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H

IGHER

L

ODAY ALGEBRAS

Norbert Poncin

University of Luxembourg

Geometry of Manifolds and Mathematical Physics Krakow 2011

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O

UTLINE

Higher (Lie and) Loday (Leibniz) algebras:

1 Coalgebraic approach

2 Category theoretical standpoint

3 Operadic view

4 Supergeometric framework

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L

IE AND

L

ODAY INFINITY CATEGORIES

C

OALGEBRAIC APPROACH

(4)

L

ALGEBRAS

:

HOMOTOPY INVARIANT EXTENSIONS OF

DGLA

S

(L,d)

p

i (V,d) pi=idV,ip∼h idL

(L,d) :DGLA⇒(V,d) :Lalgebra THEOREM

(L,d)and(V,d)homotopy equivalent ds. AnLstructure on L induces anLstructure on V .

⇝Importance ofLin BRST, closed string theory

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L

ALGEBRAS

: DQ

OF

P

OISSON MANIFOLDS

(V,[−,−]) :GLA,𝜋 ∈V1,[𝜋, 𝜋] =0 𝔤:=𝜈V[[𝜈]],(𝔤,[−,−], ∂𝜋): DGLA

𝜋𝜈 =𝜋+𝜎, s.th. 𝜎∈MC(𝔤) ={s∈𝔤1:∂𝜋s+12[s,s] =0}

Def(𝔤) =MC(𝔤)/G(𝔤) Def:L→Set THEOREM

If F :L→L is a Qiso, thenDef(F) :Def(L)→Def(L)is bijective.

L= (Tpoly(M) = Γ(∧TM),[−,−]SN,0): DGLA L= (Dpoly(M)⊂ ℒ(C(M)),[−,−]G, ∂𝜇): DGLA

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L

ALGEBRAS

𝜋p: (sV)∨p→sV, 𝜋:S(sV)→sV

L(V)

∥ +

{(𝜋1, 𝜋2, 𝜋3, . . .), multilin., AS,∣𝜋p∣=2−p}

CoDiff1(S(sV))

∥ +

CoDer1(S(sV))

1)𝜋12=0 2)𝜋1der. of𝜋2 3)𝜋2Jacobi id. modulo homotopy Example: (𝜋1, 𝜋2,0, . . .)DGLA

seq. conditions

Q2=0= [Q,Q]

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L

ALGEBRAS

𝜋p: (sV)∨p→sV, 𝜋:S(sV)→sV

L(V)

∥ +

{(𝜋1, 𝜋2, 𝜋3, . . .), multilin., AS,∣𝜋p∣=2−p}

CoDiff1(S(sV))

∥ +

CoDer1(S(sV))

1)𝜋12=0 2)𝜋1der. of𝜋2 3)𝜋2Jacobi id. modulo homotopy Example: (𝜋1, 𝜋2,0, . . .)DGLA

seq. conditions

Q2=0= [Q,Q]

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L

ALGEBRAS

𝜋p: (sV)∨p→sV, 𝜋:S(sV)→sV

L(V)

∥ +

{(𝜋1, 𝜋2, 𝜋3, . . .), multilin., AS,∣𝜋p∣=2−p}

CoDiff1(S(sV))

∥ +

CoDer1(S(sV))

1)𝜋12=0 2)𝜋1der. of𝜋2 3)𝜋2Jacobi id. modulo homotopy Example: (𝜋1, 𝜋2,0, . . .)DGLA

seq. conditions ≃ Q2=0= [Q,Q]

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Lod

ALGEBRAS [AMMAR, P, ’08]

Lod(V)

∥ +

@

@

{(𝜋1, 𝜋2, 𝜋3, . . .), multilin., AS,∣𝜋p∣=2−p}

CoDiff1(T(sV))

∥ +

CoDer1(T(sV))

?

?

