2 GABRIEL C. DRUMMOND-COLE
From this convention, you view this as a dg algebra, and the graded Leibniz rule
crmes from our convention,
d(a ⋅ a
′
) = µ [(d ⊗ id
A
+ id
A
⊗ d
A
)(a ⊗ a
′
)] = da ⋅ a
′
+ (−1)
∣a∣
a ⋅ da
′
The most important example, let A be a k-linear Abelian category. Then C(A)
the category of chain complexes in A. Then this can be made into a dg category as
follows. The objects and composition are the same as in C(A) and the morphisms
for chain complexes C and D, the gradings are Hom
Cdg
(C, D) =
p
Hom
Cdg
(C, D)
p
where Hom
Cdg
(C, D)
p
is
∏
i
Hom
A
(C
i
, D
i+p
).
Now I have to define the differential, so d
p
takes f
i
to d
i+p
D
○f
i
+(−1)
p+1
f
i+1
○d
i
C
.
So if I draw one piece this looks like
C
i
d
C
//
f
i
C
i+1
f
i+1
D
i
d
D
//
D
i+1
so that d measures the failure of commutativity of this diagram.
That’s the primary example of a dg category. You can take Z
0
, objects are the
same as in Cdg(A). The morphisms are the kernel, they’re the kernel of d
0
. Then
H
0
(Cdg(A)) has the same objects, and the morphisms are ker d
0
/imd
0
, which are
chain maps modulo homotopy.
For a later purpose you want the opposite category, if A is a dg category with
d and ○ then the opposite category A
op
consists of the following data, the objects
are the same as in A and the morphisms are opposite; the differential d
op
(X, Y ) =
d(Y, X) and the composition g ○
op
f is defined as (−1)
∣g ∣∣f ∣
f ○ g.
Now let me introduce A
∞
categories, which is a cousin of a dg category.
Definition 1.2. A (unital) A
∞
category A consists of objects, and morphisms
Hom
A
(X, Y ) a Z or Z/2-graded kmodule and it comes with a composition, structure
maps m
d
which goes
Hom
A
(X
0
, X
1
) ⊗ ⋯ ⊗ Hom
A
(X
d−1
, X
d
) → Hom
A
(X
0
⊗ X
d
)
which is a multi-k-linear map of degree 2 − d satisfying the relations
k
1
+k
2
=k+1
(−1)
∣x
1
∣+⋯+∣x
i−1
∣+i−1
m
k
1
(x
1
, . . . , mk
2
(x
i
, . . . , x
i+k−1
), ⋯, x
k
) = 0.
How do these start? The first few are m
1
○m
1
= 0 and m
1
(m
2
(x
0
, x
1
))+m
2
(m
1
(x
0
), x
1
)+
(−1)
∣x
0
∣+1
m
2
(x
0
, m
1
(x
1
)) = 0.
Then there is the unit, which is that m
k
(⋯, e
x
, ⋯, 0) is zero, and that m
2
(e, x) =
x = (−1)
∣x∣
m
2
(x, e).
Some remarks, in general this is not a category. If m
k
= 0 for k ≥ 3 this is a dg
category.
Let me finish my talk by saing why these come into play in the ∞ category
setting. We want to measure some A
∞
algebra from the algebro-geometric side.
To that purpose, we should enlarge the A
∞
category. We have structures in
algebraic geometry, ⊕, [1], ⊗, cone.
So what do we do? We think about the Yoneda embedding.