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(1)
and
e = e + b,+ e.
(2)
By hypothesis, a ERG. Therefore, by 1.60 and (1)) e E RC. Hence, by 1.63 and (2), e = O and finally, again by (I), a=O. In case p = w we proceed indirectly, i.e., we assume that a# 0. Then a+d#O, and the hypothesis gives a+d<*a.w.
Consequently, by 1.22(ii), a.w<*a+d
i.e., for some element f ,
a +d=f +a .w.
(3)
The hypothesis yields also c
+ c,,, ( a+ 6,) Q a . w
98
APPENDIX A
whence, by 1.22(i), either
c+%,,(a+b,)
(4)
=a - w
or else, for some finite ordinal p', C + ~ , < , ( a + b , ) G a-p'.
(5)
If (4) holds, we obtain by (3) and the hypothesis a -0=a *0+ f +a .w.
(6)
Now, since a E RC, we also have a . o E RC by 1.61(ii). Hence, by 1.63, (6) implies that a.o=O and that, consequently, a=O. If (5) holds, we have for some element g
a .p'
=c
+ z,
+ +g = c + Gcrr(a+ b,) + C,, (a + b,+pJ) + g,
( a 6,)
i.e., (7)
a-p'
= c+s,,,(a+b,)+a+d'
where
d'
= b,,
+ s<, (a+ b,+pl+l) + 9.
Since ,u' is finite, we are confronted in ( 7 ) with the situation discussed in the earlier part of the proof, and we again obtain a=O. Thus the assumption that a p O leads to a contradiction, and the proof is complete. A.6 is clearly a generalization of 1.63 and presents the affirmative solution of the problem formulated in Chapter 1 in a remark following 1.64. In the ordinal algebra of all reflexive types (cf. 2.9) A.6 holds for arbitrary ordinals ,LA, and not only for p < o .
APPENDIX B A UNIQUE DECOMPOSITION THEOREM FOR RELATIONAL ADDITION BY
BJARNI J6NSSON The principal result of this appendix involves a set A of reflexive relation types and states that, under suitable conditions on A , every reflexive relation type can be uniquely represented a sum of indecomposable relation types, the summation being carried out over a relation whose type belongs to A . (The notion of indecomposability involved in the discussion is of course defined relative to the set A.) Three particular cases of this theorem were previously known. The f i s t of them, for the set of all order types, was jointly obtained around 1944 by Tarski and the author of this appendix and coincides with Theorem 2.12 in the main part of the monograph; the second, for the set of so-called cardinal types, W R S found around 1945 by the author; the third, for the set of what can be called square types, has been recently proved by Chang and Tarski. This lead Tarski to raise the question of formulating and establishing a general unique decomposition theorem which would comprehend the three results as special cases. Our result constitutes a solution of this problem. la) The terminology and symbolism introduced in the main part of the monograph will be employed here. I n addition, by a subrelation of a relation R we understand a relation of the form R n ( B x B ) where B is some set; as is easily seen, S is a subrelation of R if and only if
S = R n [ P ( S )x F ( S ) ] . 16) The result was first stated (without proof) in the abstract [7]; the abstract contains some remarks which have not been included h this appendix.
100
APPENDIX B
By a subtype of a relation type a we mean the type of a subrelation of R where a = t ( R ) . We shall also need a generalization of the notions of an indecomposable relation and of an indecomposable relation type (defined in Chapter 2 ) . A relation R is said to be indemposable under a set K of relations if R # 0 and if the conditions
R = G e g T T iS, E K , T i ) ( T jfor every i, j E F ( S ) with i # j jointly imply that there exists at most one element i E F ( S ) such that T,#O. Similarly, a relation type a is said to be indecomposable under a set A of relation types if LY # 0 and if the conditions a=
zi,spi and
t (8)E
A
jointly imply that there exists at most one element i E F ( S ) such that O. The set of all reflexive relation types which are indecomposable under a set A of relation types will be denoted by I ( A ) . I n the following theorems B.1-B.4 (which partly generalize 2.1-2.5) we formulate certain elementary properties of general relational addition.