1)𝜋21=0 2)𝜋1der. of𝜋2 3)𝜋2Jacobi id. modulo homotopy Example:(𝜋1, 𝜋2,0, . . .)DGLodA

? seq. conditions ≃? Q2=0= [Q,Q]

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T

WISTED COASSOCIATIVE COALGEBRA

THEOREM

Δ(v1⊗. . .⊗vp−1⊗vp) =

p−2 i=1

𝜎∈sh(i,p−1−i)±v𝜎(1)⊗. . .⊗v𝜎(i)

v𝜎(i+1)⊗. . .⊗ v𝜎(p−1)⊗vp

(T(V),Δ):twistedcoassociative coalgebra, i.e.

(id⊗

Δ)Δ = (Δ⊗

id)Δ +(T⊗

id)(Δ⊗ id)Δ

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Lod

CONDITIONS

THEOREM

Cn=

i+j=n+1

k≥j

𝜎∈sh(k−j,j−1)

𝜒(𝜎)(−1)(k+i−j)(j−1)(−1)j(v𝜎(1)+...+v𝜎(k−j)) 𝜋i(v𝜎(1), ...,v𝜎(k−j), 𝜋j(v𝜎(k+1−j), ...,v𝜎(k−1),vk),vk+1, ...,vn) =0,

𝜒(𝜎) :Koszul sign, n≥1.

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Lod

COHOMOLOGY

Lod(V)

∥ +

{seq. 𝜋= (𝜋1, 𝜋2, . . .)multilin.,∣𝜋p∣=2−p}

[𝜋, 𝜋]Stem=0?

Cochain space={seq. multilin.}

[−,−]Stem?

⇝Lodcohomology ?

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Lod

COHOMOLOGY

Lod(V)

∥ +

{seq.𝜋 = (𝜋1, 𝜋2, . . .)multilin.,∣𝜋p∣=2−p}

CoDiff1(T(sV))

∥ +

CoDer1(T(sV))

[𝜋, 𝜋]Stem=0 ≃ Q2=0= [Q,Q]

Cochain space={seq. multilin.} ≃ CoDer(T(sV))

≃ [−,−]

[−,−]Stem

⇝Lodcohomology

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S

TEM BRACKET

THEOREM

[𝜋, 𝜌]Stem=∑

q≥1

s+t=q+1

(−1)1+(s−1)⟨e1,𝜌⟩[𝜋s, 𝜌t]Stem,

[A,B]Stem=jAB−(−1)⟨(A,a),(B,b)⟩jBA,

jBA= (−1)⟨A,B⟩

I∪J∪K=N(a+b+1) I,J<K,∣J∣=b

(−1)⟨B,VI⟩+b∣I∣(−1)(I;J)𝜀V(I;J)

A(VI ⊗B(VJ⊗vk1)⊗VK∖k1)

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D

ESCENDANTS

THEOREM

[𝜋,−]Stemencodes

graded Loday (DT), graded Lie (LMS), graded Poisson, graded Jacobi (GM, up to isom) cohomologies

Loday infinity, Lie infinity (FP),2n-ary graded Loday and Lie(MV, VV) cohomologies

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C

ATEGORY THEORETICAL APPROACH

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C

ATEGORIFICATION

-

A SHARPER VIEWPOINT

Sets⇝categories Maps⇝functors

Equations⇝natural isomorphisms + coherence laws

1 vs≃linear set⇝2vs≃linear category

2 LA≃vs + bilinear map + AS, Jacobi

L2A≃2vsL+ bilinear functor[−,−]+ trilinear natural isomorphismJ : [−,[−,−]]+↻⇒ 0 + coherence laws Semistrict L2A [Baez, Crans, ’04], weak L2A [Roytenberg,

’07]

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2

CATEGORIES

2 category (rough description):

objectsA,1-morphismsf :A→B,2-morphisms 𝛼:f ⇒f (homological algebra, string theory)

vertical composition:f,f,f′′∈Hom(A,B),𝛼:f ⇒f, 𝛽 :f ⇒f′′,

𝛼∙𝛽 :f ⇒f′′

functorial horizontal composition:

∘:Hom(A,B)×Hom(B,C)→Hom(A,C)is a bifunctor, i.e.

is s.th. if𝛼:f ⇒f,𝛽 :g⇒g, then 𝛼∘𝛽 :f ∘g ⇒f∘g

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H

ORIZONTAL AND VERTICAL COMPOSITIONS

CCCC

//EE

~~

// // CC

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2

CATEGORY

Lie2Alg

Objects: L2A(L,[−,−],J),(L,[−,−],J), . . . 1-morphisms:

lin funF :L→L

bilin natural isoF2: [−,−]∘(F ⊗F)⇒F ∘[−,−]

respect of Jacobiators 2-morphisms:

lin natural transfo𝜃:F :L→L⇒G:L→L respect ofF2andG2

2vs:s,t :L1→L0 + 1,∘; 2term:𝜋1:V1→V0; 𝜋1=t∣kers Lie2Alg

≃2TermL

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2

CATEGORY

Lie2Alg

Objects: L2A(L,[−,−],J),(L,[−,−],J), . . . 1-morphisms:

lin funF :L→L

bilin natural isoF2: [−,−]∘(F ⊗F)⇒F ∘[−,−]

respect of Jacobiators 2-morphisms:

lin natural transfo𝜃:F :L→L⇒G:L→L respect ofF2andG2

2vs:s,t :L1→L0 + 1,∘; 2term:𝜋1:V1→V0; 𝜋1=t∣kers Lie2Alg≃2TermL

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2

CATEGORY

Lod2Alg

THEOREM

Lod2Alg≃2TermLod Suppression of AS = destruction of simplifications Conceptual approach to and explicit formulae for 1- and 2-morphisms

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C

ATEGORIFICATION VS

.

HOMOTOPIFICATION

[KHUDAVERDYAN, MANDAL, P, ’10]

Conjecture 1:LnA≃nTermL

L2A ∼ catL fun[−,−] transJ coh

L3A :∼ 2-catL 2-fun[−,−] 2-transJ 2-modI ?coh?

↕ ↕ (1)(2)(3)(4)(5)

3TermL ∼ Vi, 𝜋1,C1 𝜋2,C2 𝜋3,C3 𝜋4,C4 C5 Answer 1a: (5) involves more than 100 terms

Answer 1b: (2) is “[−,−]respects∘ ↔C2” and holds true only under two (acceptable)conditions

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C

ATEGORIFICATION VS

.

HOMOTOPIFICATION

Fact:Vectn-Catis a symmetric monoidal category L×L → L′′

⊠ ↓ ↗ L⊠L

!⊠:L×L →L⊠L is not ann-functor ! (★)

Conjecture 2: Use

𝒩 :VectCat→s(Vect),N :s(Vect)→C+(Vect), EZ:N(S)⊗N(T)↔N(S⊗T) :AW

Answer 2:Obstruction = defect (★)

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O

PERADIC APPROACH

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D

EFINITION OF AN OPERAD

5 definitions:

classical, partial compositions, type of algebras, functorial, combinatorial

algebra→matrices, operad→algebra operad:

vsP(n),n∈ℕ, of abstractn-ary operations -Tn

Sn-module structure onP(n) linear composition maps

𝛾i1...ik :P(k)⊗P(i1)⊗. . .⊗P(ik)→P(i1+. . .+ik), which are associative, respect theS-action (and possibly the unit)

(27)

D

EFINITION OF AN OPERAD

5 definitions:

classical, partial compositions, type of algebras, functorial, combinatorial

algebra→matrices, operad→algebra operad:

vsP(n),n∈ℕ, of abstractn-ary operations -Tn Sn-module structure onP(n)

linear composition maps

𝛾i1...ik :P(k)⊗P(i1)⊗. . .⊗P(ik)→P(i1+. . .+ik), which are associative, respect theS-action (and possibly the unit)

