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Joint work with Yves Félix, Aniceto Murillo and Daniel Tanré
If 𝒻: 𝑿 ⟶ 𝒀 is a continuous map between simply
connected CW-complexes, the following properties are
equivalent:
1. 𝜋𝑛 𝒻 ⨂ℚ ∶ 𝜋𝑛 𝑿 ⨂ℚ⟶ 𝜋𝑛 𝒀 ⨂ℚ , 𝑛 ≥ 2.≅
2. 𝐻𝑛 𝒻 ⨂ℚ ∶ 𝐻𝑛 𝑿 ;ℚ ⟶ 𝐻𝑛 𝒀 ;ℚ , 𝑛 ≥ 2.≅
Such a map is called a rational homotopy equivalence.
𝑿 is rational if its homotopy groups are ℚ-vector spaces.
A rationalisation of 𝑿 is a pair (𝑿ℚ , 𝑒), with 𝑿ℚ a rational
space and and 𝑒 ∶ 𝑿 ⟶ 𝑿ℚ a rational homotopy equivalence.
The study of the rational homotopy type of 𝑿 is the
study of the homotopy type of its rationalisation 𝑿ℚ.
The study of the rational homotopy type of 𝑿 is the
study of the homotopy type of its rationalisation 𝑿ℚ.
Then, if 𝑿 is a finite simply connected CW-complex
𝜋𝑛 𝑿 = ⨁𝑟ℤ ⨁ ℤ𝑝1𝑟1⨁⋯⨁ ℤ𝑝𝑚𝑟𝑚
𝜋𝑛 𝑿ℚ ≅ 𝜋𝑛 𝑿 ⨂ℚ = ⨁𝑟ℚ
The rational homotopy
type of 𝑿 is completely
determined in algebraic
terms.
DGL CDGA
A differential graded Lie algebra is a
graded vector space 𝐿 = ⨁𝑝𝜖ℤ 𝐿𝑝 with:
A bilinear operation . , . ∶ 𝐿 × 𝐿 ⟶ 𝐿
such that 𝐿𝑝 , 𝐿𝑞 ⊂ 𝐿𝑝+𝑞 satisfying:
𝑎, 𝑏 = − −1 𝑝𝑞 𝑏, 𝑎 , 𝑎 ∈ 𝐿𝑝 , 𝑏 ∈ 𝐿𝑞
𝑎, [𝑏, 𝑐] = 𝑎, 𝑏 , 𝑐 + −1 𝑝𝑞 𝑏, [𝑎, 𝑐] ,
𝑎 ∈ 𝐿𝑝 , 𝑏 ∈ 𝐿𝑞 , 𝑐 ∈ 𝐿
a)
b)DGL
A linear map 𝜕 ∶ 𝐿 ⟶ 𝐿 such that
𝜕𝐿𝑝 ⊂ 𝐿𝑝−1 satisfying:
𝜕 ∘ 𝜕 = 0
𝜕 𝑎, 𝑏 = 𝜕𝑎, 𝑏 + −1 𝑝 𝑎, 𝜕𝑏 ,
𝑎 ∈ 𝐿𝑝 , 𝑏 ∈ 𝐿
A differential graded Lie algebra is a
graded vector space 𝐿 = ⨁𝑝𝜖ℤ 𝐿𝑝 with:
a)
b)DGL
DGL
𝐒𝐢𝐦𝐩𝐥𝐲 𝐜𝐨𝐧𝐧𝐞𝐜𝐭𝐞𝐝𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 DGL +⟶
𝜆 ⟶
< ∙ >𝑄
< 𝜆(𝑿) >𝑄 ≃ 𝑿ℚ
Rational homotopy
equivalencesQuasi-isomorphisms
(𝐿, ∙,∙ , 𝜕) is a DGL-model of 𝑿 if
𝜆(𝑿) 𝐿⋯⟶≃ ⟶≃
⟶≃ ⟶≃
DGL
𝐒𝐢𝐦𝐩𝐥𝐲 𝐜𝐨𝐧𝐧𝐞𝐜𝐭𝐞𝐝𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 DGL +⟶
𝜆 ⟶
< ∙ >𝑄
< 𝜆(𝑿) >𝑄 ≃ 𝑿ℚ
Rational homotopy
equivalencesQuasi-isomorphisms
(𝐿, ∙,∙ , 𝜕) is a DGL-model of 𝑿 if
(𝐿, ∙,∙ , 𝜕)⟶≃
(𝕃(𝑊), 𝑑)
Minimal Quillenmodel
𝐻𝑛( )𝐿
Rational homotopy groups
≅ 𝜋𝑛+1(𝑿)⨂ℚ
Rational homology groups
𝐿(𝕃 𝑊 , 𝜕) ⟶≃
𝑠(𝑊 ⊕ℚ) ≅ 𝐻∗(𝑋; ℚ)DGL
DGL
Spheres
Products
Wedge products
𝕃 𝑣 , 0 , 𝑣 = 𝑛 − 1is a model for the 𝑛-dimensional sphere 𝑆𝑛.
