Delooping of the K-theory of strictly derivable Waldhausen categories
Satoshi Mochizuki
Introduction
In this short note, for a morphism of Waldhausen categories f : A = (A ,wA) → B = (B,wB), we will define Cone f to be a Waldhausen category. There exists the canonical morphism of Waldhausen categories κ f : B → f κ f Cone f (see Definition 2.5). We will show that the sequence A → B → Cone f induces fibration sequence of K( f ) K(κ f ) spaces K(A) → K(B) → K(Cone f ) on connective K-theory (see Theorem 2.7). Moreover we will define a notion of strictly derivable Waldhausen categories (see Definition 1.6) and define non-connective K-theory for strictly derivable Waldhausen categories (see Definition 3.12).
1 Admissible classes of morphisms and w-thick subcategories
In this section, let C be a category with cofibrations. We fix a zero object 0 of C .
Definition 1.1 (Admissible class of morphisms). We say that a class w of morphisms in C is admissible if w satisfies the following three conditions. (Closed under isomorphisms). w contains all isomorphisms.
(Two out of three property for compositions). w satisfies the two out of three property. Namely for a f g pair of composable morphisms x → y → z, if two of g f , f and g are in w, then the third one is also in w. (Two out of three property for cofibration sequences). In the commutative diagram of cofibration sequences below j q x / / y / / y/x (1)
a b c arXiv:1803.07254v2 [math.KT] 6 Aug 2020 x0 / / y0 / / y0/x0, j0 q0
if two of a, b and c are in w, then the third one is also in w.
Lemma 1.2. Assume that C is enriched over the category of abelian groups. If w is an admissible class of morphisms in C , then w satisfies the gluing axiom of [Wal85]. In particular the pair (C ,w) is a category with cofibrations and weak equivalences.
Proof. Since C is close under finite coproducts, C is an additive category. In the commutative diagram below, assume that a, b and c are in w. y o x / / z
b a c y0 o x0 / / z0.
1 Then there are commutative diagrams of cofibrations sequences.
y / / y ⊕ z / / z x / / y ⊕ z / / y tx z
b 0 b c a 0 bt c b 0 c 0 c a 0 0 0 0 0 0 0 0 0 y / / y ⊕ z / / z , x / / y ⊕ z / / y tx0 z .