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Quantum D-modules for toric nef complete intersections
Etienne Mann, Thierry Mignon
To cite this version:
Etienne Mann, Thierry Mignon. Quantum D-modules for toric nef complete intersections. 2011.
�hal-00649232�
QUANTUM
D
-MODULES FOR TORIC NEF COMPLETE INTERSECTIONSby
Etienne Mann & Thierry Mignon
Abstra t. Onasmoothproje tivevarietywith
k
ampleline bundles,wedenotebyZ
the omplete interse tionsubvarietydened bygeneri se tions.Wedenethetwistedquantum
D
-modulewhi hisave torbundlewithaat onne tion,a atpairing andanaturalintegrablestru ture. An appropriatequotientof itisisomorphi to theambientpartofthequantumD
-moduleofZ
.When the variety is tori , these quantum
D
-modules are y li . The twisted quantumD
-module anbepresentedviamirrorsymmetrybytheGKZsystemasso iatedtothetotalspa e of thedualof thedire t sumofthese linebundles.A questionis to know whatis thesystemof equations that denethe ambiantpart ofthe quantum
D
-moduleofZ
. We onstru tthissystemasaquotientidealoftheGKZsystem.Wealsostateandprovethenon-equivarianttwistedGromov-Wittenaxiomsintheappendix.
Contents
1. Introdu tion... 1
2. Twisted and redu ed quantum
D
-moduleswith geometri interpretation. 4 3. Batyrev rings fortori varieties with a splittedve tor bundle... 174. GKZ systems, quotient ideals and residual
D
-modules... 295. Isomorphisms between quantum
D
-modules and GKZ systems via mirror symmetry... 39A. Twisted Axioms forGromov-Witten invariants... 48
B. Proof of Proposition 2.17... 54
Referen es... 58
1. Introdu tion
Mirrorsymmetryleadstomanydierentformulationsinmathemati s: equivalen eof
de-rived ategories(known asHomologi alMirror Symmetryby Kontsevi h [Kon95℄),
isomor-phism of Frobenius manifolds (see [Bar00℄), omparison of Hodge numbers for Calabi-Yau
varieties (see for example[Bat94℄), isomorphism of Givental's ones (see [Giv98℄),
isomor-phism of pure polarized TERP stru tures (see [Her06℄) or variation of non- ommutative
Hodge stru tures (see [KKP08℄), ...
2010 Mathemati s Subje t Classi ation. 14N35,53D45,14F10.
Key words and phrases. Quantum dierential modules, Gromov-Witten invariants, Batyrev rings, GKZsystems,mirrorsymmetry,
D
-modules,tori geometry.E.MissupportedbythegrantoftheAgen eNationaledelaRe her heNewsymmetriesonGromov-Witten theories ANR-09-JCJC-0104-01.
look at quantum ohomology with a dierential module approa h : see Kim [Kim99℄ for
homogeneous spa es, see Coates-Corti-Lee-Tseng [CCLT06℄ and Guest-Sakai [GS08℄ for
weighted proje tive spa es,see alsothe worksof Iritani[Iri06℄,[Iri07℄,[Iri08℄ and[Iri09℄,
the book of Cox-Katz [CK99℄ and the one of Guest [Gue10℄.
From the small quantum produ t on a smooth proje tive variety, we an dene a trivial
ve torbundleover
H
0
(X, C)
× V × C
whereV
⊂ (C
∗
)
r
andr := dim
C
H
2
(X, C)
whose ber isH
∗
(X, C)
. This bundle isendowed with aat onne tion and anon-degenerated pairing.
This onne tion is sometimes alled the Dubrovin-Givental onne tion. When
X
is a tori smooth Fano variety, Givental (see also Iritani [Iri09℄ for tori weak Fano orbifolds) givesan expli it presentation of this
D
-module using GKZ systems. To prove this isomorphism, he uses the equality, up to amirror map, between the so alledI
andJ
fun tions.Intheveryni earti le[Iri09℄,Iritanienri hesthisquantum
D
-modulebyaddinganatural integral stru ture i.e., he denes aZ
-lo alsystem whi h is ompatible with the onne tion. We all quantumD
-module, denoted byQDM(X)
, the trivial bundle endowed with a at onne tion, a at non-degenerated pairing and a natural integral stru ture. ThisZ
-lo al system is natural in the following sense. Assume thatX
has a mirror (for instan eX
is a weakFanotori orbifolds)thatisaLaurentpolynomialsu hthatitsBrieskornlatti e(whi hisave tor bundlewithaat onne tion)isisomorphi tothe quantum
D
-moduleofX
. On this Brieskorn latti e, we have a natural integral stru ture that omes fromthe Lefs hetz'sthimbles. The integral stru ture dened by Iritani is natural be ause it orresponds to
the naturalone on the mirror. Noti e that the bundle, the onne tion, the pairing and the
integralstru tureispartofthedenitionofaTERPstru turedenedbyHertlingin[Her06℄
or a variation of non- ommutative Hodge stru ture dened by Kontsevi h, Katzarkov and
Pantev in [KKP08℄.
In this paper, we investigate the same kind of obje ts asso iated to a smooth proje tive
variety
X
together with a splittedve tor bundleE
whi h isglobally generated.WeusethetwistedGromov-Witteninvariantsandthetwistedquantumprodu tstodene
a trivial ve tor bundle, denoted by
F
, onH
0
(X, C)
× V × C
where
V
is an open in(C
∗
)
r
where the twisted quantum produ t is onvergent. Inspired by the lassi al ase, we dene
a at onne tion
∇
, a at pairingS
and an integral stru tureF
Z
on it. We all twisted quantumD
-module,thequadrupleQDM(X,
E) := (F, ∇, S, F
Z
)
. Itsatisesalltheproperties of the lassi alQDM(X)
ex ept that the pairingS
is degenerated. We quotient by the kernel ofS
and we get a better obje t, alled redu ed quantumD
-module and denoted byQDM(X,
E) := (F , ∇, S, F
Z
)
. More pre isely, we onsider the trivial ve tor bundleF
with thebersH
2∗
(X, C)/ ker m
c
top
wherem
c
top
: α
→ c
top
(
E)∪α
forany ohomology lassα
. The data(F,
∇, S, F
Z
)
pass tothisquotientand wegetQDM(X,
E)
that satisesallthe lassi al properties and nowS
is non-degenerated. So it really looks like a quantumD
-module of a variety. Indeed, we have ageometri interpretation ofQDM(X,
E)
:Theorem 1.1 (See Theorem 2.42). Let
L
1
, . . . ,
L
k
be ample line bundles onX
, and assume thatdim
C
X
≥ k + 3
. LetZ
be the zero of a generi se tion ofE := ⊕
k
i=1
L
i
. Denote byι : Z ֒
→ X
the losedembedding. Thenthe redu edquantumD
-moduleQDM(X,
E)
is iso-morphi to the sub-quantumD
-moduleQDM
amb
(Z)
ofQDM(Z)
whose ber isι
∗
H
2∗
(X, C)
.