If (𝐿, 𝜕) and (𝐿′, 𝜕′) are DGL-models
for 𝑿 and 𝒀 respectively, then 𝐿 × 𝐿′, 𝜕 × 𝜕′
is a DGL-model of 𝑿 × 𝒀.
If (𝕃 𝑉 , 𝑑) and (𝕃 𝑊 , 𝑑′) are minimal DGL
models for 𝑿 and 𝒀 respectively, then
(𝕃 𝑉 ⊕𝑊 ,𝐷) is a DGL-model of 𝑿 ∨ 𝒀.
A based topological space (𝑿, ∗) ( 𝕃 𝑉 , 𝜕 )
𝑿𝑛 𝑛-skeleton ( 𝕃(𝑉<𝑛), 𝜕 )
= 𝑒𝛼𝑛+1 𝑣𝛼 ∈ 𝑉𝑛
𝑓𝛼 ∶ 𝑆𝑛 → 𝑿𝑛 ; [𝑓𝛼] ∈ Π𝑛(𝑿𝑛)
𝜕𝑣𝛼 ∈ 𝐻𝑛−1(𝕃 𝑉<𝑛 )
≅
Π𝑛(𝑿𝑛)⨂ℚ
CW-decomposition
A commutative differential graded algebra
is a graded vector space 𝐴 = ⨁𝑝𝜖ℤ 𝐴𝑝 with:
A bilinear operation ∙ ∶ 𝐴 × 𝐴 ⟶ 𝐴
such that 𝐴𝑝 ∙ 𝐴𝑞 ⊂ 𝐴𝑝+𝑞 satisfying:
𝑎 ∙ 𝑏 = −1 𝑝𝑞𝑏 ∙ 𝑎, 𝑎 ∈ 𝐴𝑝 , 𝑏 ∈ 𝐴𝑞
𝑎 ∙ (𝑏 ∙ 𝑐) = (𝑎 ∙ 𝑏) ∙ 𝑐 , 𝑎, 𝑏, 𝑐 ∈ 𝐴a)
b)CDGA
CDGA
A commutative differential graded algebra
is a graded vector space 𝐴 = ⨁𝑝𝜖ℤ 𝐴𝑝 with:
A linear map 𝑑: 𝐴 ⟶ A such that
𝑑𝐴𝑝 ⊂ 𝐴𝑝+1 satisfying:
𝑑 ∘ 𝑑 = 0
𝑑(𝑎 ∙ 𝑏) = (𝑑𝑎) ∙ 𝑏 + −1 𝑝𝑎 ∙ (𝑑𝑏) ,
𝑎 ∈ 𝐿𝑝 , 𝑏 ∈ 𝐿
a)
b)
CDGA
𝐍𝐢𝐥𝐩𝐨𝐭𝐞𝐧𝐭, 𝐟𝐢𝐧𝐢𝐭𝐞 𝐭𝐲𝐩𝒆𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 CDGA +⟶
𝐴𝑃𝐿 ⟶
< ∙ >𝑆Rational homotopy
equivalencesQuasi-isomorphisms
< 𝐴𝑃𝐿(𝑿) >𝑆 ≃ 𝑿ℚ
(𝐴, 𝑑) is a CDGA-model of 𝑿 if
𝐴𝑃𝐿(𝑿) 𝐴⋯⟶≃ ⟶≃
⟶≃ ⟶≃
CDGA
⟶𝐴𝑃𝐿
𝐍𝐢𝐥𝐩𝐨𝐭𝐞𝐧𝐭, 𝐟𝐢𝐧𝐢𝐭𝐞 𝐭𝐲𝐩𝒆𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 CDGA +
⟶
< ∙ >𝑆Rational homotopy
equivalencesQuasi-isomorphisms
< 𝐴𝑃𝐿(𝑿) >𝑆 ≃ 𝑿ℚ
(𝐴, 𝑑) is a CDGA-model of 𝑿 if
