Mon- tagnon [9]. We also study the Azumaya nature of D~(0)X(m)=Sˆ B(m)X=SOX(m) D(0)X(m)=S, which is also introduced by Montagnon. At first we give a review of the canonical indexed algebraAgpX associated to the log structure ofXintroduced by Lorenzon [5] and Montagnon'sD~(m)X=SandD~(0)X(m)=S.

4.1 ±Indexed algebra associated to a log structure 4.1.1 ± TheIgpX-indexed algebraD~(m)X=S

First we recall the definition ofAgpX (I, 3.1 of [5]). LetXbe a fine log scheme. We consider the extension of sheaves of abelian groups

0 ! OX ! MgpX !d IgpX !0:

HereIgpX is the quotient sheafMgpX=OX. We defineAgpX as the contracted product MgpX ^OX OX which is the quotient of MgpX OX by the equivalence relation (ax;y)(x;ay) wherea;x;yare local sections ofOX;MgpX andOXrespectively. The projectionMgpX OX ! MgpX ! IgpX induces a mapAgpX ! IgpX which makesAgpX an IgpX-indexedOX-module. For a local sectioniofIgpX, the fiberMgpX;iofMgpX ! IgpX ati is anOX-torsor. This implies that the fiberAgpX;iofAgpX ! IgpX atiis an invertibleOX- module.AgpX has a multiplication map induced by the addition mapMgpX MgpX ! MgpX overIgpX IgpX ! IgpX. HenceAgpX forms anIgpX-indexedOX-algebra, called the IgpX-indexed algebra associated to the log structure.

Next let us recall the definition of the sectionesofAgpX associated to a sections ofMgpX. For each eÂtale openUofXand a sections2 MgpX(U),strivializes theOX-

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torsorMgpX;d(s). Thus it gives a basises:ˆ(s;1) of the invertibleOU-moduleAgpX;d(s). Then

e0ˆ1; esetˆes‡t; aes ˆeas fors;t2 MgpX(U) anda2 OX(U).

The construction of AgpX is functorial in the following sense. For a morphism f :X!Yof fine log schemes, we have a commutative diagram

where vertical arrows are isomorphisms iff is strict. This induces a commutative diagram

where horizontal arrows are isomorphisms if f is strict. So we get the following proposition.

PROPOSITION4.1. If f :X!Y is a strict morphism of fine log schemes, then Agpf :fAgpY ! AgpX is an isomorphism ofIgpX-indexed algebras.

Next we recall the definition ofIgpX-indexed leftD(m)X=S-module structure onAgpX (Subsection 4.1.1 of [9]). Let be the trivial sheaf of abelian groups on X. W e naturally regardD(m)X=Sas a-indexedOX-algebra andIgpX as a sheaf of-sets. Since the natural projections pni :PnX;(m)!X with iˆ0;1 are strict, we have the iso- morphism ofIgpX-indexedOX-algebras

en :pn1 AgpX ! APnX=S;(m)  pn0 AgpX:

These isomorphisms are compatible with respect tonby construction and satisfy the cocycle condition. Hence we can define an IgpX-indexed left D(m)X=S-module structure onAgpX by

D(m)X=S AgpX ,! D(m)X=Sp1AgpX ƒƒƒide!D(m)X=Sp0AgpX ,! HomOX PX=S;(m);OX

AgpX OXPX=S;(m)! AgpX: By calculation with the sectiones s2 IgpX

, one can see that the action ofD(m)X=S onAgpX satisfies the Leibniz formula (for more details, see Subsection 4.1 of [9]).

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Therefore we have the following nontrivial ring structure on D~(m)X=S which is a central object in this article.

PROPOSITION-DEFINITION4.2. Let X!S be a log smooth morphism of fine log schemes. Let D~(m)X=S denote theIgpX-indexedOX-moduleAgpX OXD(m)X=S. Then there exists a unique IgpX-indexed OX-algebra structure on D~(m)X=S such that the maps AgpX !D~(m)X=S; a7!a1 and D(m)X=S!D~(m)X=S; P7!1P are homomorphisms and that for any a2 AgpX, P2 D(m)X=S and k2Nr, we have the relations aPˆ (a1)(1P)and

(1@hki)(a1)ˆX

ik

k i ( )

(@hk ii:a)@hii: Heref@hkigis as in Proposition-Definition3.6.