THEOREM B.l. (i) x R O = X . o R i = O . (ii) If j E F ( R ) , and if'S,=O whenever i E F ( R ) and i#j, then X,RSi=Sj. (iii) Sj _C L s R S ifor every j E F ( R ) . (iv) If Ti C S j for every i E F ( R ) , then X,.Ti C x.BSI. (v) x.RTi)(Xif and only if T i ) ( # for every i E F(R). (vi) I f T = then G,,-,Uj= Uj. (vii) If B is the set of all elements i E F ( R ) such that S,#O and if T = R n ( B x B ) , then x*RSi=zi,TSi. (viii) T * ( .Si) = X , R ( TSJ. . PROOF : obvious.
zsR#%, x,R
zjaT
zi,
THEOREM B.2. If T=x,.Si. and if Si)(Sjwhenever i, ~ E F ( R )
and i # j , then we have: (i) T n [S(SJ x F ( S , ) ] = S i for every i E F ( R ) ; (5) T n [ F ( S , )x F ( S j ) ]= P(S,)x F ( S j )whenever i # j and(i,j) E R ;
(iii) T
n [ F ( S i )x F ( S j ) ] = O whenever i, j
PROOF : obvious.
E
F ( R ) , and (i, j ) $ R .
101
DECOMPOSITION THEOREM FOR RELATIONAL ADDITION
THEOREM B.3. If all the relations S , with i E F(R) are reflexive, is also reflexive. Conversely, if the relation then the relation Z s R S ii s reflexive, and if Si)(Xj whenever i,j E P(R)and izj, then all the relations A, with i E F ( R ) are reflexive. PROOF:The first part of the theorem is obvious, the second part follows from B.2(i).
xsRSi
THEOREM B.4. If C+,RTi=Zk.S U,, all the relations T i with i E F ( R ) and U , with k E F(S) are reflexive, and T , ) ( T , whenever i , j E F ( R ) and i # j , then Ti=Xk,s(Tin U,) for every i E F ( R ) . PROOF:
By B.l(iii) we have
Ti = Ti n 2 k . S
so that (l)
Ti=
ukeF(S)(Tin
uk)
u,
UU<E.Z)eS.k+Z(Tin
>
[F(uk)xF(uZ)l)*
Using B.l(iii), B.2(i), and 2.1(i), we see that, if (k, 1) E S and k # l , then Ti
[(F( uk) x
( uZ)l = =
=
CF
IF
( uk)
x
( ul)l
CFVi)n F ( Uk)l x [ F (Ti)n F ( UJl F ( T i n U , ) x F ( T , n UZ),
and we conclude by (1) that
Ti = s , s (Tin uJ* Next we prove a refinement theorem which will subsequently be used to obtain unique decomposition theorems for the addition of reflexive relations (B.6) and the addition of reflexive relation types (B.9).
THEOREM B.5 [GENERAL REFINEMENT THEOREM FOR RELATIONAL ADDITION]. Let K be a set of reflexive relations with the following properties (a) there exists a n R E K such that R#O; (b) if R E K and S i s isomorphic to a subrelation of R , then S E K ; (c) if X E K for every finite subrelation S of R, then R E K ; (d) if R E K , Si E K for every i E F ( R ) , and S,)(Xj whenever a', j E F ( R ) and i#j, then c.,Si E K.
102
APPENDIX B
Suppose R is a reflexive relation, I is a non-empty set, and Si E K for every i E I . If R = Zkm8iQi,k for every i E I , and if Qi,k)( Qi,l whenever i E I , k, 1 E F ( S J and k # l , then there exist reflexive relations T , Wi,kwith i E I and k E F(S,), and U , with f E F ( T ) which satisfy the following conditions : (i)
T E K , and WiVkE K for all i E I a.nd k E F(S,); (ii) R=C,.,U,, and U,#O for every f E F ( T ) ; (iii) T = for every i E I ; (iv) QiSk= zj,w,,U, for all i E I and k E F(S,); (v) U j ) ( U,, whenever f , g E F ( T ) and f # g ; (vi) WiSk)(Wi,, whenever i E I , k, E E F(S,), and k f l . PROOF:Observe that by B.3 all the relations QiSkwith i E I and k E F(S,) are reflexive. Consider the set C of all functions f on I such that f ( i ) E F(S,) for every i E I, and for each f E C let
z.S6Wd.k
U , = n i e r Qi.m-
(1)
Let the relation V and the set D be defined by the conditions: (2)
( f , g) V if { every i I. E
and only if f , g E C and ( f ( i ) , g ( i ) ) € 8 , for
E
f
(3)
E
D if and only if f E C and U,#O.