(𝐴, 𝑑)⟶≃
(⋀𝑉, 𝑑)
CDGA
Rational homotopy groups
Rational cohomology groups
𝐻∗ 𝐴, 𝑑 ≅ 𝐻∗(𝑿; ℚ )
(𝐴, 𝑑)⟶≃
(⋀𝑉, 𝑑)
Hom(𝑉𝑘 , ℚ) ≅ 𝜋𝑘(𝑿)⨂ ℚ
Eilenberg-MacLane spaces
Wedge products
Products
⋀𝑣, 0 , 𝑣 = 𝑛is a model of the Eilenberg-MacLane
space 𝐾(ℤ, 𝑛).
If (𝐴, 𝑑) and (𝐴′, 𝑑′) are CDGA-models
for 𝑿 and 𝒀 respectively, then 𝐴 × 𝐴′, 𝑑 × 𝑑′
is a CDGA-model of 𝑿 ∨ 𝒀.
If (⋀𝑉, 𝑑) and (⋀𝑊, 𝑑′) are minimal
models for 𝑿 and 𝒀 respectively, then
(⋀ 𝑉 ⊕𝑊 ,𝐷) is a CDGA-model of 𝑿 × 𝒀.CDGA
CDGA
Postnikov decomposition
𝐒𝐢𝐦𝐩𝐥𝐲 𝐜𝐨𝐧𝐧𝐞𝐜𝐭𝐞𝐝𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 DGL +⟶
𝜆 ⟶
< ∙ >𝑄
𝐍𝐢𝐥𝐩𝐨𝐭𝐞𝐧𝐭, 𝐟𝐢𝐧𝐢𝐭𝐞 𝐭𝐲𝐩𝒆𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 CDGA +⟶
𝐴𝑃𝐿 ⟶
< ∙ >𝑆
𝐒𝐢𝐦𝐩𝐥𝐲 𝐜𝐨𝐧𝐧𝐞𝐜𝐭𝐞𝐝𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 DGL +
⟶𝜆
⟶
< ∙ >𝑄
𝐍𝐢𝐥𝐩𝐨𝐭𝐞𝐧𝐭, 𝐟𝐢𝐧𝐢𝐭𝐞 𝐭𝐲𝐩𝒆𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬 CDGA +⟶
𝐴𝑃𝐿 ⟶
< ∙ >𝑆
⟶⟶ sLA⟶⟶sCHA⟶⟶sGrp
< 𝐴 >𝑆= Hom𝑪𝑫𝑮𝑨(𝐴, Ω )
< 𝐴 >𝑆 is defined for 𝐴 a ℤ-graded CDGA but
< 𝐿 >𝑄 has only sense for positively graded DGL’s
𝐒𝐢𝐦𝐩𝐥𝐲 𝐜𝐨𝐧𝐧𝐞𝐜𝐭𝐞𝐝, 𝐟𝐢𝐧𝐢𝐭𝐞 𝐭𝐲𝐩𝒆𝐂𝐖− 𝐜𝐨𝐦𝐩𝐥𝐞𝐱𝐞𝐬
⟶
⟶ℒ 𝒞∗
The goal is to understand the rational behaviour of the spaces:
map 𝑿, 𝒀 , map∗ 𝑿, 𝒀 , map𝑓 𝑿, 𝒀 , map𝑓∗ (𝑿, 𝒀)
If 𝑿 and 𝒀 are finite type
CW-complexes
map 𝑿, 𝒀 has the homotopy
type of a CW-complex.
