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Local Spin lift from the matrix logarithm

Statement

Let (V,B) be a finite-dimensional nondegenerate real quadratic space, let J=diag⁡(ϵ1,…,ϵn) be its matrix in an orthogonal anisotropic basis with ϵi=Q(ei)∈{1,−1}, and let SO(V,B) have the subspace topology from matrices. There is a neighborhood U of the identity in SO(V,B) and a continuous map s:U→Spin⁡N=1(V,Q) with s(I)=1 and ρ(s(A))=A.

Facts & Assumptions

Given: The Clifford relation, group conventions, and PBW theorem cited below.

[F1]

eiej+ejei=2B(ei,ej)1 and ei2=Q(ei)1 (Universal Clifford algebra of a quadratic space, Polarized relations in a Clifford algebra).

[F2]

The orthogonal square-free monomials form a basis; in particular the bivectors eiej are linearly independent (PBW basis and exterior associated graded for a Clifford algebra).

[F3]

α, reversion, Clifford conjugation and N(x)=xxˉ have the conventions used here (Clifford involutions and the norm of a vector product).

[F4]

Γ, ρ, and Spin⁡N=1 are defined as in Real Clifford group, Pin, and the two Spin subgroups, and the norm-one product characterization is in Normalized Pin products and Clifford norm.

Proof

technique · direct
1.1givenconstructalgebra

If n=0, set U={I0}, L=0, and s(I0)=1; this is a continuous section with norm one. For n>0, choose a submultiplicative matrix norm and shrink a neighborhood U of I in SO(V,B) until ∥A−I∥, ∥AT−I∥, and ∥A−1−I∥ are all less than 1. Then the series L=log⁡A=∑m≥1(−1)m+1(A−I)m/m and the corresponding series for AT and A−1 converge absolutely and continuously. The scalar power-series identities, by absolute Cauchy products, give exp⁡L=A, log⁡(AT)=LT, and log⁡(A−1)=−L. From ATJA=J one gets JAJ=A−T, so conjugating the logarithm series gives JLJ=−LT, equivalently LTJ+JL=0.

2.1F1F2step 1.1algebra

For i<j, direct use of [F1] gives [eiej,ek]=2(B(ej,ek)ei−B(ei,ek)ej). The n(n−1)/2 bivectors therefore map under b↦ad⁡b∣V to a basis of the matrices L satisfying LTJ+JL=0: each coefficient cij independently gives entries Lij=2cijϵj and Lji=−2cijϵi. Thus there is a unique bivector b(L)=∑i<jcijeiej with [b(L),v]=Lv for every v∈V, and it depends linearly and continuously on L.

3.1F3F4step 2.1construct

Set s(A)=exp⁡(b(L)) in the finite-dimensional Clifford algebra. Since b(L) is even, α(s(A))=s(A). The convergent commutator series gives s(A)vs(A)−1=exp⁡(ad⁡b(L))(v)=exp⁡(L)v=Av, so s(A)∈Γ and ρ(s(A))=A.

4.1F3F4step 3.1algebra∎

Reversion negates each bivector, hence Clifford conjugation sends b(L) to −b(L) and exp⁡(b(L))‾=exp⁡(−b(L)). Therefore N(s(A))=exp⁡(b(L))exp⁡(−b(L))=1. By [F4], s(A)∈Spin⁡N=1. Continuity of matrix logarithm on U, of b(L), and of the finite-dimensional algebra exponential proves continuity of s, with s(I)=1.

Remarks

This explicit local section proves the infinitesimal-to-local group lift needed for a topological covering; the abstract exact sequence alone would not do so.

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