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In order to prove that Form 221 is false we shall give a proof that
in \(\cal N51\) there is no non-principal measure on \(A\), the set of atoms.
Suppose, \(m\) is a non-principal measure on \(A\) supported by the
partition \(P =(B_1, \ldots, B_n)\) of \(A\). Since
\(m\) is finitely additive on disjoint sets, \(m(A)=1\), and \(m(\{a\})
=0\), for all \(a\in A\). It follows that there must be an \(i \le n\)
such that \(B_i\) is infinite and
\(m(B_i)\ne 0\). There exist pairwise disjoint
infinite subsets, \(S_1\), \(S_2\), and \(S_3\), of \(B_i\) such that
\(B_i=S_1\cup S_2\cup S_3\). Suppose \(\sigma_1, \sigma_2\in G_P\) are
such that
\begin{align}
\sigma_1(S_1)= S_2\cup S_3\hbox{ and } \sigma(S_2\cup S_3)=S_1 \tag{1}\\
\sigma_2(S_1)=S_2,\ \sigma_2(S_2)=S_3,\hbox{ and }\sigma_2(S_3)=S_1 \tag{2}\\
\end{align}
Then, we would have
(a) \(m(S_1) = m(S_2\cup S_3) = m(S_2) + m(S_3)\), by (1).
(b) \(m(S_1) = m(S_2) = m(S_3)\), by (2).
Consequently, \(m(S_1) = 2m(S_1)\), which implies that \(m(S_1)=0\).
Thus, by b., \(m(B_i)=0\), which is a contradiction.
In order to prove that Form 90 and Form 64 are true, we need the following
lemma which is a slight strengthening of Form 314 (from
Degen [1988]). The proof requires the axiom of choice but we intend to
use the lemma in the ground model where \(AC\) holds.
(i) \(\psi = \rho_2\circ\rho_1\) and
(ii) For all \(B\subseteq A\), if \(\psi(B) = B\) then \(\rho_1(B) = B\) and \(\rho_2(B) = B\).
If every element of \(X\) has support \(P\) then \(X\) is well orderable
in \(\cal N51\) and the proof is easy. We therefore assume that
\(y\in X\) and there is a \(\phi\in G_P\) such that \(\phi(y) \ne y\).
Step 1. We show that we may assume that \(y\) has a support
\[
Q = (C_1,C_2,C_3,\ldots,C_{n_0},C_{n_0+1},\ldots,C_n)
\]
where
a. \(n_0\ge 3\) and \(C_3\) is infinite.
b. For \(1\le j\le n_0\), \(C_j \subseteq B_1\) and for \(n_0 < j\le n\), \(C_j \cap B_1 = \emptyset\).
c. \(\phi(C_1) = C_2\), \(\phi(C_2) = C_1\), and for every \(a\in A - (C_1\cup C_2)\), \(\phi(a) = a\).
First, we may assume (by refining \(P\) if necessary) that each \(B_i\)
is either infinite or a singleton. Secondly, by writing
\(\phi = \prod_{i=1}^k \phi_i\) where \(\phi_i(a) = a\) for \(a\in A-B_i\)
and replacing \(\phi\) by one of the \(\phi_i\), we may assume that
there is an \(i \le k\) such that \(\phi(a) = a\) for \(a\in A - B_i\).
(If \(\prod_{i=1}^k \phi_i(y) \ne y\) then for some \(i\), \(\phi_i(y)
\ne y\).) Further it is no loss of generality to assume that \(i = 1\).
Let \(Q = (C_1,\ldots,C_n)\) be a support of \(y\). By replacing
each \(C_j\) with the two sets \(C_j\cap B_1\) and \(C_j - B_1\) (if
necessary) and reordering the \(C_j\)'s we may assume that
there is an \(n_0\le n\) such that
\(C_j \subseteq B_1\) for \(j\le n_0\) and \(C_j \cap B_1 = \emptyset\)
for \(j > n_0\). As in the proof of the previous theorem (using the
lemma) we may assume that \(\phi\) is a reflection. By replacing
\(Q\) by a partition whose cells are
\(\{C_i \cap \phi(C_j) : 1\le i,j\le n\} - \{\emptyset\}\) we may
assume (since \(\phi\) is a reflection) that
\(\forall i\), \(1\le i\le n\), \(\exists j\), \(1\le j\le n\) such that
\(\phi(C_i) = C_j\) and \(\phi(C_j) = C_i\). (By our simplifying
assumptions so far, \(\phi(C_j) = C_j\) for \(j > n_0\).)