If 𝑿 and 𝒀 are nilpotent map𝑓 𝑿, 𝒀 is nilpotent.
If 𝑿 is a finite CW-complex map𝑓 𝑿, 𝒀 is of finite type.
If 𝑿 and 𝒀 are 1-connected map𝑓 𝑿, 𝒀 is 1-connected.
Let 𝑿 be a finite CW-complex and 𝒀 be a nilpotent,
finite type CW-complex.
(𝐵⋕, 𝛿)
⋀ V⨂𝐵⋕ , 𝐷
𝐷 𝑣⨂𝛽 = σ𝑗(−1)𝑤 |𝛽𝑗
′|(𝑢⨂𝛽𝑗′) (𝑤⨂𝛽𝑗
′′) + 𝑣⨂𝛿𝛽
𝑿 (𝐵 , 𝑑) CDGA CDGC 𝐵⋕𝑛 = 𝐵−𝑛
(⋀𝑉, 𝑑)𝒀 Sullivan model
if 𝑣 ∈ V such that d𝑣 = 𝑢𝑤 and 𝛽 ∈ 𝐵⋕ with
∆𝛽 = σ𝒋𝛽𝒋′⨂𝛽𝒋
′′V⨂𝐵⋕
The following Sullivan algebra is a model for map 𝑿, 𝒀 .
Let ϕ: (⋀𝑉, 𝑑) ⟶ 𝐵 be a model of 𝑓: 𝑿 ⟶ 𝒀 .
Let 𝐾ϕ be the differential ideal generated by 𝐴1 ∪ 𝐴2 ∪ 𝐴3
𝐴1 = (𝑉 ⊗ 𝐵⋕)<0 𝐴2 = 𝐷(𝑉 ⊗ 𝐵⋕)0
𝐴3 = 𝛼 − 𝜙 𝛼 𝛼 ∈ (𝑉 ⊗ 𝐵⋕)0 }
The projection
map𝑓 𝑿, 𝒀 ⟶ map 𝑿, 𝒀
⋀ V⨂𝐵⋕ , 𝐷 ⟶ ⋀ V⨂𝐵⋕ , 𝐷 /𝐾ϕ
is a model of the injection
⋀ V⨂𝐵⋕ , 𝐷 /𝐾ϕ ≅ ⋀𝑉 ⊗𝐵⋕1⨁(𝑉 ⊗ 𝐵⋕)≥2, 𝐷𝝓
𝑿 , 𝒀 with DGL-models 𝐿 , 𝐿′ , respectively.
𝑓: 𝑿 ⟶ 𝒀 .
map𝑓 𝑿, 𝒀 ,DGL-model of map𝑓 𝑿, 𝒀 ?
(𝐵⋕, 𝛿)𝑿 CDGC 𝐵⋕, 𝛿 = 𝒞∗(𝐿) Cartan-Eilenberg
(⋀𝑉, 𝑑)𝒀 Sullivan model ⋀𝑉, 𝑑 = 𝒞∗ 𝐿′ cochains on 𝐿′
map𝑓 𝑿, 𝒀 ,DGL-model of map𝑓 𝑿, 𝒀 ?
(𝐵⋕, 𝛿)𝑿 CDGC 𝐵⋕, 𝛿 = 𝒞∗(𝐿) Cartan-Eilenberg
(⋀𝑉, 𝑑)𝒀 Sullivan model ⋀𝑉, 𝑑 = 𝒞∗ 𝐿′ cochains on 𝐿′
Consider the ℤ-graded vector space 𝐻𝑜𝑚ℚ(𝒞∗ 𝐿 ′ 𝐿′).
Let f ∶ 𝒞∗ 𝐿 ⟶ 𝐿′ be a linear map of degree 𝑝.