Noti e thatour integral stru ture
F
Z
dened onQDM(X,
E)
is naturalbe ause itindu es the natural one onQDM
amb
(Z)
.Then the next natural question is : an we nd a presentation of
QDM(X,
E)
andQDM(X,
E)
whenX
is a tori smooth variety interms of GKZ systems ?Denote by
D
the sheaf of dierential operators on the basis spa e of theF
(this is not reallytrue, the operatorsthat we onsider arezq
a
∂
q
a
whereq
a
are variable inH
2
(X, C)
z
isthe oordinateonC
). Denote byY
the totalspa eofthe dualve tor bundleE
∨
. Denote
by
G
the ideal sheaf asso iated to the GKZ system of the tori varietyY
. We have the followingresult.Theorem 1.2 (see Theorem 5.10). Let
X
beasmoothtori varietywithk
linebundlesL
1
, . . . ,
L
k
su h that(ω
X
⊗ L
1
⊗ . . . ⊗ L
k
)
∨
is nef. We put
E := ⊕
k
i=1
L
i
.1. If the line bundles
L
1
, . . . ,
L
k
are globally generatedthen we have the following isomor-phism :D/G
−→ Mir
∼
∗
(
F, ∇)
where
Mir
isthe mirror map of Givental andF
is the sheaf of se tions ofF
.2. If the line bundles
L
1
, . . . ,
L
k
are ample, we have the following ommutative diagramD/G
∼
Mir
∗
(
F, ∇)
D/ Quot(bc
top
,
G)
∼
Mir
∗
(
F, ∇)
where
bc
top
is an operator atta h to the ohomology lassc
top
(
E)
( f.Notation 4.1) andQuot(bc
top
,
G)
is the left quotient idealhP ∈ D, bc
top
P
∈ Gi
.Noti e that, unlike the ommutative ase, the set
{P ∈ D, bc
top
P
∈ G}
is not an ideal. The ideal sheafQuot(bc
top
,
G)
answer to the following question whi h is addressed in the [CK99, p.94-95and p.101℄: What dierentialequationsshall we addtoG
toget an isomor-phism withQDM
amb
(Z)
?The isomorphisms above are based on the equality (up to the mirror map) between the
twisted
J
-fun tion and the twistedI
-fun tionof Givental(see [Giv96℄and [Giv98℄)and a areful analysis of the lo alfreeness and rankof GKZ modules. Freeness and rankrequiresthe study of Batyrev rings of the tori variety
Y
the total spa e ofE
∨
whi h willappear
as the restri tion of the
D
-modules atz = 0
, and an be thought asa twisted Batyrev ring of the pair(X,
E)
.Proving this theorem leads to develop quite a lot of materialsand results whi h deserve
some pre isions. Letus sket h our strategy of proof.
Forthe rst pointof the theorem above,we show that
D/G
is alo allyfreesheaf of rankdim
C
H
2∗
(X, C) = rk F
(see Theorem 4.10). This is done in2
steps.Werst prove the oheren e of
D/G
(see Theorem 4.5). This impliesthe lo alfreeness overz
6= 0
and we use Adolphson's result in[Ado94℄ to ompute the rank.On
z = 0
,we have atautologi al isomorphismbetweenD/G |
z=0
and the Batyrev ring ofY
. We prove that this ring is lo ally free of rankrk F
over a suitable algebrai neighborhoodU
(see below).Forse ond point of the theorem above, we showin Theorem 4.14 :
On
z = 0
, we prove that the natural morphism betweenD/ Quot(bc
top
,
G) |
z=0
and the residualBatyrev ring (see Denition 3.39) ofY
is anisomorphism. We prove that this residual ring islo allyfree ofrankrk F = dim H
2∗
(X)
− dim ker m
c
top
overU
.on
z
6= 0
the oheren e ofD/G
implies thatD/ Quot(bc
top
,
G)
islo allyfreeof rank less thanrk F
.Letus olle tthe pre iseresultsthatwe proveonthe Batyrevrings,whi hare interesting
ontheir own :
Theorem 1.3. Let
X
be a smooth tori variety withk
globally generated line bundlesL
1
, . . . ,
L
k
su hthatthe total spa e of the ve tor bundleE := ⊕
k
divisor. Denote by
U
the good neighborhood in the spe trum of the Novikov ring dened in Notation 3.34.1. (See Theorem 3.26) Denote by
B
the Batyrev ring (see Denition 3.12) of the total spa e ofE
∨
.The morphism :
Spec(B)
|
U
−→ U
is nite, at, of degreedim H
2∗
(X, C)
.
2. (See Proposition 3.40) Moreover, if the line bundles
L
1
, . . . ,
L
k
are ample then the morphism :Spec(B
res
)
|
U
−→ U
is nite, at, of degreedim H
2∗
(X, C)
whereB
res
is
the residualBatyrev ring (see Denition 3.39).
The plan of this arti le is the following.
In Se tion 2,we dene rst (Subse tion 2.1) the twisted quantum
D
-moduleQDM(X,
E)
withallitspropertiesanditsnaturalintegralstru ture. Thenwedenetheredu edquantumD
-moduleQDM(X,
E)
in Subse tion 2.2. Finally, we give the geometri interpretation in Subse tion 2.3where we prove the rst Theorem 1.1.In Se tion 3, we fo us on Batyrev rings for tori varieties. Noti e that this se tion an
be read independently of the rest of the paper. The rst Subse tion 3.1is devoted tosome
re alls on tori geometry. In Subse tion 3.1 we onstru t the fan of the total spa e of the
ve tor bundle
E
. In Subse tion 3.2, we dene the Batyrev rings. Subse tion 3.3 is devoted to some re alls on the primitive olle tions. In Subse tion 3.4, we prove that the quantumStanley-Reisner ideal has a Groebner basis indexed by primitive olle tions (See Theorem
3.22). In Subse tions 3.5and 3.6, we prove the Theorem 3.26 and Proposition 3.40 quoted
above inTheorem 1.3.
In Se tion 4, we fo us on GKZ modules. We prove rst that the GKZ module
D/G
is oherentinTheorem 4.5. Thenweprovethatitislo allyfreeof rankrk F
inTheorem4.10. We nish by a result on the residual GKZ moduleD/ Quot(bc
top
,
G)
(see Theorem 4.14). These results use Theorem 3.26 and Proposition 3.40 of the previous se tion.InSe tion5,westartbysomere allonGivental'smirrorsymmetryinSubse tion5.1then
we state and prove Theorem 1.2 inSubse tion 5.2.