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O

PERADS ASSOCIATED TO TYPES OF ALGEBRAS

Example:

AA

P(1) =𝕂T1

P(2) =𝕂T2(12) +𝕂T2(21)(encoding of symmetries) P(3) =𝕂T2(T2,T1) +𝕂T2(T1,T2)(encoding of defining relations)

P(n) =𝕂[Sn] General case:

type of algebras

generating operations with symmetries⇝Sn-moduleM(n) defining relations⇝ideal (R)

operadP=ℱ(M)/(R)

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T

WISTING MORPHISMS

A: D(GA)A, C: D(GA)C, suspensions + reductions understood Homalg(T(C),A)≃Hom𝕂(C,A)≃Homcoalg(C,Tc(A)) ΩC: DAcobar complex, BA: DC bar complex

d2(a1⊗. . .⊗an) =∑

±a1⊗. . .⊗𝜇(ai,ai+1)⊗. . .⊗an

HomDA(ΩC,A)≃TW(C,A)≃HomDC(C,BA) Qiso(ΩC,A)≃Kos(C,A)≃Qiso(C,BA)

d𝛼 :C⊗AΔ⊗id→ C⊗C⊗Aid⊗𝛼⊗id→ C⊗A⊗Aid⊗𝜇C⊗A

ΩBA→ A: bar-cobar resolution of A

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K

OSZUL DUALITY FOR ALGEBRAS AND OPERADS Quadratic data:V,R⊂V⊗2(e.g. R=⟨v ⊗v−v⊗v⟩) Quadratic algebra:A(V,R) =T(V)/(R)⊃𝕂⊕V (e.g. S(V)) Quadratic coalgebra:

C(V,R) =𝕂⊕V ⊕⊕

k≥2

i+j+2=k

V⊗i⊗R⊗V⊗j ⊂Tc(V) Koszul dual coalgebra ofA(V,R):

A¡ =C(sV,s2R)⊃𝕂⊕sV TW(A¡,A)∋𝛼:A¡ ↠sV →V ↣A

If𝛼∈Kos(A¡,A), then

ΩA¡ → A

Extension of this minimal model ofKoszul algebras[Priddy, ’70]

toKoszul operads[Ginzburg, Kapranov, ’94]

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I

NFINITY ALGEBRAS VIA OPERADS

End(V): endomorphism operad on a vsV

P→End(V): operadic morphism,typeP algebra structure onV

IfP is aKoszul operad,

P:=

ΩP¡ → P

↘ ↓

End(V)

FromΩℒie¡andΩℒod¡we recoverLandLodstructures onV

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I

NFINITY ALGEBRAS VIA OPERADS

End(V): endomorphism operad on a vsV

P→End(V): operadic morphism,typeP algebra structure onV

IfP is aKoszul operad,

P:=ΩP¡ → P

↘ ↓

End(V)

FromΩℒie¡andΩℒod¡we recoverLandLodstructures onV

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O

CCURRENCES OF

L

ODAY AND

Lod

ALGEBRAS

Leibniz (Loday) algebras

★Origin: periodicity phenomena inK-theory

★Examples:

1 Courant-Dorfman bracket, Courant algebroid bracket

2 Loday bracket associated with a Nambu-Poisson structure

3 Derived brackets Loday infinity algebras

★Origin: universal GLA and cohomologies

★Examples:

1 Fulton-MacPherson type compactification [Kontsevich, ’03]

[Merkulov, ’09]

2 Formal deformation of a DGLodA and derived brackets [Uchino, ’09]

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S

UPERGEOMETRIC APPROACH

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K

OSZUL DUALITY FOR OPERADS REVISITED

Ginzburg-Kapranov, ’94:

P-algebra onV ⇌Q∈Der1(ℱPgr!(sV)),Q2=0 Example:

L-algebra⇌homological vf on apointed formal smfd Geometric ‘example’:

L-algebroid⇌homological vf on asplitℕ-mfd Particular case:

LAD⇌homological vf on asplit smfd

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R

EQUIREMENTS

Find a concept ofLoday algebroidthat is close to the notion of Lie algebroid

contains Courant algebroids as special case reduces to a Loday algebra over a point

includes a differentiability condition on both arguments, and interpret it ashomological vf on a supercommutative mfd

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L

ODAY ALGEBROIDS

:

FIRST ATTEMPT

‘Definition’: ALoday algebroidis a Loday bracket[−,−]on sections of a vbE together with aleft and right anchor J. Grabowski, G. Marmo:

Ifrk(E) =1,[−,−]is AS and 1st order Ifrk(E)>1,[−,−]is ‘locally’ aLAD bracket

‘No’ new examples⇝modify ‘definition’

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L

ODAY ALGEBROIDS

:

SECOND ATTEMPT

𝜌: Γ(E)→DerC(M),C(M)-linear

x(fY) =∂xf Y +f ∂xY,∂x2(fY) =∂2xf Y +2∂xf∂xY +f ∂x2Y [X,fY] =f[X,Y] +𝜌(X)f Y

[Xiei,fYjej] =

XiakijfYj ek+Xi𝜌aiaf Yjej+Xi𝜌ai f ∂aYj ej−Yi𝜌aiaXj ej 𝜌(X)(df⊗Y) =Xi𝜌akijaf Yjek

𝜌: Γ(E)C

(M)−lin

−→ Γ(TM)⊗C(M)EndC(M)Γ(E) 𝜌:E →TM⊗EndE

Cohomology theory⇝representation,traditional left anchor

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D

EFINITION [GRABOWSKI, KHUDAVERDYAN, P, ’11]

DEFINITION

ALoday algebroid(LodAD) is a Loday bracket on sections of a vb EM together with two bundle maps𝜌:ETMand

𝛼:ETMEndE such that

[X,fY] =f[X,Y] +𝜌(X)f Y and

[fX,Y] =f[X,Y]𝜌(Y)f X+𝛼(Y)(df X).

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C

OURANT ALGEBROID ET AL

EXAMPLES

Loday algebra

(twisted) Courant-Dorfman (TM⊕TM)

Grassmann-Dorfman (TM⊕ ∧TM orE⊕ ∧E)

Leibniz algebroid associated to a Nambu-Poisson structure Courant algebroid

...

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E

XTENSION TO

L

ODAY ALGEBROIDS

(I)

(E,[−,−], 𝜌)⇌Q∈Der1(Γ(∧E),∧),Q2=0 (E,[−,−], 𝜌)→LAD cohomology operator𝜌

𝜌is the C-E operator restricted to

C(M)(Γ(E),C(M)) = Γ(∧E)

𝜌is the Loday operator restricted to LinC(M)

D

(Γ(E),C(M)) = Γ(⊗E)

=:D(E)

(D⋔Δ)(X1, . . . ,Xp+q)

= ∑

𝜎∈sh(p,q)

sign(𝜎)D(X𝜎1, . . . ,X𝜎p) Δ(X𝜎p+1, . . . ,X𝜎p+q)

(42)

E

XTENSION TO

L

ODAY ALGEBROIDS

(I)

(E,[−,−], 𝜌)⇌Q∈Der1(Γ(∧E),∧),Q2=0 (E,[−,−], 𝜌)→LAD cohomology operator𝜌

𝜌is the C-E operator restricted to

C(M)(Γ(E),C(M)) = Γ(∧E)

𝜌is the Loday operator restricted to

LinC(M)

D(Γ(E),C(M))

= Γ(⊗E)

=:D(E)

(D⋔Δ)(X1, . . . ,Xp+q)

= ∑

𝜎∈sh(p,q)

sign(𝜎)D(X𝜎1, . . . ,X𝜎p) Δ(X𝜎p+1, . . . ,X𝜎p+q)

