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<record version="1" id="502">
 <title>test ocr</title>
 <name>TestOcr</name>
 <created>2009-02-07 00:04:11</created>
 <modified>2009-02-07 00:04:11</modified>
 <type>Definition</type>
 <creator id="1" name="bloftin"/>
 <modifier id="1" name="bloftin"/>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="msc" code="00."/>
 </classification>
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 <content>The operation $v/c$ is bilinear, and it is easy to verify that
$$
(7.2)\text{ }\quad \delta v/c=v/\partial c+(-1)^{\mathfrak{i}}\delta(v/c).
$$
\quad Assume now that $v$ is an equivariant cochain; for ow $\epsilon\pi$ we have $\alpha c=\alpha\Sigma n_{J}e_{f}=\Sigma(\alpha n_{j})(\alpha e_{j})$, then
$$
(v/\alpha c)\cdot\sigma=\Sigma(\alpha n_{j})v\cdot(\alpha e_{f})\otimes\sigma=\Sigma(\alpha n_{j})\alpha v\cdot(e_{j}\otimes\sigma)
$$
$$
=\alpha^{2}\Sigma n_{j}v\cdot(e_{f}\otimes\sigma)=(v/c)\cdot\sigma.
$$
Thus, in this case,

\noindent
(7.3) $v/\alpha c=v/c$ and $v/(\alpha c-c)=0$.

\noindent
Consequently, the definition of $v/c$ extends to the case of $v$, an equi- variant cochain, and $c$ an element of $[C_{i}(W;Z_{m}^{\langle q)})]_{\pi}\approx C_{i}(Z_{m}^{(q)}\otimes_{\pi}W)$;the relation (7.2) holds for this extended operation.

\quad Now take $v=\emptyset^{\#}u^{n}$ and $c\epsilon C_{i}(Z_{m}^{1q)}\otimes_{\pi}W)$, then
$$
\phi\# u^{n}fc\epsilon C^{nq-i}(K;Z_{m})
$$
is defined as the reduction by $c$ of the $n^{\mathrm{t}\mathrm{h}}$ power of $u$. Suppose that $u$ is a cocycle, then $\phi\# u^{n}$ is an equivariant cocycle, and if $c$ is a cycle, it follows from (7.2) that $\phi\# u^{n}/c$ is a cocycle. Moreover, if the cycle $c$ is varied by a boundary, then (7.2) implies that $\phi\# u^{n}/c$ varies by a co- boundary. If $u$ is varied by a coboundary $\phi\# u^{n}/c$ also varies by a coboundary. We only remark here that the proof of this last fact requires a special argument and is not, as in the preceding case, an immediate consequence of (7.2). Thus the class $\{\phi\# u^{n}/c\}$ is a function of the classes $\{u\}, \{c\}$, and it is independent of the particular $\phi_{\#}$, since by (3.1) any two choices of $\phi_{\#}$ are equivariantly homotopic. Then Steenrod defines $\{u\}^{n}/\{c\}$, the reduction by $\{c\}$ of the $n^{\mathrm{t}\mathrm{h}}$ power of $\{u\}$, by
$$
\{u\}^{n}/\{c\}=\{\phi\# u^{n}/c\}.
$$
This gives the Steenrod reduced power operations; they are operations defined for $u\epsilon H^{q}(K;Z_{m})$ and $c\epsilon H_{i}(\pi;Z_{m}^{\langle q)})$, and the value is
$$
u^{n}/c\epsilon H^{nq-i}(K;Z_{m}).
$$
\quad In general, the reduced powers $u^{n}/c$ are linear operations in $c$, but may not be linear in $u$. We will list some of their $\mathrm{p}\mathrm{r}\mathrm{o}\varphi$ rties. Unless otherwise stated, we assume $u$ and $c$ as above.

\quad First, we have

(7.4) $u^{n}/c=0$ if $i&gt;nq-q$.

\quad Let $f:K\rightarrow L$ be a map and $f^{*}: H^{q}(L;Z_{m})\rightarrow H^{q}(K;Z_{m})$, the induced homomorphism; then
$$
(7.5)\text{ }\quad f^{*}(u^{n}/c)=(f^{*}u)^{n}/c.
$$
This result implies topological invariance for reduced powers</content>
</record>