We nish this paper by two appendi es. Appendix A ontains the proof of the twisted
Gromov-Witten invariants in genus
0
that are known from the experts. We add it by la k of referen es.Appendix B is a omplete proof of the atness of the onne tion
∇
using the twisted axioms.A knowledgment: WethankThomasRei helt,ClaudeSabbahandChristianSevenhe k
for useful dis ussions. The seminar in Paris organized by Serguei Barannikov and Claude
Sabbahon the non- ommutativeHodge stru tures wasthe starting point of this paper. We
also thank Antoine Douai for helping in the organization of the workshop in Luminy on
the work of Iritani. We are also grateful to Hiroshi Iritani that pointed out the referen e
[Mav00 ℄ (see Remark 2.40) The rst author is supported by the ANR New symetries in
Gromov-Witten theories number ANR- 09-JCJC-0104-01.
Notation 1.4. We use alligraphi letters for the sheaves like
M, M
res
,
G, B, L, E
. We
use boldlettersfor modules or ideals onnon ommutativerings
M, M
res
, G, A, . . .
.
2. Twisted and redu ed quantum
D
-modules with geometri interpretationLet
X
be a smooth proje tive omplex variety of dimensionn
andk
globally generated linebundlesL
1
, . . . ,
L
k
. Denote byE
the sumE := L
1
⊕ · · · ⊕ L
k
.Werstdenethetwistedquantum
D
-module,denotedbyQDM(X,
E)
,asso iatedtothese data (Denition 2.24). This is a trivial bundle of rankdim
C
H
2∗
(X, C)
with an integrable
It turns out that the pairing of the twisted quantum
D
-module is degenerated, whi h makesQDM(X,
E)
a not so natural obje t, without lear geometri meaning. In a se ond paragraph we introdu e the redu ed quantumD
-moduleQDM(X,
E)
(Denition2.34) ; itis onstru ted as the quotient ofQDM(X,
E)
by the kernel of the endomorphismm
c
top
, whi h is the up multipli ation by the Euler lassc
top
(
E)
ofE
:m
c
top
: H
2∗
(X, C)
−→ H
2∗
(X, C)
α
7−→ α ∪ c
top
(
E).
The redu ed quantum
D
-module is a trivial bundle of rankdim H
2∗
(X, C)
− dim ker m
c
top
with anintegrable onne tion,a at nondegenerated pairingand an integral stru ture.
If
dim X
≥ k + 3
, we also onsider a generi se tion ofE
and denote byZ
the omplete interse tion subvariety dened as the zero lo us of this se tion. By Bertini's theorem overC
, the subvarietyZ
is smooth and onne ted. Assuming moreover that theL
i
are ample linebundles, the Lefs hetz theorem givesan isomorphismbetweenH
2
(X, C)
and
H
2
(Z, C)
.
We an ompare
QDM(X,
E)
,QDM(X,
E)
and the lassi al, untwisted, quantumD
-module ofZ
,QDM(Z)
. This willbe made inthe last subse tion.Notation 2.1. For
0
≤ i ≤ 2n
, denote byH
i
(X) := H
i
(X, C)
the omplex
ohomol-ogy group of lasses of degree
i
. Also denote byH
∗
(X)
the omplex ohomology ring
⊕
2n
i=0
H
i
(X)
; the even part of this ring will be writtenH
2∗
(X)
. Put
s = dim
C
H
2∗
(X)
and
r = dim
C
H
2
(X)
.Wex,on e andforall,ahomogeneousbasis
(T
0
, . . . , T
s−1
)
ofH
2∗
(X)
su hthat
T
0
= 1
is the unitforthe up produ t andthatthe lassesT
1
, . . . , T
r
formabasis ofH
2
(X, Z)
modulo
torsion. Denoteby
(t
0
, . . . , t
s−1
)
theasso iated oordinatesandputτ :=
P
s−1
a=0
t
a
T
a
andτ
2
:=
P
r
a=1
t
a
T
a
. Also denoteby(T
0
, . . . , T
s−1
)
the Poin aré dual in
H
2∗
(X)
of
(T
0
, . . . , T
s−1
)
. Asa onvention, WewillwriteH
2
(X, Z)
forthedegree2
integerhomologymodulotorsion. Denoteby(B
1
, . . . , B
r
)
thedualbasisof(T
1
, . . . , T
r
)
inH
2
(X, Z)
. Theasso iated oordinates willbe denoted by(d
1
, . . . , d
r
)
.We denote by
T
X
the tangent bundle ofX
,ω
X
the anoni al sheaf, and x a anoni al divisorK
X
.Asa onvention,wewillmakenonotationaldistin tionbetweenve torbundlesandlo ally
free sheaves, writingfor example
E
andL
i
forboth.2.1. Twistedquantum
D
-module. Inthissubse tion,wedenethetwistedquantumD
-moduleQDM(X,
E) = (F, ∇, S, F
Z
)
.2.1.a. Twistedquantumprodu t. Firstre allthedenitionofthetwistedGromov-Witten
invariant ( f.[Giv96℄and [CG07℄ or[CK99, Se tion 11.2.1℄and [Pan98℄).
Let
ℓ
be inN
andd
be inH
2
(X, Z)
. Denote byX
0,ℓ,d
the modulispa e of stable maps of degreed
fromrational urveswithℓ
marked points toX
. The universal urve overX
0,ℓ,d
isX
0,ℓ+1,d
:X
0,ℓ+1,d
π
e
ℓ+1
X
X
0,ℓ,d
where
π
isthemap thatforgets the(ℓ + 1)
-thpointandstabilizes,ande
ℓ+1
isthe evaluation atthe(ℓ + 1)
-thmarked point.Re all that a onvex bundle
N
onX
is a ve tor bundle su h that, for any stable mapf : C
→ X
whereC
is a rationalnodal urve,H
1
(C, f
∗
N ) = 0
Proposition 2.2. Let
N
beagloballygeneratedve torbundle(notne essarilysplitted)of rankb
thenN
is onvexandthesheafN
0,ℓ,d
:= R
0
π
∗
e
∗
ℓ+1
N
islo allyfreeofrankR
d
c
1
(
N )+b
. Proof. Let usprove the onvexity ofN
. Wefollow[FP97 ,Lemma 10℄.Let
f : C
−→ X
be a stable map andp
be a non singular pointonC
. We willprove by indu tion onthe number of irredu ible omponents ofC
thatH
1
(C, f
∗
N ⊗ O
C
(
−p)) = 0.
(2.3)
First,assumethat
C
≃ P
1
. We anwrite
f
∗
(
N ) ≃ ⊕
b
i=1
O
P
1
(a
i
)
witha
1
, . . . , a
b
inZ
. Sin eN
isgloballygenerated,f
∗
(
N )
alsois,whi himplies
a
i
≥ 0
foranyi
in{1, . . . , b}
. Itfollows thatH
1
(P
1
, f
∗
N ⊗ O
C
(
−p)) = ⊕
b
i=1
H
1
(P
1
,
O
P
1
(a
i
− 1)) = 0
. AssumenowthatC = C
′
∪ C
0
whereC
0
≃ P
1
and
p
inC
0
. Denote byp
1
, . . . , p
q
thepoints ofC
0
∩ C
′
. Noti e that
C
′
has exa tly
q
onne ted omponents interse tingC
0
on exa tly one point. Ea hp
i
is a smooth point of one of these omponents. We have the following exa t sequen e0
f
∗
N ⊗ O
C
′
(
−
P
q
i=1
p
i
)
f
∗
N ⊗ O
C
(
−p)
f
∗
N ⊗ O
C
0
(
−p)
0
From the asso iatedlong exa t sequen e and by the indu tive assumptiononthe onne ted
omponents of
C
′
,we dedu e the equality (2.3). The exa t sequen e :
0
f
∗
N ⊗ O
C
(
−p)
f
∗
N
f
∗
N ⊗ O
p
0
gives
H
1
(C, f
∗
N ) = 0
.