𝔇f = f ∘ δ − −1 f 𝜕′ ∘ f ∶ 𝒞∗ 𝐿 ⟶ 𝐿′
(𝐵⋕, 𝛿)𝑿 CDGC 𝐵⋕, 𝛿 = 𝒞∗(𝐿) Cartan-Eilenberg
(⋀𝑉, 𝑑)𝒀 Sullivan model ⋀𝑉, 𝑑 = 𝒞∗ 𝐿′ cochains on 𝐿′
Consider the ℤ-graded vector space 𝐻𝑜𝑚ℚ(𝒞∗ 𝐿 ′ 𝐿′).
Let f , g ∶ 𝒞∗ 𝐿 ⟶ 𝐿′ be linear maps of degree
𝑝 and 𝑞 respectively.
𝒞∗ 𝐿
𝒞∗ 𝐿 ⨂𝒞∗ 𝐿
⟶
∆
⟶f ⊗ g
𝐿′⨂ 𝐿′
⟶[f, g ]
⟶
𝐿′
[−,−]
( 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′ , 𝔇, −,− ) is a DGL-model of map (𝑿, 𝒀)
𝒞∗ 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′ , 𝔇, −,− = ⋀ V⨂𝐵⋕ , 𝐷
U. Buijs, Y. Félix and A. Murillo, Trans. Amer. Math.Soc. 2008
𝒞∗ 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′ , 𝔇, −,− = ⋀ V⨂𝐵⋕ , 𝐷
What about the components ⋀𝑉 ⊗ 𝐵⋕1⨁(𝑉 ⊗ 𝐵⋕)≥2, 𝐷𝝓 ?
ϕ|(𝑠𝐿′)⋕⋕ : 𝒞∗ 𝐿 ⟶ 𝑠𝐿′⟶ 𝐿′෨𝜙
𝒻: 𝑋 ⟶ 𝑌
𝜙: 𝒞∗(𝐿′) ⟶ 𝒞∗ 𝐿⋕
𝜙:⋀(𝑠𝐿′)⋕⟶ 𝒞∗ 𝐿⋕
𝜙|(𝑠𝐿′)⋕: (𝑠𝐿′)⋕⟶ 𝒞∗ 𝐿⋕
Continuous function
𝜙: (⋀𝑉, 𝑑) ⟶ 𝐵 CDGA-morphism
Linear map of degree 0
Linear map of degree -1
𝒞∗ 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′ , 𝔇, −,− = ⋀ V⨂𝐵⋕ , 𝐷
What about the components ⋀𝑉 ⊗ 𝐵⋕1⨁(𝑉 ⊗ 𝐵⋕)≥2, 𝐷𝝓 ?
ϕ|(𝑠𝐿′)⋕⋕ : 𝒞∗ 𝐿 ⟶ 𝑠𝐿′⟶ 𝐿′෨𝜙 Linear map of degree -1
෩𝜙 ∈ 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′−1 𝔇෪𝜙 = 𝔇+ 𝑎𝑑෪𝜙
Maurer-Cartan equation
is a differential if and only if
𝔇෩𝜙 = −1
2[ ෩𝜙 , ෩𝜙 ]
𝒞∗ 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′ , 𝔇, −,− = ⋀ V⨂𝐵⋕ , 𝐷
What about the components ⋀𝑉 ⊗ 𝐵⋕1⨁(𝑉 ⊗ 𝐵⋕)≥2, 𝐷𝝓 ?
ϕ|(𝑠𝐿′)⋕⋕ : 𝒞∗ 𝐿 ⟶ 𝑠𝐿′⟶ 𝐿′෨𝜙 Linear map of degree -1
෩𝜙 ∈ 𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′−1 𝔇෪𝜙 = 𝔇+ 𝑎𝑑෪𝜙
𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′𝑛
෩𝜙=
0 if 𝑛 < 0
𝐻𝑜𝑚ℚ 𝒞∗ 𝐿 ′ 𝐿′𝑛 if 𝑛 > 0
if 𝑛 = 0Ker 𝔇෪𝜙
Let 𝑨 be an associative algebra.