By decomposing \(\phi\) into a product \(\phi = \prod_{r=1}^m \gamma_r\)
where for each \(r\), \(1\le r\le m\) there are \(i\) and \(j\) such that
\(\gamma_r(a) =a\) for \(a\in A - (C_i\cup C_j)\), \(\gamma_r(C_i) = C_j\)
and \(\gamma)r(C_j) = C_i\) and replacing \(\phi\) by one of the
\(\gamma_r\), we may assume that \(\phi(a) = a\) for \(a\in A - (C_i\cup C_j)\),
\(\phi(C_i) = C_j\) and \(\phi(C_j) = C_i\). It is no loss of generality
to assume that \(i = 1\) and \(j = 2\).
Finally, we may assume that for some \(i\), \(3\le i\le n_0\), \(C_i\) is
infinite. Assuming that this is not the case and using the facts
that \(C_1 \cup C_2 \subseteq B_1\) and that \(B_1\) is infinite we
conclude that \(C_1\) and \(C_2\) are infinite. Let \(C'\) be any infinite
subset of \(C_1\) whose complement in \(C_1\) is infinite. Note that
\(C_2\) is the disjoint union \(C_2 = \phi(C')\cup \phi(C_1 - C')\).
Therefore, \(Q' = (C',\phi(C'),C_1 -C',\phi(C_1 -C'), C_3,\ldots,C_n)\)
is a partition of \(Q\) which supports \(y\). Define \(\phi'\) and \(\phi''\)
(both in \(G_P\)) as follows:
\[
\phi'(a) = \begin{cases}
\phi(a) & a\in C'\cup \phi(C')\\
a & \hbox{otherwise}
\end{cases}
\]
and
\[
\phi''(a) = \begin{cases}
\phi(a) & a\in (C_1 - C')\cup \phi(C_1 - C')\\
a & \hbox{otherwise}
\end{cases}
\]
Clearly \(\phi = \phi'\circ\phi''\) and therefore
one of \(\phi'\) or \(\phi''\) moves \(y\). Assume without loss of
generality that \(\phi'(y) \ne y\) then replace \(Q\) with \(Q'\)
and \(\phi\) by \(\phi'\).
This completes step 1.
Step 2. We use \(y\) to obtain an infinite subset \(R\) of \(X\) whose
complement in \(X\) is infinite.
Our primary tool will be the following lemma.
Partition \(C_3\) into sets \(\{S_j, T_j, U_j, V_j : j\in \omega\}\)
so that \(|S_j| = |T_j| = |U_j| = |V_j| = |C_1|\) (\(=|C_2|\)).
Let \(C_3'\) and \(C_3''\) denote the sets
\(\bigcup_{j\in\omega}(S_j\cup T_j)\) and
\(\bigcup_{j\in\omega}(U_j\cup V_j)\) respectively. Let
\(\tau\in G_P\) satisfy \(\tau(a) =a\) for all \(a\in A - (C_1\cup C_2\cup
S_0\cup T_0)\), \(\tau(C_1) = S_0\), \(\tau(S_0) = C_1\), \(\tau(C_2) =
T_0\) and \(\tau(T_0) = C_2\). Let \(\nu\in G_P\) satisfy \(\nu(a) =a\)
for all \(a\in A - (C_1\cup C_2 \cup U_0 \cup V_0)\), \(\nu(C_1) = U_0\),
\(\tau(U_0) = C_1\), \(\tau(C_2) = V_0\) and \(\tau(V_0) = C_2\). For
\(j\in\omega\), \(j\ge 1\), let \(\sigma_j\in G_P\) satisfy \(\sigma_j(a)
=a\) for \(a\in A - (S_0\cup T_0\cup S_j\cup T_j)\), \(\sigma_j(S_0) =
S_j\), \(\sigma_j(S_j) = S_0\), \(\sigma_j(T_0) = T_j\) and
\(\sigma_j(T_j) = T_0\). Similarly, for \(j\ge 1\), let \(\gamma_j \in
G_P\) satisfy \(\gamma_j(a) = a\) for all \(a\in A - (U_0\cup V_0\cup
U_j\cup V_j)\), \(\gamma_j(U_0) = U_j\), \(\gamma_j(U_j) = U_0\),
\(\gamma_j(V_0) = V_j\), and \(\gamma_j(V_j) = V_0\).
The partition \(P' = (C_1,C_2,C_3',C_3'',\ldots,C_{n_0},B_2,\ldots,
B_k)\) is a refinement of \(P\) and therefore is a support of \(X\).
Hence the two sets \(R_1 = \{\psi(\tau(y)) : \psi\in G_{P'}\}\)
and \(R_2 = \{\psi(\nu(y)) : \psi\in G_{P'}\}\) are subsets of \(X\).