Now, the stalk at a point
(C, x
1
, . . . , x
ℓ
, f : C
→ X)
inX
0,ℓ,d
of the K-theoreti push-forwardN
0,ℓ,d
isH
0
(C, f
∗
N ) − H
1
(C, f
∗
N )
. Sin eN
is onvexH
1
(C, f
∗
N ) = 0
andH
0
(C, f
∗
N )
has dimensionR
d
c
1
(
N ) + b
by Riemann-Ro h. Thus,N
0,ℓ,d
is lo ally free of dimensionR
d
c
1
(
N ) + b
onX
0,ℓ,d
. LetE
0,ℓ,d
bethe sheafR
0
π
∗
e
∗
ℓ+1
E
asin Proposition 2.2. Forj
in{1, . . . , ℓ}
,we dene the surje tive morphismE
0,ℓ,d
→ e
∗
j
E
by evaluating the se tion to thej
-th marked point. We deneE
0,ℓ,d
(j)
tobethe kernel of this map that is we have the following exa t sequen e0
E
0,ℓ,d
(j)
E
0,ℓ,d
e
∗
j
E
0
(2.4)
By Proposition 2.2, for any
j
∈ {1, . . . , ℓ}
the bundleE
0,ℓ,d
(j)
has rankR
d
c
1
(
E)
.For
i
∈ {1, . . . , ℓ}
, letN
i
bethe linebundleonX
0,ℓ,d
whoseber atapoint(C, x
1
, . . . , x
ℓ
,
f : C
→ X)
isthe otangent spa eT
∗
C
x
i
. Putψ
i
:= c
1
(N
i
)
inH
2
(X
0,ℓ,d
)
. Denition 2.5. Letℓ
be inN
,γ
1
, . . . , γ
ℓ
be lasses inH
2∗
(X)
,
d
be inH
2
(X, Z)
and(m
1
, . . . , m
ℓ
)
be inN
ℓ
. For
j
in{1, . . . , ℓ}
, the (j
-th) twisted Gromov-Witten invariant with des endants of these data is dened and denoted byD
τ
m
1
(γ
1
), . . . , ^
τ
m
j
(γ
j
), . . . , τ
m
ℓ
(γ
ℓ
)
E
0,ℓ,d
:=
Z
[X
0,ℓ,d
]
vir
c
top
(
E
0,ℓ,d
(j))
ℓ
Y
i=1
ψ
m
i
i
e
∗
i
γ
i
where
e
i
: X
0,ℓ,d
→ X (1 ≤ i ≤ ℓ)
is the evaluationmorphism to thei
th marked point and[X
0,ℓ,d
]
vir
is the virtual lass onX
0,ℓ,d
. Denition 2.6. Letτ
2
bea lass ofH
2
(X)
and
γ
1
, γ
2
beinH
2∗
(X)
. The twisted small
quantum produ t (withrespe t to
E
) ofγ
1
andγ
2
is dened byγ
1
•
tw
τ
2
γ
2
:=
s−1
X
a=0
X
d∈H
2
(X,Z)
e
R
d
τ
2
D
γ
1
, γ
2
, e
T
a
E
0,3,d
T
a
τ
inH
2∗
(X)
, abig twisted quantum produ t :
γ
1
•
tw
τ
γ
2
:=
s−1
X
a=0
DD
γ
1
, γ
2
, e
T
a
EE
0
T
a
.
As usual, wehave :•
tw
τ
2
:=
•
tw
τ
|
τ =τ
2
. Wewillnot use of bigtwisted quantum produ ts. 2. One an alsodene the smalltwistedquantum produ t without hoosing a basis by :γ
1
•
tw
τ
2
γ
2
:=
X
d∈H
2
(X,Z)
e
R
d
τ
2
e
3∗
e
∗
1
γ
1
∪ e
∗
2
γ
2
∪ c
top
(
E
0,3,d
(3))
∩ [X
0,3,d
]
vir
(2.8)2.1.b. Parameters. The quantum produ t written in Denition 2.6 depends on the
pa-rameter
τ
2
inH
2
(X)
. The Pi ard group
Pic(X)
a ts onH
2
(X)
inthe followingway : for
L
inPic(X)
,L.τ
2
= τ
2
+ 2
√
−1πc
1
(
L)
. The numbere
R
d
τ
2
being invariant by this a tion, the quantum produ t is naturallydened overH
2
(X)/ Pic(X) = H
2
(X)/2
√
−1πH
2
(X, Z)
.
Letus extend the lo us of the parameter. Denote by NE
(X)
Z
⊂ H
2
(X, Z)
the Mori one ofX
, generated asa semi-group by numeri al lasses of irredu ible urves inX
.Notation 2.9. The semigroup algebras of NE
(X)
Z
andH
2
(X, Z)
will be respe tively denoted byΛ
andΠ
:Λ = C[
NE(X)
Z
] = C[Q
d
, d
∈
NE(X)
Z
],
Π = C[H
2
(X, Z)] = C[Q
d
, d
∈ H
2
(X, Z)]
whereQ
d
are indeterminates satisfyingrelations :
Q
d
.Q
d
′
= Q
d+d
′
.
The s heme
Spec Λ
is an irredu ible, possibly singular, ane variety of dimensionr
. De-note byV
the set of omplex points ofSpec Λ
. Points ofV
are hara ters(1)
of NE
(X)
Z
. Ifq
is su h a hara ter, denote byq
d
its evaluation on
d
in NE(X)
Z
. Sin eX
is pro je -tive, the Mori one is stri tly onvex and there exists a unique hara ter sending anyd
inH
2
(X, Z)
\ {0}
to0
. Wewilldenotethis hara ter by0
and allit,asusual,the large radius limit ofX
.The s heme
Spec Π
is atorus ofdimensionr = rk H
2
(X, Z)
. The set of omplex pointsofSpec Π
will be denoted byT
; a point ofT
is a hara ter ofH
2
(X, Z)
andT
is a smooth subset ofV
. We will identifyT
andH
2
(X)/2
√
−1πH
2
(X, Z)
via the natural surje tive
morphismof omplex variety :
Ψ : H
2
(X, C)
−→ T
(2.10)τ
7−→ q
τ
:=
h
d
∈ H
2
(X, Z)
7→ q
τ
d
= e
R
d
τ
i
The kernel ofΨ
is2
√
−1πH
2
(X, Z)
. Thus, the large radius limit
0
inV
⊃ T
is a limit inH
2
(X)/2
√
−1πH
2
(X, Z)
.
