algebraic factorization for chain algebras
TRANSCRIPT
Algebraic Factorization for Chain Algebras
Jonathan ScottCleveland State University
Joint work with K. Hess and P.-E. Parent
Operads and Higher Structures in Algebraic Topology andCategory Theory
U Ottawa, August 2 2019
Lifting Functorially
Let C be a category with two classes of morphisms, C and F . Alifting problem with respect to C and F is a commutative square,
A C
B D
f g
where f ∈ C and g ∈ F . A solution to the given lifting problem isa dotted arrow that makes the diagram commute.
I When can the solution be provided in a functorial manner?
I We are interested C = cofibrations, F = acyclic fibrations, inDGA.
Factorization Systems
I Let n be the poset category 1→ 2→ · · · → n.
I If C is any category, then C2 is the category of arrows in Cand commutative squares. Similarly, C3 is the category ofcomposable pairs of morphisms. Composition defines afunctor C3 → C2.
I A factorization system is a section of the composition functor.Composing with the “first arrow” and “second arrow”functors leads to two functors L,R : C2 → C2.
A Gϕ ELϕ
ϕ
Rϕ
The Beginnings of Structure
Given a factorization system (L,R), the (same) diagrams
A A
Gϕ E
Lϕ ϕ
Rϕ
and
A Gϕ
E E
Lϕ
ϕ Rϕ
provide the components of co-unit and unit naturaltransformations,
ε : L⇒ I and η : I ⇒ R
where I is the identity functor on C2.
R-Algebras
An R-algebra is a morphism ϕ along with a structure “morphism”:
Gϕ A
E E
m1
Rϕ m ϕ
m2
that is unital, as expressed in the following diagram.
R-Algebras, continued
A Gϕ A
E E E
ϕ
Lϕ m1
Rϕ ϕ
m2
In particular,
I ϕ is a retract of Rϕ.
I m2 = 1E , so we abuse notation and refer to m by its toparrow.
I m is a retraction of Lϕ.
L-Coalgebras
Dually, an L-coalgebra is a morphism θ with a structure“morphism”,
A A
E Gθ
θ Lθ
c
that is co-unital with respect to εθ, so
I θ is a retract of Lθ;
I c is a section of Rϕ.
A Solution
The lifting problem with respect to L-coalgebras and R-algebrashas a functorial solution. Let θ : A→ B be an L-coalgebra andϕ : C → D be an R-algebra.
A C
Gθ Gϕ
B D
Lθ
θ
Lϕ
ϕ
Rθ
Rϕ
m
c
Putting the “A” in WAF
I Problem: If ϕ is an R-algebra, then Rϕ is not necessarily. Thisis an issue if we want to make this useful for model categories.
I (Riehl 2011) If R is a monad with structure µ : R2 ⇒ R thatis unital w.r.t. η, and L is a comonad with ∆ : L⇒ L2
co-unital w.r.t ε, then “everything works”.
I Every cofibrantly generated model category has a weakalgebraic factorization system for the (cofibration, acyclicfibration) and (acyclic cofibration, fibration) factorizations.
Our Project
Find comonad L : DGA2 → DGA2 and monadR : DGA2 → DGA2 such that
I (L,R) forms a factorization system;
I The cofibrations and acyclic fibrations in DGA are preciselythe L-coalgebras and R-algebras, respectively.
The Factorization
We make use of the obvious mapping-cylinder factorization inDGC and the bar-cobar adjunction.
TheoremLet M be a left-proper model category that satisfies
1. If gf is a fibration, then g is a fibration;
2. there is a functorial cofibrant replacement functor Q on M;
3. there is a functorial (cofibration, acyclic fibration)factorization Q(M2)→M3.
Then the functorial cofibration-acyclic fibration factorizationextends to M2 →M3.
Proof by Diagram
Let ϕ : X → Y . Then Qϕ : QX → QY factors functorially as
QX Nϕ QY .λϕ ρϕ
∼
Form the diagram
QX Nϕ QY
X Gϕ
Y .
λϕ
∼ σ
∼ρϕ
∼Lϕ
ϕ
Rϕ
Our Case
We let Q = ΩB. Let ϕ : A→ E be a morphism in DGA.
I There is a functorial cylinder object, IBA, on BA.