Also let
T = V n (Dx D),
(4)
and for each i E I and k by the condition: (5)
(f4g)
E
E
F ( S J let Wi.k be the relation defined
WiaEif and only if ( f , g ) E T and f ( i ) = g ( i ) = k .
By our hypothesis we have = ' k e P ( S 4 l 'k.i&
for every i (6)
E
U(k.I)eSi.k+Z
[F(&6.k)
x F(Qi,t)l
I and, consequently,
= nieI
(ukeP(S')
Qik
U(k.Z)eSr,k+2 [F(&i.k)
F(&i.t)l)
DECOMPOSITION THEOREM FOR RELATIONAL ADDITION
For each i
E
103
I and (k, Z) E S let ~ Yi.k.l
=
x
LP(&i.k)
(Qi.t)1
9
and use B.2(i),(ii) to infer that Y ; , k , k = Qi,k
Y4,k.I =
F (QiSk) X F
for every i E I and k E E”(s,), whenever i €1,0,I> E Si, and k # 1.
(Qi,$)
By (2) and (6) we therefore have
R = U(r.o)sv nitr Yi.tci),m or, equivalently,
R = Ujtc nisIQijci)u U
R=
U t c m U,UU
(Rn[ w J , ) x W g ) 1 ) .
For any ordered couple ( f , g) E V with f # g we can choose an element j E I such that f ( j ) # g ( j ) and use (1) and B.2(ii) to infer that
F ( U , ) x F(U0)c F ( Q m )x FP&7(?7) c R. Together with ( 7 ) this gives
R = U,t,,p
u, u U < f . I ) E Y . f * Q [F(U,) x F(U0)l = Xf.7 u,,
and using (3), (4)) and B.l(vii) we conclude that
R=
2f.T
uf.
Thus (ii) holds; (v) and (vi) readily follow from (1) and (5). Now suppose i E I and k E F(X,). By (ii) and B.4 we have (8)
&i.k = L \ f . T ( Q i . k
uf)-
It follows from (1) that Q k n U,= U , in case /(a)= k , but Qimkn U , = 0 in caae f ( i )# E . By ( 5 ) , ( 8 ) , and B.l(vii) we therefore have and (iv) holds.
Q6.k
=
X,.W*,~ ui,
104
APPENDIX B
Next we prove (iii). Suppose i E I , and consider any functions f, g ED. Then f E F(Wi,,a) and g E F(Wisos) by (4) and (5). If (f, g ) E T, then (f(i), g(i)) E S ( by (2) and (a), and it follows by (6) that ( f , g) E W,,,,,, in case f(i)=g(i), while
(f, 9 ) E F ( W i , f d x F(Wi.u,d in cilse f ( i ) # g ( i ) , so that in either c&8e
( f , g>
(9)
z . S i Wi.k*
Conversely, aasume that (9) holds. If f ( i )=g(i), then (f, g) E Wi,l,6 by (vi) and B.2(i). If f(i)#g(i), then (f(i), g(i)) E S by ~ (9), (vi), and B.2(iii), and it follows by (l), (3) and B.2(ii) that 0
For every
+ F(U,)xII’(Uu)CP(Q,,,,,,)xP(Q,,,,it)
iEI
cR.