The smallquantum produ t an now be dened with parameter
q
inV
:Denition 2.11. Let
q
be inV
andγ
1
, γ
2
be inH
2∗
(X)
. The twisted small quantum
produ t is dened by
γ
1
•
tw
q
γ
2
:=
s−1
X
a=0
X
d∈H
2
(X,Z)
q
d
D
γ
1
, γ
2
, e
T
a
E
0,3,d
T
a
(1)
Bya hara ter ofasemi-group
R
ofH
2
(X, Z)
wemean anappli ationq
: R
−→ C
su h thatq(0) = 1
andq(d + d
′
) = q(d).q(d
′
)
forany
d, d
′
in
R
. IfR
isagrouptheimageofq
isinC
∗
. If
q
issu ha hara ter, wewillwriteq
d
:= q(d)
. A hara ter
q
ofasemi-groupR
givesa omplexpointSpec C
−→ Spec C[R]
whi h will alsobedenotedbyq
; this orresponden eisabije tion. Noti ethat,ifd
is inR
,Q
d
isafun tion on
Spec
C
C[R]
andwehave:Q
d
(q) = q
d
.Denition2.11andDenition2.6are ompatible: Forany
τ
2
inH
2
(X)
,Ψ(τ
2
)
isinT
andγ
1
•
tw
τ
2
γ
2
= γ
1
•
tw
Ψ(τ
2
)
γ
2
.Assumption 2.12. We willassumethat there exists an open subset
V
ofV
ontaining the large radius limit0
su h that :∀q ∈ V , ∀γ
1
, γ
2
∈ H
2∗
(X), γ
1
•
tw
q
γ
2
is onvergent.This assumptionis easilyshown tobe true whenthe linebundle
(ω
X
⊗ L
1
⊗ · · · ⊗ L
k
)
∨
is
ample,thatiswhenthe ompleteinterse tionvariety
Z
dened byE
isFano. Inother ases, su h as Calabi-Yausubvarieties of tori varieties onsidered below, one may use [Iri07℄ tohe k this assumption.
Notation 2.13. We denote by
V
the omplex nonsingular varietyV := V
∩ T
.Thus,
V
is a smooth lo us inV
where the quantum produ t is onvergent. Wehave : large radius limit= 0
∈ V
( onvergent produ t)⊂
V
= Spec
C
Λ
∪
∪
0 /
∈ V
( onvergent produ t)⊂ T = Spec
C
Π
∼
−→ (C
∗
)
r
As a onvention, we willdenote neighborhood of
0
inV
by an overlined apital letter, and itsinterse tionwithT
by thesame apitalletterwithoutoverlining(V
isa ompa ti ation ofT
inthe neighbourhood of the large radiuslimit).Letus re all some properties of the twisted quantum produ t :
Proposition 2.14. For any
q
inV
the twisted quantum produ t•
tw
q
isasso iative, om-mutative, with unityT
0
:= 1
.Proof. This isa lassi alproof, assoonasthe twistedGromov-Wittenaxiomsare known.
The twisted axioms are shown in Appendix A. Su h proves are given by Pandharipande in
[Pan98℄, Proposition 3, for a smooth hypersurfa e of
P
n
and by Iritani in Remark 2.2. of
[Iri11℄, inthe general ase.
2.1. . Thetrivialbundlewithanintegrable onnexion. Usingbasis
T
1
, . . . , T
r
andB
1
, . . . ,
B
r
denedin2.1,wehave:Π = C[H
2
(X, Z)]
∼
−→ C[q
±
1
, . . . , q
r
±
]
whereq
a
:= Q
B
a
( f.footnote 1). Thus ifd =
P
r
a=1
d
a
B
a
we getQ
d
=
Q
r
a=1
q
a
d
a
inΠ
. Viewing theq
a
's as oordinates ofT
, we get :q
d
=
Q
r
a=1
q
a
d
a
for anyq
∈ T
. Fora
in{1, . . . , r}
, we put :δ
a
:= q
a
∂
q
a
δ
z
:= z∂
z
.
Re all that
t
0
is the oordinateonH
0
(X)
.
Notation 2.15. We denote by
F
the trivialholomorphi ve tor bundleof berH
2∗
(X)
over
H
0
(X)
× V × C
:
F :=
H
2∗
(X)
× H
0
(X)
× V × C
→ H
0
(X)
× V × C
together with the following meromorphi onne tion :
∇
∂
t0
:= ∂
t
0
+
1
z
1
•
tw
q
,
∇
δa
:= δ
a
+
1
z
T
a
•
tw
q
,
∇
δ
z
:= δ
z
−
1
z
E
•
tw
q
+µ
where
µ
isthe diagonalmorphismdened byµ(T
a
) :=
1
2
(deg(T
a
)
− (dim
C
X
− rk E)) T
a
andE
(t
0
, q, z) := t
0
1
+ c
1
(
T
X
⊗ E
∨
)
. This global se tion
E
ofF
orresponds to the Euler eld. Noti ethatthetwistedprodu t•
tw
q
doesnotdependont
0
be auseofthetwistedfundamental lass Axiom ( f.PropositionA.4).In the untwisted ase, it is known that
∇
is aat onne tion and its at se tions an be des ribed expli itly. Letus give the equivalent property in the twisted ase. We dene themulti-valuated ohomologi almeromorphi fun tion
L
tw
(t
0
, q, z) :
H
2∗
(X)
−→ H
2∗
(X)
γ
7−→ L
tw
(t
0
, q, z)γ = e
−t
0
/z
q
−T /z
γ
−
s−1
X
a=0
X
H2(X,Z)
d6=0
q
d
q
−T /z
γ
z + ψ
, e
T
a
0,2,d
T
a
(2.16) whereψ := ψ
1
= c
1
(N
1
)
isthe lass ofH
2
(X
0,3,d
)
given beforeDenition 2.5,1
z + ψ
:=
X
k∈N
(
−1)
k
ψ
k
z
−k−1
,
q
−T /z
= q
−T
1
/z
.
· · · .q
−T
r
/z
:= e
−z
−1
P
r
a=1
T
a
log(q
a
)
andlog(q
a
)
isthe multi-valuatedfun tion,or any determinationof the logarithm ona simply onne ted open subset ofV .
For an endomorphism
u
, we denotez
u
:= exp(u log z)
. The following Proposition is the
twisted version of Proposition2.4in [Iri09℄.