𝑨 × 𝑨⟶ 𝑨 bilinear and associative.
(𝒂, 𝒃) ⟼ 𝒂 ∙ 𝒃
𝑨 𝑡 = {
𝑖=0
∞
𝒂𝑖𝑡𝑖 , 𝒂𝑖 ∈ 𝑨 }
A deformation of 𝑨 in 𝑨 𝑡 is a new bilinear and
associative product ∗: 𝑨 𝑡 × 𝑨 𝑡 ⟶ 𝑨 𝑡
(σ𝑖=0∞ 𝒂𝑖𝑡
𝑖) ∗ (σ𝑖=0∞ 𝒃𝑖𝑡
𝑖) = 𝒂0 ∙ 𝒃0 + 𝒄1𝑡1 + 𝒄2𝑡
2 + 𝒄3𝑡3 +⋯ 𝒄𝑖 ∈ 𝑨
We can deform any algebraic structure on a vector sace 𝑨.
Instead of 𝑨 𝑡 , we can consider a local ring 𝑅 with a
unique maximal ideal 𝔐 with 𝑅/𝔐 ≅ 𝕂.
A deformation of 𝑨 in 𝑨⨂𝑅 is an operation:
∗: 𝑨⨂𝑅 × 𝑨⨂𝑅 ⟶ (𝑨⨂𝑅)
satisfying the same properties of the original such that
we recover the original operation taking quotient by 𝔐
𝑨× 𝑨⟶ 𝑨.
We denote by Def 𝑨, 𝑅 the set of equivalence
clases of deformations of 𝑨 in 𝑨⨂𝑅
“In characteristic 0 every deformation problem
is governed by a differential graded Lie algebra”
There exists a differential graded Lie algebra
𝐿 = 𝐿(𝑨 , 𝑅) such that we have a bijection
Def 𝑨, 𝑅 ≅ 𝑀𝐶(𝐿)/𝒢
Let 𝐿 be a DGL. 𝑎 ∈ 𝐿−1 is a Maurer-Cartan
element if satisfies the equation
𝜕𝑎 = −1
2[ 𝑎 , 𝑎 ]
Two Maurer-Cartan elements 𝑎, 𝑏 ∈ 𝑀𝐶(𝐿) are
gauge-equivalent 𝑎 ∼𝒢 𝑏 if there is an element
𝑥 ∈ 𝐿0 such that
𝑏 = 𝑒ad𝑥 𝑎 −𝑒ad𝑥 𝑎 − id
ad𝑥(𝜕𝑥)
For each 𝑛 ≥ 0 , consider the standard 𝑛-simplex ∆𝑛
∆𝑝𝑛= 𝑖0, … , 𝑖𝑝 0 ≤ 𝑖0 ≤ ⋯ ≤ 𝑖𝑝 ≤ 𝑛 }, if 𝑝 ≤ 𝑛 ,
∆𝑝𝑛= ∅, if 𝑝 > 𝑛.
Let 𝕃 𝑠−1∆𝑛 , 𝑑 be the complete free DGL on the desuspended
rational simplicial chain complex
𝑑𝑎𝑖0,…,𝑖𝑝 =
𝑗=0
𝑝
(−1)𝑗𝑎𝑖0,…,𝑖𝑗,…,𝑖𝑝
where 𝑎𝑖0,…,𝑖𝑝 denotes the generator of degree 𝑝 − 1 represented
by the 𝑝-simplex 𝑖0, … , 𝑖𝑝 ∈ ∆𝑝𝑛.
Sullivan’s question
Problem:
Define a new differential in 𝕃 𝑠−1∆𝑛 such that:
For each 𝑖 = 0,… , 𝑛 the generator 𝑎𝑖 ∈ ∆0𝑛 is
a Maurer-Cartan element.
1.
𝜕𝑎𝑖 = −1
2[𝑎𝑖 , 𝑎𝑖]
2. The linear part 𝜕1 of 𝜕 is precisely 𝑑
Sullivan’s question
Case 𝑛 = 0 𝑎0
𝕃 𝑠−1Δ0 , 𝑑 = 𝕃 𝑎0 , 𝑑
where 𝑑𝑎0 = 0.