we therefore have
F ( U , ) XP(U,) Z R n CP(Qi.t(iJ xp(Qj.o(lJl’ so that
Rn
(QjA(9)) x
F (Qj,U(9Jl
f
0;
but by B.2(iii) this implies that ( f ( j ) , g ( j ) ) €Xi. Using (2) and (4) we conclude that ( f , g) E T, and (iii) holds. Observe that by (b), (d), (iii), and (vi) the two parts of condition (i) are equivalent. I n proving that this condition is satisfied we shall first consider the caae in which I has a finite number n of elements. For n= 1 the conclusion is trivial; for, if I consists of just one element i, then V is isomorphic to Sj by (2), hence T is isomorphic to a subrelation of S , by (a), so that T E K by (b). Suppose m is a positive integer and assume that (i) holds in the case in which n=m. If n=m+ 1, then we consider arbitrary elements j E I and k E F(X,) and let I’ be the set of all elements i E I with i # j . Repeating the construction given at the beginning of the proof with I replaced by 1’,we consider the set C’ of all functions f on I‘ such that f(i) E F(S,) for every i E 1’,let (10)
u;= nw
Qi.,(i)
DECOMFOSITION T H E O RE M FO R RELATIONAL ADDITION
105
for every function f EC’, and define the set D’ and the relations V’ and T‘ by the conditions: (11)
77’ if and only i f f , g ( every (f’g) i It; E
E
C and (f(i), g(i)) E Si for
E
f
(12)
E
D‘ if and only if f EC’ and U;#O; TI= V’ n (D’ x D’).
(13)
By our inductive hypothesis we have T’ E K. For each function f E F ( W i s k we ) let h(f) be the function on I‘ such that h ( f ) ( i ) = f ( i )for every i E I. From (1)-(5) and (10)-(13) we see that h maps the set F ( W i J in a one-to-one way into the set D’= F ( T ’ ) and that, if f , g E P(Wi,k), then the conditions
E
Wj&, < f ( i )g?( i ) ) ESi for every i
EI
f , and < h ( f ) , h ( g ) ) E T ’
are equivalent. Hence h maps Wi,k isomorphically onto a subrelation of T’.Consequently Wick E K by (b). Thus we see that, if (i) holds for n = m , then it also holds for n = m + 1. It follows by induction that (i) holds whenever I is finite. Dropping the assumption that I be finite, we consider a finite subrelation P of T.Then there exists a finite subset I’ of I such that, i f f and g are any distinct members of F ( P ) ,then f ( i ) # g ( i ) for some i E I . Again we let C‘ be the set of all functions f on I’ such that f ( i ) E F(S,) for every i E I f , and define the relations U; with f EC’, the set D’, and the relations V‘ and T‘by the conditions (10)-(13). By the particular case of (i) which has already been proved we then have T’ E K. For each function f E F(P)let h(f) be the function on I‘ such that h(f)(i)=f(i) for every i E I f . From (1)-(4) and (10)-(13) we see that h maps the set F(P)in a one-to-one way into the set F(T’)and that, if ( f , g ) E P ,then ( h ( f ) ,h ( g ) ) E T‘. Conversely, suppose f and g are distinct members of F ( P ) , and assume that (h(f),h(g)) ET’.We can then find an element j E I such that f ( j ) # g ( j ) , and by ( 1 1) and (13) we have ( f ( j ) , g ( j ) ) E S ~It. follows by ( l ) , (3), and B.2(ii) that 0
f
F(U,)xF(U,)CF(&i.tn)XP(&i.Pcn)CR.