Proposition 2.17. 1. The onne tion
∇
is at. 2. Fora
in{1, . . . , r}
andγ
∈ H
2∗
(X)
we have∇
∂
t0
L
tw
(t
0
, q, z)γ = 0,
∇
δ
a
L
tw
(t
0
, q, z)γ = 0
∇
δ
z
L
tw
(t
0
, q, z)γ = L
tw
(t
0
, q, z)
µ
−
c
1
(
T
X
⊗ E
∨
)
z
γ
3. The multi-valued ohomologi alfun tion
L
tw
(t
0
, q, z)z
−µ
z
c
1
(T
X
⊗E
∨
)
is a fundamental so-lution of∇
aboveH
0
(X)
× V × C
.Noti e that, as afundamental solution,
L
tw
is onvergent above
H
0
(X)
× V × C
.
This kindof resultis lassi alinthe untwisted ase ([CK99℄, [Iri09℄). Byla k referen es
ontwistedGromov-Witten invariants,we write down a proof infull details inAppendix B.
2.1.d. The degenerated pairing. Denote by
(
·, ·)
the Poin aré duality onH
2∗
(X)
. AsD
γ
1
, γ
2
, e
T
a
E
0,3,d
isnot symmetri inthe three arguments wedo not havethe Frobenius
rela-tion, that is :
(γ
1
•
tw
q
γ
2
, γ
3
)
6= (γ
1
, γ
2
•
tw
q
γ
3
).
Nevertheless we an dene asymmetri bilinearform :
Denition 2.18. The twisted pairingon
H
2∗
(X)
isdened by :∀γ
1
, γ
2
∈ H
2∗
(X), (γ
1
, γ
2
)
tw
:=
Z
X
γ
1
∪ γ
2
∪ c
top
(
E).
Proposition 2.19. 1. The bilinear form
(
·, ·)
tw
is degenerated with kernel
ker m
c
top
where
m
c
top
is dene as :m
c
top
: H
2∗
(X)
−→ H
2∗
(X)
2. For
γ
1
, γ
2
, γ
3
inH
∗
(X)
, we have the Frobenius relation :
(γ
1
•
tw
q
γ
2
, γ
3
)
tw
= (γ
1
, γ
2
•
tw
q
γ
3
)
tw
.
Proof. The rst laimis obvious.
By Denition 2.18 and Remark 2.8, it is enough to prove the following equality for any
d
∈ H
2
(X, Z)
:Z
X
e
3∗
e
∗
1
γ
1
∪ e
∗
2
γ
2
∪ c
top
(
E
0,3,d
(3))
∩ [X
0,3,d
]
vir
∪ γ
3
∪ c
top
(
E)
=
Z
X
e
3∗
e
∗
1
γ
2
∪ e
∗
2
γ
3
∪ c
top
(
E
0,3,d
(3))
∩ [X
0,3,d
]
vir
∪ γ
1
∪ c
top
(
E).
The exa t sequen e :
0
E
0,3,d
(3)
E
0,3,d
e
∗
3
E
0
gives
c
top
(
E
0,3,d
(3)).c
top
(e
∗
3
E) = c
top
(
E
0,3,d
)
. By proje tion formulawe get :Z
X
e
3∗
e
∗
1
γ
1
∪ e
∗
2
γ
2
∪ c
top
(
E
0,3,d
(3))
∩ [X
0,3,d
]
vir
∪ γ
3
∪ c
top
(
E)
=
Z
[X
0,3,d
]
vir
e
∗
1
γ
1
∪ e
∗
2
γ
2
∪ e
∗
3
γ
3
∪ c
top
(
E
0,3,d
)
As the lastnumberis invariant by permuting the lass
γ
i
, we dedu e the proposition. LetO := O
H
0
(X)×V ×C
be the sheaf of holomorphi fun tions onH
0
(X)
× V × C
, and
F
be thesheafof holomorphi se tionsofF
. LetΓ(
O)
be the ringof globalse tionsofO
,andΓ(
F)
be theΓ(
O)
-modulesof global se tion ofF
;Γ(
O)
is endowed with the involution :κ :
Γ(
O)
−→
Γ(
O)
f (t
0
, q, z)
7−→ f
κ
:= f (t
0
, q,
−z)
Denote by
Γ(
F)
κ
the
Γ(
O)
-moduleequals,asaset, toΓ(
F)
and endowed with thefollowing multipli ation :∀f ∈ Γ(O), s ∈ Γ(F), f.s := f
κ
.s
. Wedene a asesquilinear pairing
S : Γ(
F)
κ
⊗ Γ(F) −→ Γ(O)
by xing itsvalue on onstant se tionsof
F
:∀γ
1
, γ
2
∈ H
2∗
(X), S(γ
1
, γ
2
) = (γ
1
, γ
2
)
tw
.
As a onsequen e, weget :
∀s
1
, s
2
∈ Γ(F), ∀(t
0
, q, z)
∈ H
0
(X)
× V × C,
S(s
1
, s
2
)(t
0
, q, z) = (s
1
(t
0
, q,
−z), s
2
(t
0
, q, z))
tw
.
Proposition 2.20. 1. The pairing
S
is∇
-at. 2. For anys
1
, s
2
inΓ(
F)
,S(L
tw
.s
1
, L
tw
.s
2
) = S(s
1
, s
2
).
3. For anyγ
1
, γ
2
inH
2∗
(X)
we haveS(L
tw
(t
0
, q, z)z
−µ
z
c
1
(T
X
⊗E
∨
)
γ
1
, L
tw
(t
0
, q, z)z
−µ
z
c
1
(T
X
⊗E
∨
)
γ
2
)
=S(e
√
−1πc
1
(T
X
⊗E
∨
)
γ
1
, e
√
−1πµ
γ
2
).
Proof. 1. Bythe FrobeniuspropertyofProposition2.19.(2),forany
a
∈ {1, . . . , r}
and for anys
1
, s
2
∈ Γ(F)
, wehave :δ
a
S(s
1
, s
2
) = S(
∇
δ
a
s
1
, s
2
) + S(s
1
,
∇
δ
a
s
2
)
∂
t
0
S(s
1
, s
2
) = S(
∇
∂
t0
s
1
, s
2
) + S(s
1
,
∇
∂
t0
s
2
).
By the denition of
µ
and Proposition 2.19.(2), for anys
1
, s
2
∈ Γ(F)
we haveδ
z
S(s
1
, s
2
) = S(
∇
δ
z
s
1
, s
2
) + S(s
1
,
∇
δ
z
s
2
).
Hen e,
S
is∇
-at.2. By atnessof
S
and Proposition 2.17.(2), we dedu e that∀γ
1
, γ
2
∈ H
2∗
(X), δ
a
S(L
tw
γ
1
, L
tw
γ
2
) = 0.
So the expression
(L
tw
(t
0
, q,
−z)γ
1
, L
tw
(t
0
, q, z)γ
2
)
tw
does not depend onq
. By the asymptoti ofL
tw
atthe large radius limit,we get
(L
tw
(t
0
, q,
−z)γ
1
, L
tw
(t
0
, q, z)γ
2
)
tw
∼
q=0
(q
−T /z
γ
1
, q
T /z
γ
2
)
tw
= (γ
1
, γ
2
)
tw
.
