$\DeclareMathOperator\MSO{MSO}\DeclareMathOperator\MSpin{MSpin}\DeclareMathOperator\SO{SO}\DeclareMathOperator\BSO{BSO}\DeclareMathOperator\BG{BG}\DeclareMathOperator\BO{BO}\DeclareMathOperator\MG{MG}\DeclareMathOperator\Spin{Spin}\MG(d)$ is the Thom space of the pullback of the vector bundle $V_d$ over $\BO(d)$ along the map $\BG(d) \to \BO(d)$. The colimit of $\Sigma^{-d}\MG(d)$ is $\MG$. The $\MG$ is the Thom spectrum of $G$.
It is known that $M(\Spin\times \SO(d))= \MSpin \wedge \BSO(d)_+$, where $\BSO(d)_+$ is a disjoint union of $\BSO(d)$ with a point.
My question is: What is the Thom spectrum of $(\Spin\times_{Z_2} \SO(d))$?
The hope is to break down the spectrum to familiar one of $\MSpin$. the smash product $\wedge$, the suspension $\Sigma^{-n}$, and perhaps the Thom spectrum $\MSO(d)$.
For $d=4$, $M(\Spin\times_{Z_2}\SO(4))=\MSpin\wedge\Sigma^{-3}\MSO(3)\wedge\Sigma^{-3}\MSO(3)$, which breaks down to the familiar spectra.
For $d=6$, $M(\Spin\times_{Z_2}\SO(6))$, could we do the similar break down?
For $d=8$, $M(\Spin\times_{Z_2}\SO(8))$, could we do the similar break down?
Note that $\SO(6)=\Spin(6)/Z_2=\operatorname{PSU}(4)$. $\SO(8)=\Spin(8)/Z_2$.
EDIT: The $d$ is even for $\SO(d)$ here. Also the modded out $Z_2$ is shared between the identified normal of Spin and SO groups.
- Spin is the tangent structure (tangent spin bundle) of any dimensions of any base Spin-manifold.
- $\SO(d)$ is the principal SO structure and principal SO-bundle.