106
APPENDIX B
For every i so that
E1
we therefore have
F ( U d x F(UU)c
n [F(Qi.to)x F(Q4.UdIY
Rn [F(Qi.fdXFfQi.B(i.))l
+ 0,
but by B.2(iii) this implies that (f(i),g ( i ) ) €Xi. Using (2) and (4), we infer that ( f , g) E T and hence ( f , g) E P. Thus h maps P isomorphically onto a subrelation of T‘, and we have P E K by (b). Since this holds for every finite subrelation P of T, we conclude by (c) that T E K, and the proof is complete. Several equivalent formulations of the set of premises (a)-(d) in B.5 are known. Thus, for instance, we can respectively replace (b) and (d) by the following conditions:
(b’) if R E K and S is isomorphic to a finite subrelation of R, then S E K; (d’) if R and all the relations Si with i E F ( R ) are finite members 01 K and if S,)( Sj whenever i , j E F ( R ) and i # j , then CeRSi E K. Condition (b’) is clearly weaker than (b), but it is easily seen that the two conditions are equivalent on the basis of (c); the same applies to conditions (d) and (d‘). It is less obvious that condition (c) can be replaced by the following condition which is equivalent to (c) on the basis of (b) or (b’): (c‘)
if i is any subset of K which i s simply ordered by set inclusion, then U R E R L E K. 16)
If in B.5 we take for K the set of all reflexive relations, then
the premises (a)-(d) are clearly satisfied, and we obtain a simplified la)
For the equivalence of (c) and (c’) see Theorem 1.2 and its proof in
[18], pp. 578 f. It may be mentioned that Theorem 1.2 gives a simple metamathematical characterization of those sets K of relations which satisfy
B.5(b),(c). I n fact, such sets K prove t o coincide with the sets of models of arbitrary (possibly infinite) systems of first-order universal sentences, with a two-placed predicate ae, the only non-logical constant. I t would be interesting to obtain a simple metamatliematical characterization for the sets K which satisfy B.5(b), (c),(d).
107
DECOMPOSITION THEOREM FOR RELATIONAL ADDITION
form of the refinement theorem, which, however, is not adequate for our purposes.
THEOREM B.6. If K i s a set of reflexive relations which has the properties (a)-(d) listed in Theorem B.5, then every reflexive relation R can be represented in the form
R
= G.T
u
E F ( T ) are indecomposable U,)( U , whenever f , g E F(T)and f i g . This representatiort is unique in the following sense: if
where T
E
K , all the relations U , with f
under K , and
R = 2i.V
w,
is unother representation with the same properties, then there exists a function h which maps T isomorphically onto V in such a way that U,= W,,, for every f E F ( T ) . PROOF: Roughly speaking, we are going to apply B.5 to all possible representations of R as a sum of pairwise strictly disjoint non-empty relations over a relation belonging to K . More precisely, we choose a set I , relations S , E K with i E I , and relations Qr,k# 0 with i E I and k E F ( S J which satisfy the following three conditions : (1) (2)
(3)
I
Qi,k)(Qtvl
R = L,sd QCmk for every i E I ; whenever i E I , k, I E F(S,), and 1;
zk,S,Q;
f
1;
if R = is any representation of R with S' E K , Q;# 0 for every k E F ( S ) , and QL)(Qi whenever lc, 1 E F ( S ' ) and k#E, then there exist an element j E I and a function h mapping S' isomorphically onto S , in such a way that Q;=Qi,h(k, for every k E F( S') .
That this set 1 is non-empty follows from conditions (a)and (b). In view of (1) and (2) we infer from B.5 that there exist relations T,Ur+,,with i E I and I% E F(S,), and U , with f E F ( T ) which satisfy conditions (i)-(vi) listed there. Since K has the property B.5(b), we see from B.l(vii) that in order to prove that u, is
108
APPENDIX B
indecomposable under K it is sufficient to consider decompositions
uo = 2.v, Q;
(4)
where V , E K, Q;#O for every k E P(V,), and Qd)( Q; whenever k, I E P(V,) and k f I , and to show that under these conditions P(V,) consist5 of just one element. Clearly we may also assume that P(7,) n F ( T )= 0. For every f E F(T)with f # g let 7 , be the relation consisting of just the one ordered couple
U , = &.v,Q; and V , E K for every f~ F ( T ) .
Letting
S' = 2 i . T V,, we therefore infer from B.l(vi) and B.5(ii) that
R=
2,sQ;.