Therelation
S(L
tw
.s
1
, L
tw
.s
2
) = S(s
1
, s
2
)
isalsotrueforanys
1
, s
2
∈ Γ(F)
by sesquilin-earity.3. By the previous formula and the atness, we dedu e that the left hand side does not
depends on
z
. Sowe an putz = 1
. We dedu e that the lefthand side is equaltoS(e
−
√
−1πµ
e
√
−1πc
1
(T
X
⊗E
∨
)
γ
1
, γ
2
).
As
S(
−µ(γ
1
), γ
2
) = S(γ
1
, µ(γ
2
))
for anyγ
1
, γ
2
inH
2∗
(X)
, we dedu e the formula.
2.1.e. Integral stru ture. In the same way than Iritani [Iri09, Denition 2.9℄ (see also
[Iri11, footnote 8 p.20℄), we dene an integral stru ture on the ve tor bundle
F
with on-ne tion∇
, ompatible tothe pairingS
.Denote by
γ
the Euler onstant. Fora ve tor bundleN
onX
of rankb
, we onsider the invertible ohomology lassb
Γ(
N ) :=
b
Y
i=1
Γ(1 + ν
i
) = exp
−γc
1
(
N ) +
X
b≥2
(
−1)
b
(b
− 1)!ζ(b) Ch
b
(
N )
!
where
ν
1
, . . . , ν
b
are the ChernrootsofN
andCh
b
(
N )
is the lassof degree2b
of the Chern hara terCh(
N )
. Denote byK(X)
the Grothendie k group of ve tor bundlesonX
. Re all that the morphismCh : K(X)
→ H
2∗
(X, Z)
be ome an isomorphism after tensored by
C
(see for instan e Theorem 3.25 p.283in [Kar78℄).Denition 2.21. Forany
v
inK(X)
,we putZ
tw
(v) := (2π)
−(n−k)/2
L
tw
(t
0
, q, z)z
−µ
z
c
1
(T
X
⊗E
∨
)
b
Γ(
T
X
)b
Γ(
E)
−1
(2
√
−1π)
deg /2
Ch(v).
We allZ
tw
(K(X))
the
b
Γ
-integral stru ture onQDM(X,
E)
and wedenote it byF
Z
. Remark 2.22. Noti ethatZ
tw
(v)
isamulti-valuedatse tionofthebundle
(F,
∇)
and thatZ
tw
(K(X))
⊗
Z
C
isthe set ofat se tionsofF
. We an understandthe formulaofZ
tw
above asthe twist by
b
Γ(
T
X
)b
Γ(
E)
−1
of the naturalintegral stru ture given by
K(X)
.K(X)
(2
√
−1π)
deg /2
Ch
(F, d)
b
Γ(T
X
)b
Γ(E)
−1
(F, d)
(2π)
−n/2
L
tw
(t
0
,q,z)z
−µ
z
c1(TX ⊗E
∨ )
(F,
∇)
Proposition 2.23. For any
v
1
, v
2
inK(X)
, we have :S(
Z
tw
(v
1
),
Z
tw
(v
2
)) =
Z
X
Proof. Using Proposition2.20.(3) and
e
√
−1πµ
= (
−1)
deg /2
(
√
−1)
k−n
, we dedu e thatS(
Z
tw
(v
1
),
Z
tw
(v
2
))
=(2
√
−1π)
k−n
Z
X
c
top
(
E)e
√
−1πc
1
(T
X
⊗E
∨
)
Γ(
b
T
X
)b
Γ(
E)
−1
(2
√
−1π)
deg /2
Ch(v
1
)
∪ (−1)
deg /2
Γ(
b
T
X
)b
Γ(
E)
−1
(2
√
−1π)
deg /2
Ch(v
2
)
We have the following fa ts : for any
α, β
inH
2∗
(X)
, for any
v
inK(X)
and for anyδ
∈ H
2
(X)
,
β
∪ (2
√
−1π)
deg /2
α = (2
√
−1π)
deg /2
(β/(2
√
−1π)
deg β/2
∪ α)
Z
X
(2
√
−1π)
deg /2
α = (2
√
−1π)
n
Z
X
α
(
−1)
deg /2
Γ(1 + δ) = Γ(1
− δ)(−1)
deg /2
(
−1)
deg /2
Ch(v) = Ch(v
∨
).
Denote by
ν
1
, . . . , ν
n
the Chern root ofT
X
andǫ
1
, . . . , ǫ
k
the Chern roots ofE
. From the above properties, we dedu e thatS(
Z
tw
(v
1
),
Z
tw
(v
2
)) =
Z
X
c
top
(
E)e
c
1
(T
X
⊗E
∨
)/2
n
Y
i=1
Γ
1 +
ν
i
2
√
−1π
Γ
1
−
ν
i
2
√
−1π
∪
k
Y
j=1
Γ
1 +
ǫ
j
2
√
−1π
−1
Γ
1
−
ǫ
j
2
√
−1π
−1
Ch(v
1
⊗ v
2
∨
)
Usingthe formalidentity
Γ(z)Γ(1
− z) =
π
sin(πz)
, we dedu e thatΓ(1
− z)Γ(1 + z) =
ze
−z/2
1
− e
−z
.
This implies the formula.
Re all fromDenition 2.21 that we denote
F
Z
the integral stru tureZ
tw
(K(X))
.
Denition 2.24. Thetwisted quantum
D
-moduledenotedbyQDM(X,
E)
isthe quadru-ple(F,
∇, S, F
Z
)
.2.2. Redu edquantum
D
-module. Inthissubse tionwedenetheredu edquantumD
-module, denoted byQDM(X,
E)
, whi h is a quadrupleF ,
∇, S, F
Z
. The pairing
S
is non-degenerated.Re all that
m
c
top
isthe endomorphismm
c
top
: H
2∗
(X)
−→ H
2∗
(X)
α
7−→ c
top
(
E) ∪ α.
Put
H
2∗
(X) := H
2∗
(X)/ ker m
c
top
and all it the redu ed ohomology ring of(X,
E)
. Sin em
c
top
is agraded morphism, the ve tor spa eH
2∗
(X)
is naturally graded. Forγ
∈ H
2∗
(X)
,
we denoteby
γ
its lass inH
2∗
(X)
.Denote by
F
the trivialbundleH
2∗
(X)
× H
0
(X)
× V × C → H
0
(X)
× V × C
. On
F
,we willdene a onne tion∇
and a non-degenerated paringS
. They willbe indu ed by those onF
.For any
γ
1
, γ
2
∈ H
2∗
(X)
, dene the redu ed pairing
(
·, ·)
red
whi h is a bilinear form on
H
2∗
(X)
by(γ
1
, γ
2
)
red
:= (γ
1
, γ
2
)
tw
.