The first condition implies:
𝕃 𝑎0 , 𝜕𝑎0 = −1
2[𝑎0, 𝑎0]
Sullivan’s question
Case 𝑛 = 1
𝕃 𝑠−1Δ1 , 𝑑 = 𝕃 𝑎0, 𝑎1, 𝑎01 , 𝑑
where 𝑑𝑎0 = 𝑑𝑎1 = 0.
𝑑𝑎01 = 𝑎1 − 𝑎0.
The first condition implies:
𝜕𝑎0 = −1
2𝑎0, 𝑎0 , 𝜕𝑎1 = −
1
2[𝑎1, 𝑎1]
The second condition implies:
𝜕1𝑎01 = 𝑎1 − 𝑎0.
𝑎0 𝑎01 𝑎1
𝜕2 𝑎01 = 𝜕(𝑎1 − 𝑎0)
= −1
2𝑎0, 𝑎0 +
1
2𝑎1, 𝑎1 ≠ 0
𝜕2 𝑎01 = 𝜕(𝑎1 − 𝑎0 +1
2𝑎01, 𝑎0 +
1
2[𝑎01, 𝑎1])
=1
4𝑎01, 𝑎0 , 𝑎0 −
1
4𝑎01, 𝑎1 , 𝑎1
+1
4[𝑎01, 𝑎1, 𝑎0 ] ≠ 0
𝜕𝑎01 = 𝑎1 − 𝑎0 +𝜆1 𝑎01, 𝑎0 + 𝜇1[𝑎01, 𝑎1]+1
2+1
2
+𝜆2 𝑎01, [𝑎01, 𝑎0] + 𝜇2[𝑎01, 𝑎01, 𝑎1 ]
⋯
Sullivan’s question
Case 𝑛 = 1
𝕃 𝑠−1Δ1 , 𝑑 = 𝕃 𝑎0, 𝑎1, 𝑎01 , 𝑑
where 𝑑𝑎0 = 𝑑𝑎1 = 0.
𝑑𝑎01 = 𝑎1 − 𝑎0.
The first condition implies:
𝜕𝑎0 = −1
2𝑎0, 𝑎0 , 𝜕𝑎1 = −
1
2[𝑎1, 𝑎1]
The second condition implies:
𝜕1𝑎01 = 𝑎1 − 𝑎0.
𝑎0 𝑎01 𝑎1
𝜕𝑎01 = 𝑎01, 𝑎1 +
𝑖=0
∞𝐵𝑖𝑖!ad𝑎01
𝑖 ( 𝑎1 − 𝑎0)
Bernoulli numbers are defined by theseries 𝑥
𝑒𝑥 − 1=
𝑛=0
∞𝐵𝑛𝑛!𝑥𝑛
𝑒𝑥 − 1
𝑥=
𝑛=0
∞1
𝑛 + 1 !𝑥𝑛Since
𝐵0 = 1, 𝐵1 = −1
2, 𝐵2 =
1
6, 𝐵3 = 0, 𝐵4 = −
1
30, 𝐵5 = 0, 𝐵6 =
1
42, ⋯
Sullivan’s question
Sullivan’s question
Case 𝑛 = 2
𝕃 𝑠−1Δ2 , 𝑑 = 𝕃 𝑎0, 𝑎1, 𝑎2, 𝑎01, 𝑎02, 𝑎12, 𝑎012 , 𝑑
𝑑𝑎0 = 𝑑𝑎1 = 𝑑𝑎2 = 0
𝑑𝑎01 = 𝑎1 − 𝑎0
𝑑𝑎02 = 𝑎2 − 𝑎0
𝑑𝑎12 = 𝑎2 − 𝑎1
𝑑𝑎012 = 𝑎12 − 𝑎02 + 𝑎01
𝑎0
𝑎1
𝑎2
𝑎01
𝑎02
𝑎12𝑎012
MC
MC MC
LS
LS
LS
𝜕𝑎012 = 𝑎12 − 𝑎02 + 𝑎01 +Ψ
𝜕𝑎012 = 𝑎12 ∗ 𝑎01 ∗ −𝑎02 − [𝑎012, 𝑎0]
BCH
Sullivan’s question
The Baker-Campbell-Hausdorff formula
Let 𝑥, 𝑦 be two non-commuting variables. 𝑇(𝑥, 𝑦)
The Baker-Campbell-Hausdorff formula 𝑥 ∗ 𝑦 is
the solution to 𝑧 = log(exp 𝑥 exp 𝑦 )
Explicitely 𝑥 ∗ 𝑦 = σ𝑛=0∞ 𝑧𝑛(𝑥, 𝑦)
𝑧𝑛 𝑥, 𝑦 =
𝑘=1
𝑛(−1)𝑘−1
𝑘
𝑥𝑝1𝑦𝑞1⋯𝑥𝑝𝑘𝑦𝑞𝑘
𝑝1! 𝑞1!⋯𝑝𝑘! 𝑞𝑘!