Since K has the property B.5(d), we see that S' E K. Furthermore, in view of B.5(ii),(v), we also have Qi# 0 for every k E P(S'),and Qi)(Q; whenever k, I E F (S') and k # 1. We can therefore apply (3) to obtain an element j E I and a function h mapping S' isomorphically onto S, in such a way that Q;=Qi,h,k,for every k E F(S'). By B.5(iii) there exists 2 E F ( T ) such that g E P ( W j J . Using (a), B.l(iii), and B.5(iv), we therefore see that, for every k E F(V,), Qi. h(k) =
QL C ug C Qi. 1 ;
and, since Q j . M r , # O , we use (2) to conclude that h ( k ) = l . This shows that F(Tr,) must consist of just one element, as was to be proved. Finally suppose we have two representations of R with the required properties :
R = 2t.T
u, = 2 . v w,.
By B.4 we then have
U,= W, =
z,y( U, n W,) for every f
E
F(T),
( U ,n W,) for every g E F ( V ) ,
DECOMPOSITION THEOREM FOR RELATIONAL A D D ITION
109
and it readily follows that there exists a one-to-one function h which maps F(T)onto P(8)in such a way that U,= Who,for every f E P(T). Furthermore, if f and g are distinct members of F(T), hhen it follows by B.2(ii),(iii) that the conditions
( f ,g> E T , P(U,)x F(U,) R, P ( K ( , , )x F(Jc(,,) c R, ( h ( f ) h(gD , E
c
are equivalent, so that h maps T isomorphically onto Y . The proof has thus been completed. Passing now to relation types we f i s t state, in B.7 and B.8, several elementary properties of relational addition of types.
THEOREM B.T. (i) ~ R O = z i , O c r i = O . If j E F(R), and if a,=O whenever i (ii)
xaa(
E
F(R) and i# j , then
= ai.
(iii) If j E F(R), then cri is a subtype of z , R a i . then is a (iv) I f , for every i E F(R)lL Y ~ is a subtype of #Ii, subtype O f z j , R b i ’ ( v ) If T=z:,.,Si, and if Si)(Si whenever i , j E F(R) and i # j , then G.R Z,s$~j = 29.T L*i* (vi) If B i s the set of all elements i E F(R) such that ai#O, and if S = R n ( B x B ) , then (vii)
z,Bmi
x,R~6=x,scri.
I X * ( Z < , R B i )= z i , B
(@. B 6 ) ’
PROOF:Parts (i), (ii), (v), (vi), and (vii) axe easy consequences of B.1, while (iii) and (iv) readily follow- from the definitions of the notions involved.
THEOREM B.8. (i) 0, 1 E RT. E RT if and only if cri E RT for every i E F(R). (ii) If z(R) E RT, then zi,R1=z(R). (iii) (ic) a . O = O . c r = O and rn.l=cr. (v) If cr E RT, then l.cr=a. PROOF:obvious,
x,Rai
We now obtain the main result of this appendix:
THEOREM B.9
[UNIQUE DECOMPOSITION
THEOREM FOR RELA-
110
APPENDIX B
Let A be any set of reflexive types satisfying the TIONAX, ADDITION]. following conditions : (a) 1 E A ; (b) if a E A and p i s a subtype of a , then /3 E A ; E A for every finite subtype ,L? of a , then a E A ; (c) if (d) if t ( R )E A and a{ E A for every i E P ( R ) ,then EA. Under these assumptions every reflexive type a can be represented in the form a = Xi.RBi
x,R~i
where t ( R )E A , and b5 E I ( A ) for every i E F ( R ) . This representation is unique in the following sense: if is another representation of the S a m kind, then there exists a function h which maps R ismorpitically onto S in such a way that pi= yh,{)fm every i E F(R). PROOF: by B.6. Using the terminology introduced in Chapter 3 , p. 82, we can formulate the last part of the preceding theorem more simply: if 01
=2t.R
Pi = 25.8 ~j
are two representations of LS: of the kind discussed, then the systems
DECOMPOSITION THEOREM FOR RELATIONAL ADDITION
111
tion of B.9 to the sets A, and RT does not lead to any interesting consequences since the resulting decompositions of a reflexive type are trivial. We want now to discuss some more interesting applications of B.9 to special sets of relation types. A relation R is called a cardinal relation if, for all x and y, the formula (s, y) E R implies that x=y. Given any set B , let B" be the set of all ordered couples (2,s) with x E B. Clearly every cardinal relation R uniquely determines a set B such that R = Bc; in fact, B= F(R). Conversely, every relation R of the form R = B" is a cardinal relation. The relational sum X , S , over a cardinal relation R = Bc obviously coincides with the union 8,. By a cardinal type we understand of course the type of a cardinal relation. The set of dl cardinal types is denoted by C T . For sums a,of relation types over a cardinal relation R = B" we introduce a special notation by putting
ud,
zg.B
The operation 2' is referred to as cardinal addtition. As a particular case we obtain the binary cardinal addition; in fact, given any two relation types ,!? and y , we put ,!?+"y = E ; € B
OLi
where B is a set consisting of two elements, say 0 and 1, and where a,,=,!? and a l = y . I n the next few theorems, B.10-B.13, we state some elementary properties of the sets CT and I ( C T ) and the operations 1' and -I-". The proofs are obvious and will be omitted.
