There's also a different way of writing down the H-space structure, that I like for its algebro-geometric flavor. (I'll talk about mathbbCPinfty here, and mathbbRPinfty should be analogous.)
Regarding mathbbCPinfty as a classifying space for complex line bundles, we know that this H-space structure is supposed to implement "tensor product of line bundles". In a (not very explicit) sense this tells us the homotopy class of mathbbCPinftytimesmathbbCPinftytomathbbCPinfty: It represents the line bundle mathcalO(1,1)=p∗1mathcalO(1)otimesp∗2mathcalO(1). We can use this description to write down a much more explicit (and classical) explicit representative.
First, let's recall what the analogous picture looks like for finite projective spaces. The line bundle mathcalO(1,1) determines (upon picking generating sections) the Segre map
mathbbCPntimesmathbbCPmtomathbbCPnm+n+m which takes (in homogeneous coordinates)
([X0:ldots:Xn],[Y0:ldots:Ym])mapsto[X0Y0:ldots:XiYj:ldots:XnYm]
where I'm choosing to be vague on the precise ordering of the coordinates.
(In the end this won't matter up to homotopy, as the maps will become homotopic upon composing with mathbbCPnm+n+mhookrightarrowmathbbCPinfty.)
The analogous formula with infinitely many homogeneous coordinate makes just as much sense, one just has to a good ordering of pairs of non-negative integers. Such an infinite Segre map gives another realization of the H-space structure.
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