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.[1]
One can define L-groups for any ring with involution R: the quadratic L-groups
L*(R)
L*(R)
The even-dimensional L-groups
L2k(R)
\epsilon=(-1)k
L2k(R)
is the abelian group of equivalence classes
[\psi]
\psi\inQ\epsilon(F)
[\psi]=[\psi']\Longleftrightarrown,n'\in{N}0:\psi ⊕
H | |
(-1)k |
(R)n\cong\psi' ⊕
H | |
(-1)k |
(R)n'
The addition in
L2k(R)
[\psi1]+[\psi2]:=[\psi1 ⊕ \psi2].
The zero element is represented by
H | |
(-1)k |
(R)n
n\in{N}0
[\psi]
[-\psi]
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.
The L-groups of a group
\pi
L*(Z[\pi])
Z[\pi]
\pi
\pi1(X)
X
L*(Z[\pi])
n
n>4
H*
Z2
Z2
H*
Z2
XG
XG=X/G
The quadratic L-groups:
Ln(R)
Ln(R)
Ln(R)\toLn(R)
The quadratic and the symmetric L-groups are 4-fold periodic (the comment of Ranicki, page 12, on the non-periodicity of the symmetric L-groups refers to another type of L-groups, defined using "short complexes").
In view of the applications to the classification of manifolds there are extensive calculations ofthe quadratic
L
L*(Z[\pi])
\pi
\pi
More generally, one can define L-groups for any additive category with a chain duality, as in Ranicki (section 1).
The simply connected L-groups are also the L-groups of the integers, as
L(e):=L(Z[e])=L(Z)
L
L*
L*.
The quadratic L-groups of the integers are:
\begin{align} L4k(Z)&=Z&&signature/8\\ L4k+1(Z)&=0\\ L4k+2(Z)&=Z/2&&Arfinvariant\\ L4k+3(Z)&=0. \end{align}
The symmetric L-groups of the integers are:
\begin{align} L4k(Z)&=Z&&signature\\ L4k+1(Z)&=Z/2&&deRhaminvariant\\ L4k+2(Z)&=0\\ L4k+3(Z)&=0. \end{align}