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L-theory

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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 very important in surgery theory.

[edit] Definition

One can define L-groups for any ring with involution R: the quadratic L-groups L * (R) (Wall) and the symmetric L-groups L * (R) (Mishchenko, Ranicki).

The even dimensional L-groups L2k(R) are defined as the Witt groups of ε-quadratic forms over the ring R with ε = ( − 1)k. More precisely, L2k(R) is the abelian group of equivalence classes [ψ] of non-degenerate ε-quadratic forms \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: [\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 L2k(R) is defined by [\psi_1] + [\psi_2] := [\psi_1 \oplus \psi_2]. The zero element is represented by H_{(-1)^k}(R)^n for any n \in {\mathbb N}_0. The inverse of [ψ] is [ − ψ].

More details and the definition of the odd dimensional L-groups can be found in the references mentioned below.

[edit] Examples and Applications

The L-groups of a group π are the L-groups L_*(\mathbf{Z}[\pi]) of the group ring \mathbf{Z}[\pi]. In the applications to topology π is the fundamental group π1(X) of a space X. The quadratic L-groups L_*(\mathbf{Z}[\pi]) play a central role in the surgery classification of the homotopy types of n-dimensional manifolds of dimension n > 4, and in the formulation of the Novikov conjecture.

The simply connected L-groups are also the L-groups of the integers: L(e) := L(\mathbf{Z}[e]) = L(\mathbf{Z}) with L = L * or L * . For quadratic L-groups, these are the surgery obstructions to simply connected surgery.

The distinction between symmetric L-groups and quadratic L-groups, indicated by upper and lower indices, reflects the usage in group homology and cohomology. The group cohomology H * of the cyclic group \mathbf{Z}_2 deals with the fixed points of a \mathbf{Z}_2-action, while the group homology H * deals with the orbits of a \mathbf{Z}_2-action.

The quadratic L-groups: Ln(R) and the symmetric L-groups: Ln(R) are related by a symmetrization map L_n(R) \to L^n(R) which is an isomorphism modulo 2-torsion, and which corresponds to the polarization identities.

The quadratic L-groups are 4-fold periodic. The quadratic L-groups of the integers are:

\begin{align}
L_{4k}(\mathbf{Z}) &= \mathbf{Z}   && \mbox{signature/8}\\
L_{4k+1}(\mathbf{Z}) &= 0\\
L_{4k+2}(\mathbf{Z}) &= \mathbf{Z}/2 && \mbox{Arf invariant}\\
L_{4k+3}(\mathbf{Z}) &= 0.
\end{align}

Symmetric L-groups are not 4-periodic in general (see Ranicki, page 12), though they are for the integers. The symmetric L-groups of the integers are:

\begin{align}
L^{4k}(\mathbf{Z}) &= \mathbf{Z} && \mbox{signature}\\
L^{4k+1}(\mathbf{Z}) &= \mathbf{Z}/2 && \mbox{deRham invariant}\\
L^{4k+2}(\mathbf{Z}) &= 0\\
L^{4k+3}(\mathbf{Z}) &= 0.
\end{align}

In view of the applications to the classification of manifolds there are extensive calculations of the quadratic L-groups L_*(\mathbf{Z}[\pi]). For finite π algebraic methods are used, and mostly geometric methods (e.g. controlled topology) are used for infinite π.


More generally, one can define L-groups for any additive category with a chain duality, as in Ranicki (section 1).

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