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E

XTENSION TO

L

ODAY ALGEBROIDS

(I)

(E,[−,−], 𝜌)⇌Q∈Der1(Γ(∧E),∧),Q2=0 (E,[−,−], 𝜌)→LAD cohomology operator𝜌

𝜌is the C-E operator restricted to

C(M)(Γ(E),C(M)) = Γ(∧E)

𝜌is the Loday operator restricted to

LinC(M)

D(Γ(E),C(M))

= Γ(⊗E)

=:D(E)

(D⋔Δ)(X1, . . . ,Xp+q)

= ∑

𝜎∈sh(p,q)

sign(𝜎)D(X𝜎1, . . . ,X𝜎p) Δ(X𝜎p+1, . . . ,X𝜎p+q)

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E

XTENSION TO

L

ODAY ALGEBROIDS

(II)

(E,[−,−], 𝜌, 𝛼)⇌Q∈Der1(D(E),⋔),Q2=0

𝒟k(E)⊂Dk(E):k-DO of deg 0 in last section and tot degk −1 𝒟k(E)⋔𝒟(E)⊂ 𝒟k+ℓ(E): reduced shuffle algebra

𝜌𝒟k(E)⊂ 𝒟k+1(E): LodAD subcomplex

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E

XTENSION TO

L

ODAY ALGEBROIDS

(III)

(E,[−,−], 𝜌, 𝛼)⇌Q∈Der1(𝒟(E),⋔),Q2=0

𝜌(X)f :=⟨Qf,X⟩

⟨ℓ,[X,Y]⟩=⟨X,Q⟨ℓ,Y⟩⟩ − ⟨Y,Q⟨ℓ,X⟩⟩ −(Qℓ)(X,Y)

Q(𝒟2(E))↮Q(𝒟0(E)⊕ 𝒟1(E))

𝒟er1(𝒟(E),⋔)⊂Der1(𝒟(E),⋔): deg 1 der + appropriate rel (E,[−,−], 𝜌, 𝛼)⇌Q∈ 𝒟er1(𝒟(E),⋔),Q2=0

(E,[−,−], 𝜌, 𝛼)⇌[Q]∈ 𝒟er1(𝒟(E),⋔),Q2=0

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L

OD

AD

AS HOMOLOGICAL VF

THEOREM

There is a 1-to-1 correspondence between LodAD structures on a vb E andequivalence classes of homological vfs

Q∈ 𝒟er1(𝒟(E),⋔),Q2=0 of the supercommutative mfd(𝒟(E),⋔).

Remarks: Homological vfQ⇝ Cartan calculusfor(D(E),⋔)

LodAD bracket isderived bracketgiven by gLa (Der(D(E),⋔),[−,−]c)and its interior der[Q,−]c

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R

EFERENCES

1 M. Ammar, P,Coalgebraic Approach to the Loday Infinity Category, Stem Differential for 2n-ary Graded and Homotopy Algebras, Ann. Inst. Fourier, 60(1), 2010, pp 321-353

2 D. Khudaverdyan, A. Mandal, P,Equivalence of the 2-categories of categorified Loday algebras and 2-term Loday infinity algebras, draft

3 D. Khudaverdyan, A. Mandal, P,Higher categorified algebras versus bounded homotopy algebras, Theo. Appl.

Cat., Vol. 25, No. 10, 2011, pp 251-275

4 P. Hilger, A. Mandal, P,Lectures on Operad Theory, preprint

5 J. Grabowski, D. Khudaverdyan, P,Loday algebroids and their supergeometric interpretation, preprint arXiv:

1103.5852

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Thank you!

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For any unital ring R , the category Ch + (R) of non-negatively graded chain complexes of left R -modules is a nitely ( and thus a cobrantly ) generated model category ( in the sense

Partial algebra, congruence relation, gamp, pregamp, variety of alge- bras, critical point, Condensate Lifting Lemma, lattice, congruence-permutable.. This work was partially