THEOREM B.lO. (i) 0, 1 E C T . (ii) If ai E CT for every i E B, then z c B u ge C T . (iii) If a , ,!? E C T , then a ,!? E C T . notion of indecomposability a variant of the unique decomposition theorem was stated by FraYssB in [ 5 ] ; however, it applies exclusively to finite relations and, apart from this restriction, its conclusion is not entirely analogous to that of B.6 or B.9.
112
(iv) If (v) If
APPENDIX B bc
E C T and /3 i s a subtype of a, then @ E C T . E C T for every finite subtype p of a, then a E CT.
r.
r.
Theorem B.7 extends automatically to the operation Thus, in particular, the associative law holds for Moreover, in opposition to the general relational addition, cardinal addition satisfies the commutative law : THEOREM B.ll. Let h. be a function which maps a set B onto a set G in a one-to-one way, and let pi and yi be types correlated with elements i E B and j E C in such a way that pi= Y,,(~,for every i E B. Then Z c B
Pi = Z e C P i .
THEOREM B.12. For any given relation types (i) O L + " / ? = @ + ~ ~ ; (p+" y ) = ( a+"I y; (ii) (iii) r x + " O = a ; (iv) if a ~ . ~ / 3 = 0then , a=@=O; (v) a.( p +C y ) = a . p + c a.y .
+"
K,
,8, and y ,
+"
THEOREM B.13. a E I ( C T ) if and only if afO and the formula a = p i c y always implies that /?=0 or y = 0. By specializing the unique decomposition theorem B.9, we obtain
B.14. l8) Every refixive type a can be represented in THEOREM the form a = Z C I ( C T )(B. xs)
where x s E CT for every 5, in the following sense: if
E
I ( C T ) . This representation i s unique
( B . 4)
=Z€I(CT)
i s another representation of the same kind, then z p = I , for every p E I(CT). PROOF:All the types belonging to the set CT are of course I*) Theorem B.14 and B.15 were first published, in a slightly different form, in [17], pp- 249 ff.(and credited there to the author of this appendix).
DECOMPOSITION TBXOREM FOR RELATIONAL ADDITION
113
reflexive. By B.10 this set satisfies the premises of B.9 for A =CT. By applying B.9 we therefore obtain a representation of any given reflexive type a :
(i)
=xca
Y4
where yi E I(CT) for every i E A . For every E I(CT) let B, be the set of all elements a' E A with yi=/?. Using B.7(v),(vii), B.8(iv), and B.ll, we easily obtain from (1) a = Z c I ( C T 1 ( C : e B p yi) = Z i c l ( C T )( Z t e B g 8 ) =zeI(CT)
( B * Z : € B p '1,
and letting xp=t(BOp) we see with the aid of B.8(iii) that is the desired representation of a. The unicity of this representation readily follows from B.9.
Consider now an arbitrary algebraic system ( A , +) formed by a non-empty set A and a binary operation -k under which A is closed. Let E be an arbitrary set, let F be the set of all functions on E to A, and, given any two functions f , g E P,let f 4. g be the function h E F determined by the formula
h(z)= f ( z )+g(z) for every x
E
E.