I The mapping cylinder on Bϕ : BA→ BE is given by thepushout
BA BE
IBA MBϕ
Bϕ
i1 jBϕ
`Bϕ
I Set λBϕ = `Bϕi0 : BA→ MBϕ
I ρBϕ : MBϕ → BE such that ρBϕλBϕ = Bϕ obtained bypush-out
I Apply cobar to get the required factorization of ΩBϕ.
The Comultiplication ∆ : L⇒ L2
Let ϕ : A→ E be a morphism of algebras.To construct the component ∆ϕ : L⇒ L2, we must construct anatural lift in the diagram
A GLϕ
Gϕ Gϕ
L2ϕ
Lϕ RLϕ∼∆ϕ
The Construction
We exploit the fact that Gϕ is a pushout.
ΩBA ΩMBLϕ
ΩMBϕ
Gϕ
A GLϕ
ΩλBLϕ
εA
ΩλBϕ
σLϕ
tϕ
σϕ
∆ϕLϕ
L2ϕ
First need tϕ!
Construction of tϕ
We exploit the fact that MBϕ is a pushout – naively.
BGϕ
BA BE MBϕ
IBA MBϕ
MBLϕ
jBLϕ
Bϕ
i1
BLϕ
jBϕ
jBϕ
σ]ϕ
`Bϕ
`BLϕ
?
And we run into trouble – upper cell only commutes up to DGChomotopy.
SHC Homotopies to the Rescue
LemmaThe diagram
BA BE MBϕ
BGϕ
MBLϕ
Bϕ
λBLϕ
jBϕ
σ]ϕ
jBLϕ
commutes up to natural SHC homotopy (i.e., once the cobarconstruction is applied).
The Missing Piece
In the proof of the lemma, we construct a natural DGA homotopy
h : Ω(IBA)→ ΩMBLϕ
from ΩλBLϕ to Ω(jBLϕ σ]ϕ jBϕ Bϕ). Then tϕ is given by thethe pushout,
ΩBA ΩBE
ΩIBA ΩMBϕ
ΩMBLϕ.
ΩBϕ
Ωi1 ΩjBϕ Ω(jBLϕσ]ϕjBϕ)
Ω`Bϕ
h
tϕ
L is a comonad for cofibrations
TheoremWith the above structure, L is a comonad, and the L-coalgebrasare precisely the cofibrations in DGA.
Proof.
I If θ is an L-coalgebra, then it is a retract of Lθ. Since Lθ is acofibration, so too is θ.
I If θ is a cofibration, then since Rθ is an acyclic fibration, canconstruct a lift
· ·
·, ·
Lθ
θ Rϕ∼δ
whose top triangle is an L-coalgebra structure on θ.
The Monad Structure of R
For DGC morphism ϕ : A→ E , again want a natural lift, this timein the diagram
Gϕ Gϕ
GRϕ E
LRϕ Rϕ∼
R2ϕ
µϕ
Exploit the fact that GRϕ is a pushout.
A Little Homological Perturbation
(In progress) There is an EZ-SDR pair of DGAs,
Gϕ E
Rϕ
h
t
From the Perturbation Lemma of Gugenheim-Munkholm, weobtain an SDR pair of DGCs,
BGϕ BE .
BRϕ
H
T
So we have
I BRϕ T = 1BE ,
I H : IBGϕ → BGϕ, H : 1BGϕ ' T BRϕ.
Putting it Together
Putting this data into a pushout diagram,
BGϕ BE
IBGϕ MBRϕ
BGϕ
BRϕ
i1 jBRϕT
`BRϕ
H
S
The Monad Structure
Define µϕ : GRϕ → Gϕ as the unique morphism that makes thepushout diagram of chain algebras,
ΩBGϕ ΩMBRϕ
Gϕ GRϕ
Gϕ
ΩλBRϕ
εGϕ σRϕS]
LRϕ
µϕ
commute.
Extending to Algebras over Koszul Operads
I Suppose we have an operad P (in chain complexes), acooperad Q, and a Koszul twisting cochain τ : Q → P.
I There are associated bar and cobar constructions that providea cofibrant replacement comonad.
I Need a homological perturbation machine. Berglund (2009)might be a good place to start.