ByProposition2.19,
ker m
c
top
isthekernelofthe twistedpairing. Itfollows thattheredu ed pairing isa welldened and non degenerated bilinearform.Wedene the pairing
S
as we did forS
but hanging(
·, ·)
tw
by
(
·, ·)
red
( f.before
Propo-sition 2.20). From (2.25),for any
s
1
, s
2
∈ Γ(H
0
(X)
× V × C, F)
,we dedu e that
S(s
1
, s
2
) = S(s
1
, s
2
)
(2.26)
Let
(φ
0
, . . . , φ
s
′
−1
)
be a homogeneousbasis ofH
2∗
(X)
and denote(φ
0
, . . . , φ
s
′
−1
)
its dual basis with respe t to(
·, ·)
red
.
Denition 2.27. Let
γ
1
, . . . , γ
n
be lasses inH
2∗
(X)
.
1. Let
d
beinH
2
(X, Z)
. The redu ed Gromov-Witten invariant ishγ
1
, . . . , γ
n
i
red
0,ℓ,d
:=
hγ
1
, . . . , ^
c
top
(
E)γ
n
i
0,ℓ,d
2. The redu ed quantum produ t is
γ
1
•
red
q
γ
2
:=
s−1
X
a=0
X
d∈H
2
(X,Z)
q
d
hγ
1
, γ
2
, φ
a
i
red
0,3,d
φ
a
Remark 2.28. By the twisted
S
n
-symmetri axiom ( f.Proposition A.2), the redu ed Gromov-Witteninvariants are welldened onthe lass inH
2∗
(X)
. Noti e that the redu ed Gromov-Witten invariant areS
n
symmetri . The onvergen e domain of•
red
q
ontainsV
. Wewillrestri t ourselvestoV
.Proposition 2.29. For any
γ
1
, γ
2
inH
2∗
(X)
, we have
γ
1
•
tw
q
γ
2
= γ
1
•
red
q
γ
2
Proof. Using Formula(2.8) for the twisted quantum produ t we get :
γ
1
•
tw
q
γ
2
=
X
d∈H
2
(X,Z)
q
d
e
3∗
α
where we putα := e
∗
1
γ
1
∪ e
∗
2
γ
2
∪ c
top
(
E
0,3,d
(3))
∩ [X
0,3,d
]
vir
. Denote byφ
b
a
∈ H
2∗
(X)
a lift ofφ
a
. ByDenition (2.25),wehavee
3∗
α =
s
′
−1
X
a=0
(e
3∗
α, φ
a
)
red
φ
a
=
s
′
−1
X
a=0
e
3∗
α, b
φ
a
tw
φ
a
Usingproje tion formula, the proposition follows from
hγ
1
, γ
2
, φ
a
i
red
0,3,d
=
hγ
1
, γ
2
,
c
top
^
(
E)b
φ
a
i
0,3,d
=
e
3∗
α, b
φ
a
tw
Dene the following onnexionon the bundle
F
:∇
∂
t0
:= ∂
t
0
+
1
z
1
•
red
q
,
∀a ∈ {1, . . . , r}, ∇
δa
:= δ
a
+
1
z
T
a
•
red
q
∇
δ
z
:= δ
z
−
1
z
E
•
red
q
+µ
where
µ
isthe diagonalmorphismdened byµ(φ
a
) :=
1
2
(deg(φ
a
)
− (dim
C
X
− rk E)) φ
a
andE
:= t
0
1
+ c
1
(
T
X
⊗ E
∨
)
.
Corollary 2.30. For any
γ
∈ H
2∗
(X)
, we have :
Proof. This follows from Proposition 2.29 and from
µ(T
a
) = µ(T
a
)
. Lemma 2.31. For any(t
0
, q, z)
inH
0
(X)
× V × C
, we have :
L
tw
(t
0
, q, z)(ker m
c
top
) = ker m
c
top
.
Proof. Let
γ
be inker m
c
top
andα
∈ H
2∗
(X)
. Sin eL
tw
(t
0
, q, z)
is an automorphism ofH
2∗
(X)
andker m
c
top
is the kernel of the twisted pairing(
·, ·)
tw
we nd, using Proposition 2.20 :α, L
tw
(t
0
, q, z)γ
tw
= L
tw
(t
0
, q,
−z).(L
tw
(t
0
, q,
−z))
−1
.α, L
tw
(t
0
, q, z)γ
tw
= L
tw
(t
0
, q,
−z)
−1
α, γ
tw
= 0.
ThenL
tw
(t
0
, q, z)γ
belongs toker m
c
top
.This lemma permit usto denea redu ed
L
fun tion : for any(t
0
, q, z)
∈ V × C
putL(t
0
, q, z) : H
2∗
(X)
−→ H
2∗
(X)
(2.32)
γ
7−→ L(t
0
, q, z)γ = L
tw
(t
0
, q, z)γ
Inthesamespiritof2.1.e,wealsogetanindu edintegralstru ture on
QDM(X,
E)
. Denote byK(X) := K(X) /
{v | Ch(v) ∈ ker m
c
top
}.
TheChern hara ter
Ch : K(X)
→ H
2∗
(X)
indu esaredu edChern hara ter
Ch : K(X)
→
H
2∗
(X)
whi h be ome anisomorphism aftertensored byC
. Foranyv
∈ K(X)
, we putZ(v) := (2π)
−(n−k)/2
L(t
0
, q, z)z
−µ
z
c
1
(T
X
⊗E
∨
)
b
Γ(
T
X
)b
Γ(
E)
−1
(2
√
−1π)
deg /2
Ch(v).
Inthe same spiritofDenition2.21, the redu ed
b
Γ
-integralstru ture onQDM(X,
E)
isgiven byZ(K(X))
and we denote itbyF
Z
.Corollary 2.33. The triple
(F ,
∇, S)
satises the following properties. 1. The onne tion∇
isat andS
is non-degenerated and∇
-at.2. A fundamental solution of
∇
is given byL(t
0
, q, z)z
−µ
z
c
1
(T
X
⊗E
∨
)
. 3. For anys
1
, s
2
∈ Γ(F)
, we haveS(L(q, z)s
1
, L(q, z)s
2
) = S(s
1
, s
2
)
4. For anyv
inK(X)
, we haveZ(v) = Z
tw
(v).
5. For anyv
1
, v
2
inK(X)
, we haveS(
Z(v
1
),
Z(v
2
)) =
Z
X
c
top
(
E) Td(T
X
) Td(
E)
−1
Ch(v
1
⊗ v
2
∨
).
Proof. (1)Proposition 2.17and Corollary2.30 impliesthe atnessfor
∇
. The atnessofS
follows from Proposition2.20 and Equality (2.26).(2) This statement follows easilyfromCorollary 2.30 and Proposition 2.17.
(3) The equality follows fromProposition 2.20 and Equality (2.26).
(4) This follows fromthe statement (2).
(5) Theequalityfollowsfromthe previousequality,Equation(2.26)andProposition2.23.
Denition 2.34. The redu ed quantum