PROOF. See Subsection 4.1 of [9]. p

REMARK4.3. In [9], Montagnon definesD~(m)X=S byAgpX OX;I D(m)X=S;I, whereOX;I resp:D(m)X=S;I

denotes an I-indexed OX-module OX I resp:D(m)X=S I with the second projection. So, in Montagnon's definition of D~(m)X=S, if we take a section aP2D~(m)X=S, thenPmay have a nontrivial index. It seems to us thatPmust have the trivial index. For example, equation (4) in the following Proposition 4.4 should actually be considered as an equation inD~(m)X=S. If@hkihas a nontrivial index, then (4) does not make sense because both sides of the equation must have the same index. If we defineD~(m)X=S:ˆ AgpX OXD(m)X=Sby regardingD(m)X=Sas a-indexedOX-algebra in a natural way, then equation (4) makes sense (both sides have the same indexQ

imiji).

Therefore, it seems to us that the natural definition of D~(m)X=S is AgpX OXD(m)X=S. However, this is not serious. Actually, if we replace in [9] AgpX OX;ID(m)X=S;I by AgpX OX D(m)X=S (and also modify the definition of B(m)X=S andF(E), see Proposition- Definition 4.7 and Subsection 6.1 respectively), then all equations in [9] make sense and all the proofs are correct without any essential changes.

Finally we recall the following formula needed later. Letm1;. . .;mr2 MgpX be a logarithmic system of coordinates. Fori2 f1;2;. . .;rgand a multi-indexj, we put ui:ˆemi anduj:ˆQ

iuiji. PROPOSITION4.4. For k2Nr,

@hki:uj ˆqk! j k uj: …4†

PROOF. See Lemme 4.2.3 of [9]. p

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4.1.2 ± TheIgpX-indexed algebraD~(0)X(m)=S

We start with a general theory of logD-modules of higher level. For details in more general settings, see Chapitre 3 of [9]. LetX!Sbe a log smooth morphism of fine log schemes defined overZ=pZ. We consider the following commutative diagram:

Here the vertical two arrows are them-th relative Frobenius ofX!Sdefined in Subsection 3.2 and q0 andq1 (resp. p0 and p1) are the first and second pro- jections. We denote by F the m-th relative Frobenius of X!S by abuse of notation. Then, by the universal property of log 0-PD envelopes, there exists a unique morphism of 0-PD fine log schemes F4:PX=S;(0)!PX(m)=S;(0) which fits into the above diagram.

PROPOSITION4.5. Let X!S be a log smooth morphism of fine log schemes.

(1) There exists F:PX=S;(m) !PX(m)=S;(0) such that F4 uniquely factors as PX=S;(0)!PX=S;(m)!F PX(m)=S, where the first map is the natural homo- morphism.

(2) Assume that we are given a logarithmic system of coordinates fmig of X!S. Let

hfkg(m) (resp.

h0fkg(0) ) denote a basis of PX=S;(m) (resp.

PX(m)=S;(0)) associated to the basis fdlogmig (resp.fdlogpmig) (see Pro- position3.11), wherepdenotes the natural projection X(m)!X explained in the beginning of Subsection 3.2. Then F:PX(m)=S;(0)! PX=S;(m) sends h0fkg(0) tohfpmkg(m).

PROOF. (1) see Proposition 3.3.1 of [9]. (2) See (i) of Proposition 3.4.1 of [9]. p Let E be a left D(0)X(m)=S-module and feng the log 0-stratification on E via the equivalence in Remark 3.5. By endowingFEwith a leftD(m)X=S-module structure by pulling backfengviaF, we have a functor

F:

left D(0)X(m)=S-modules onX(m)

!

left D(m)X=S-modules on X : …5†

REMARK4.6. Let Ebe a leftD(0)X(m)=S-module. Let

hfkg(m) and

h0fkg(0) be as in Proposition 4.5 (2). Let

@hki (resp.

@0hki ) denote the dual of

hfkg(m) (resp.

h0fkg(0) ). Then the D(m)X=S-action on FE is characterized by the following for-

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