𝑝1 + 𝑞1 > 0; ⋯ ; 𝑝𝑘+𝑞𝑘 > 0. 𝑝1 + 𝑞1 +⋯+ 𝑝𝑘 + 𝑞𝑘 = 𝑛
Sullivan’s question
The Baker-Campbell-Hausdorff formula
The Baker-Campbell-Hausdorff formula satisfies the following properties:
∗ is an associative product: 𝑥 ∗ 𝑦 ∗ 𝑧 = 𝑥 ∗ (𝑦 ∗ 𝑧)
The inverse of 𝑥 is −𝑥, i.e. 𝑥 ∗ −𝑥 = 0.
𝑥 ∗ 𝑦 can be written as a linear combination of
nested commutators
𝑥 ∗ 𝑦 = 𝑥 + 𝑦 +1
2𝑥, 𝑦 +
1
12𝑥, 𝑥, 𝑦 −
1
12𝑦, 𝑥, 𝑦 + ⋯
𝑥 ∗ 𝑦 ∈ 𝕃(𝑥, 𝑦) ⊂ 𝑇(𝑥, 𝑦)
Theorem
𝔏 = { 𝔏𝑛 } 𝑛≥0 is a cosimplicial DGL
U. Buijs, Y. Félix, A. Murillo, D. Tanré. Israel J. of Math. 2019
Definition
< 𝐿 >𝑛= 𝐻𝑜𝑚𝑐𝐷𝐺𝐿( 𝔏𝑛 , 𝐿)
cDGL ⟶< ∙ >
Theorem
𝜋0 < 𝐿 >≅ MC(𝐿)/𝒢
< 𝐿 > ≃ ∐𝑧∈MC(𝐿)/𝒢 < 𝐿𝑧 >
𝜋𝑛 < 𝐿 >≅ 𝐻𝑛−1(𝐿) 𝑛 > 1
𝜋1 < 𝐿 >≅ 𝐻0(𝐿)
For any cDGL 𝐿 we have
1.
2.
𝜋𝑛 < 𝐿 >≅ 𝐻𝑛−1(𝐿) 𝑛 > 1
𝜋1 < 𝐿 >≅ 𝐻0(𝐿)𝜋1 < 𝐿 >× 𝜋𝑛 < 𝐿 > ⟶ 𝜋𝑛 < 𝐿 >
𝜏
≅ ≅
𝐻0 𝐿 × 𝐻𝑛−1(𝐿) 𝐻𝑛−1(𝐿)?
(𝑥 , 𝑧 ) 𝑒ad𝑥(𝑧)
Reduced
Complete
HomcDGL(𝔏∙, 𝐿)
Reduced
Nilpotent, finite-type
Nilpotent, finite-type
Complete𝑁∗𝒰∙𝒢∙ ഥ𝑊(𝐿)
𝒞(𝐿) 𝑆
MC(𝐿⨂Ω∙)Neisendorfer,
Pac. J. M., 1978.Getzler’s
observation
Buijs, Félix, Murillo, Tanré, Preprint 2017
Work in progress