Steenrod operations are an example of what's known as a power operation. Power operations result from the fact that cup product is "commutative, but not too commutative". The operations come from a "refinement" of the operation of taking pth powers (squares if p=2), whose construction rests on this funny version of commutativity.
A cohomology class on X amounts to a map a:XtoR, where R=prodngeq0K(F2,n). So the cup product of a and b is given by
XtimesXtoRtimesRxrightarrowmuR.
In other words, the space R carries a product, which encodes cup product. (There is another product on R which encodes addition of cohomology classes.)
You might expect, since cup product is associative and commutative, that if you take the nth power of a cohomology class, you get a cohomology class on the quotient Xn/Sigman, where Sigman is the symmetric group, i.e.,
XnxrightarrowanRnrightarrowR
should factor through the quotient Xn/Sigman. This isn't quite right, because cup product is really only commutative up to infinitely many homotopies (i.e., it is an "E-infinity structure" on R). This means there is a contractible space E(n) with a free action of Sigman, and a product map:
mu′n:E(n)timesRntoR
which is Sigman invariant, so it factors through (E(n)timesRn)/Sigman. Thus, given a:XtoR, you get
P′(a):(E(n)timesXn)/Sigmanto(E(n)timesRn)/SigmantoR.
If you restrict to the diagonal copy of X in Xn, you get a map
P(a):E(n)/SigmantimesXtoR.
If n=2, then E(2)/Sigma2 is what Hatcher seems to call Linfty; it is the infinite real proj. space RPinfty. So P(a) represents an element
in H∗RPinftytimesXapproxH∗X[x]; the coefficients of this polynomial in x are the Steenrod operations on a.
Other cohomology theories have power operations (for K-theory, these are the Adams operations).
You can also describe the steenrod squares directly on the chain level: the account in the book by Steenrod and Epstein is the best place to find the chain level description.
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