Further, \(P'\) is a support of \(R_1\) and \(R_2\) so \(R_1\) and \(R_2\) are
in \(\cal N51\). We shall also prove the following:
(i) \((\forall j\in\omega, j\ge 1)(\sigma_j(\tau(y))\in R_1 \land \gamma_j(\nu(y))\in R_2)\).
(ii) \((\forall j\in\omega, j\ge 1)(\sigma_j(\tau(y)) \notin R_2\land \gamma_j(\nu(y))\notin R_1)\).
(iii) \((\forall j, r\in\omega, j,r\ge 1)\left(j\ne r \to [\sigma_j(\tau(y))\ne \sigma_r(\tau(y)) \land (\gamma_j(\nu(y))\ne \gamma_r(\nu(y))]\right)\).
It will follow that \(R = R_1\) is an infinite subset of \(X\) with
infinite complement in \(X\) and the proof will be complete.
To prove (i) we observe that since \(\sigma_j\) and \(\gamma_j\)
agree with the identity permutation outside of \(C_3'\) and \(C_3''\)
respectively for \(j\ge 1\), they are both in \(G_{P'}\).
For (ii) we first note that since \(Q\) is a support of \(y\),
a support of \(\nu(y)\) is given by
\[
\begin{align}
\nu(Q) & = (\nu(C_1),\nu(C_2),\nu(C_3),\ldots,\nu(C_n)) \\
& = (U_0,V_0,[C_3 - (U_0\cup V_0)]\cup(C_1\cup C_2),C_4,\ldots,C_n).
\end{align}
\]
Therefore if \(\psi\) fixes \(P'\) then \(\psi(\nu(y))\) has support
\[
\begin{align}
\psi(\nu(Q)) & = & (\psi(U_0),\psi(V_0),[\psi(C_3) - \psi(U_0\cup V_0)] \cup\psi(C_1 \cup C_2), \psi(C_4),\ldots,\psi(C_n)) \\
& = & (\psi(U_0),\psi(V_0),[C_3 - \psi(U_0\cup V_0)] \cup (C_1 \cup C_2), \psi(C_4),\ldots,\psi(C_n)).\\
\end{align}
\]
Since \(C_3'
\subseteq C_3 - \psi(U_0\cup V_0)\) we may conclude that for any
\(\lambda\in G_P\), if \(\lambda(a) = a\) for all \(a\in A - C_3'\) then
\(\lambda(\psi(\nu(Q)) = \psi(\nu(Q))\) and therefore
\(\lambda(\psi(\nu(y))) = \psi(\nu(y))\). Hence such an \(\lambda\) fixes
\(R_2\) pointwise. In particular, if we choose \(\lambda\) so that
\(\lambda(a) = a\) for all \(a\in A - (S_j\cup T_j)\), \(\lambda(S_j)
=T_j\) and \(\lambda(T_j) = S_j\) then \(\lambda\) fixes \(R_2\)
pointwise and by the lemma (with \(\delta = \sigma_j \circ \tau\))
\(\lambda(\sigma_j(\tau(y))) \ne \sigma_j(\tau(y))\). It follows
that \(\sigma_j(\tau(y)) \notin R_2\). A similar argument shows
that \(\gamma_j(\nu(y))\notin R_1\).
The argument for (iii) is similar. We shall show
\[
(\forall j,r\in \omega, j,r\ge 1)\left(j\ne r \to \sigma_j(\tau(y))\ne \sigma_r(\tau(y))\right)
\]
and leave the similar argument that \(\gamma_j(\nu(y)) \ne \gamma_r(\nu(y))\) to the reader. First note that
\(\sigma_r(\tau(y))\) has support
\[
\sigma_r(\tau(Q)) = (S_r,T_r,[C_3 -(S_r\cup T_r)]\cup(C_1\cup C_2),C_4,\ldots,C_n).
\]
Call this support \(Q'\). Since \(S_j\cup T_j\subseteq C_3 -
(S_r\cup T_r)\) any \(\lambda\) satisfying \(\lambda(a) = a\) for
all \(a\in A-(S_j\cup T_j)\) fixes \(Q'\) and therefore fixes
\(\sigma_r(\tau(y))\). In particular if we choose such a
\(\lambda\) for which \(\lambda(S_j) = T_j\) and \(\lambda(T_j) = S_j\)
then \(\lambda\) fixes \(\sigma_r(\tau(y))\) and by the lemma
(with \(\delta = \sigma_j\circ\tau\)) \(\lambda(\sigma_j(\tau(y)))
\ne \sigma_j(\tau(y))\). We can therefore conclude that
\(\sigma_r(\tau(y)) \ne \sigma_j(\tau(y))\).
This completes the proof of the theorem.
Howard-Rubin number: 128
Type: proofs of results
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