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An invariant central character of the quaternion group with no linear extension

Counterexample

The nontrivial character θ of the centre Z(Q8)={±1} of the quaternion group, θ(−1)=−1, is invariant under Q8 but has no linear extension to Q8: every linear character of Q8 takes the value 1 at −1, since −1=[i,j] lies in the commutator subgroup. Thus invariance of a normal type does not by itself make the type extendible, which is why the little group method needs the split hypothesis or the projective correction.

Facts & Assumptions

Given: The quaternion group Q8={±1,±i,±j,±k} of The quaternion group Q8={±1,±i,±j,±k} inside the nonzero quaternions and the character θ of Z(Q8)={±1} with θ(1)=1, θ(−1)=−1.

[F1]

Q8 has i2=j2=k2=−1, ij=k, ji=−k and k=ij; the element −1 is central. (The quaternion group Q8={±1,±i,±j,±k} inside the nonzero quaternions).

[F2]

A character of a normal subgroup N⊴G is invariant when gθ=θ for all g∈G, where gθ(n)=θ(g−1ng), and then the inertia group is G. (Inertia group and characters lying above a normal type).

[F3]

An extension of θ to a subgroup H with N≤H≤G is a representation ρ~:H→GL⁡(S) on the space S affording θ with ρ~∣N=ρ; at character level, an extension of θ is a character θ~ with Res⁡NHθ~=θ. (An extension of a normal subgroup representation).

[F4]

An invariant irreducible representation extends to its inertia group if and only if its Clifford obstruction class is zero. (An invariant irreducible representation extends to its inertia group exactly when the Clifford obstruction vanishes).

[F5]

The faithful two-dimensional representation of Q8 gives a projective representation of Q8/{±1}≅C2×C2 whose factor set takes the values α(y,x)=−1≠1=α(x,y) and is not a coboundary, so that H2(Q8/{±1},C×) contains a nonzero class. (The quaternion group as a cocycle central extension of C2 x C2).

[A1]

A linear extension of the one-dimensional character θ is a group homomorphism λ:Q8→C× with λ(−1)=θ(−1)=−1, since a one-dimensional representation is a homomorphism and its character is itself.

Verification

technique · counterexample
1.1

The centre of Q8 is Z(Q8)={±1}: the element −1 is central by [F1], while i, j and k are not central because ij=k and ji=−k≠k, together with their cyclic analogues; since every element of Q8 is one of ±1,±i,±j,±k by [F1], these are all the central elements.

F1givenalgebra
1.2

Every linear character λ:Q8→C× satisfies λ(−1)=1: from the relations of [F1], iji−1j−1=(ij)(ji)−1=k⋅(−k)−1=k⋅k=k2=−1, so −1 is a commutator, and multiplicativity gives λ(iji−1j−1)=λ(i)λ(j)λ(i)−1λ(j)−1=1.

F1givenalgebra
2.1

The prescription θ(1)=1, θ(−1)=−1 defines a linear character of Z(Q8): products involving 1 satisfy θ(1z)=θ(z1)=θ(z)=θ(1)θ(z), and the remaining product satisfies θ((−1)(−1))=θ(1)=1=(−1)2=θ(−1)θ(−1). These are all four pairs in Z(Q8)×Z(Q8), so the map is multiplicative. It acts on the nonzero one-dimensional space C, which has no nonzero proper subspace, hence is irreducible.

F1step 1.1given
3.1

The character θ is Q8-invariant: for g∈Q8 and z∈Z(Q8) one has gθ(z)=θ(g−1zg)=θ(z) because z is central, so gθ=θ for every g and the inertia group of θ is all of Q8 by [F2].

F2step 1.1step 2.1
4.1

Therefore θ is invariant but does not extend to a linear character of Q8: a linear extension would be a homomorphism λ:Q8→C× with λ∣Z(Q8)=θ by [F3] and [A1], in particular λ(−1)=θ(−1)=−1, whereas step 1.2 forces λ(−1)=1 for every linear character. Hence no extension of θ to Q8 exists, and the invariance established in step 3.1 is not sufficient for extendibility.

A1F3step 3.1step 1.2algebra
5.1

By [F4] the failure of extension recorded in step 4.1 is exactly the statement that the Clifford obstruction class of θ in H2(Q8/{±1},C×) is nonzero; this is a genuine obstruction, since [F5] exhibits a nonzero class in that same cohomology group, and it shows that the invariance hypothesis alone cannot replace the split hypothesis of the little group method. The character θ is the central character of the faithful two-dimensional representation of Q8, so the example is exactly the nonsplit counterpart of the extendible invariant types.

F4F5step 4.1∎

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