In mathematics, algebraic L-theory is the K-theory of quadratic forms; the term was coined by C. T. C. Wall, with L being used as the letter after K. Algebraic L-theory, also known as "Hermitian K-theory", is important in surgery theory.
Definition One can define L-groups for any ring with involution R: the quadratic L-groups L ∗ ( R ) {\displaystyle L_{*}(R)} (Wall) and the symmetric L-groups L ∗ ( R ) {\displaystyle L^{*}(R)} (Mishchenko, Ranicki).
Even dimension The even-dimensional L-groups L 2 k ( R ) {\displaystyle L_{2k}(R)} are defined as the Witt groups of ε-quadratic forms over the ring R with ϵ = ( − 1 ) k {\displaystyle \epsilon =(-1)^{k}} . More precisely,
L 2 k ( R ) {\displaystyle L_{2k}(R)}
is the abelian group of equivalence classes [ ψ ] {\displaystyle [\psi ]} of non-degenerate ε-quadratic forms ψ ∈ Q ϵ ( F ) {\displaystyle \psi \in Q_{\epsilon }(F)} over R, where the underlying R-modules F are finitely generated free. The equivalence relation is given by stabilization with respect to hyperbolic ε-quadratic forms:
[ ψ ] = [ ψ ′ ] ⟺ n , n ′ ∈ N 0 : ψ ⊕ H ( − 1 ) k ( R ) n ≅ ψ ′ ⊕ H ( − 1 ) k ( R ) n ′ {\displaystyle [\psi ]=[\psi ']\Longleftrightarrow n,n'\in {\mathbb {N} }_{0}:\psi \oplus H_{(-1)^{k}}(R)^{n}\cong \psi '\oplus H_{(-1)^{k}}(R)^{n'}} . The addition in L 2 k ( R ) {\displaystyle L_{2k}(R)} is defined by
[ ψ 1 ] + [ ψ 2 ] := [ ψ 1 ⊕ ψ 2 ] . {\displaystyle [\psi _{1}]+[\psi _{2}]:=[\psi _{1}\oplus \psi _{2}].}
The zero element is represented by H ( − 1 ) k ( R ) n {\displaystyle H_{(-1)^{k}}(R)^{n}} for any n ∈ N 0 {\displaystyle n\in {\mathbb {N} }_{0}} . The inverse of [ ψ ] {\displaystyle [\psi ]} is [ − ψ ] {\displaystyle [-\psi ]} .
Odd dimension Defining odd-dimensional L-groups is more complicated; further details and the definition of the odd-dimensional L-groups can be found in the references mentioned below.
Examples and applications The L-groups of a group π {\displaystyle \pi } are the L-groups L ∗ ( Z [ π ] ) {\displaystyle L_{*}(\mathbf {Z} [\pi ])} of the group ring Z [ π ] {\displaystyle \mathbf {Z} [\pi ]} . In the applications to topology π {\displaystyle \pi } is the fundamental group
π 1 ( X ) {\displaystyle \pi _{1}(X)} of a space X {\displaystyle X} . The quadratic L-groups L ∗ ( Z [ π ] ) {\displaystyle L_{*}(\mathbf {Z} [\pi ])}
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