The system ( F , i) thus obtained is called the cardinal (or direct) power of ( A , +) with the exponent E , in symbols ( A , +)&. Using this notation we formulate the following important consequence of B.14:
THEOREM B.15. The system (RT, +") i s isomorphic to a cardinal power of the system (CT, +"), and in fact (RT, E (CT, c)r m ) .
+")
+
P R O O F : By B.14 every reflexive type sentation of the form
(1)
a = 2;cI(CTl
(B
*
x,)
OL
has a unique repre-
114
APPENDIX B
where xs E CT for every #? E I(CT). This formula clearly establishes a one-to-one correspondence between all types in RT and all functions on I(CT) to CT. Let (2)
=ZrItCm
(B.4
be the representation of another reflexive type a'. Using B.i'(v), B.11, and B.12(v), we obtain from (1) and (2) mSCLy'
= z ; r I ( C T ) [#?+)9+".;)1
where, by B.lO(iii), xs+"xk E CT for every p E I(CT). Hence we conclude that the correspondence (between elements of RT and functions on I(CT) to C T ) given by (1) establishes an isomorphism between (RT, +") and (CT, +c)IccT). This completes the proof.
As is easily seen, the algebraic system (CT, +") involved in B.15 is isomorphic to the system (C, +) where C is the set of all cardinal numbers and + is the ordinary addition of cardinals. Hence (mainly as a consequence of the well-ordering theorem) the algebraic structure of (CT, +") and the arithmetical properties of this system are very simple. The importance of B.15 consists in the fact that, as is well known from abstract algebra, various properties of algebraic systems automatically extend to cardinal powers of these systems, and hence in particular various familiar properties of (CT, +") automatically extend to (RT, +"). Three examples of such properties are explicitly stated in the following THEOREM B.16. Suppose 01, 8, y E RT, and let v be a finite cardinal type digwent from 0. We than have: (i) if a = ~ y + " ( , ! I + ~ y ) , then ol=a+",8=a+"y; (ii) if y i s finite and a+"y=#?+"y, then a=#?; (iii) if a . v = B . v , then a=,!?.
B. 16(iii) apparently expresses a property of ordinal multiplication, and not of cardinal addition. Actually, however, ordinal multiplication by a finite cardinal type can be defined recursively in terms of +' by means of the formulas L y e
0 = 0,
Ly
.(v+"
1)= Ly .Y+" a.
115
DECOMPOSITION TEEOREM FOR RELATIONAL ADDITION
We may mention still some further properties that extend from (CT, +") to ( R T , +"). Given any two types 01 and p, let m g c p mean that n f " y = p for some type y. As is known, the set CT is simply ordered and, in fact, well ordered by the relation <". Consequently, the set CT is lattice-ordered by <', and in this lattice-ordering every non-empty subset of CT has a greatest lower bound, and every subset of CT which is bounded above has a least upper bound. Now it turns out that, although the properties of simple ordering and well-ordering do not extend from the system
A relation R will be called a square relation if it is of the form R = B x B for some set B. The set B is of course uniquely determined by R since B = F(R). For relational sums Ri over a square relation R = B x B we introduce a special notation by putting
x,B
Z r B Ri=
Clearly X r B Ri =
We also put
ud
BRi
2 i . B x B Ri.
Ui.irB.i+j
S i-OT= x
E B
LF
(Ri)
(Rj)l
'
Ri,
where B is a set consisting of two elements, say 0 and 1, and where R,=S and R,=T. The operations 2' and may be called square addition and binary square addition, respectively. It is obvious how the notion of a square relation type and the operations 2 and +* on arbitrary relation types should be defined. The set of all square types is denoted by ST. For this set ST and the operations 2 and +a we can repeat, practically without changes, all the remarks and arguments concerning CT, and +c; the results thus obtained are summarized as follows:
2
THEOREM B.17. 19) The theorems B . l k B . 1 6 (as well a8 the Theorems B.17 and B.18 are recent results which were obtained 19) jointly by Chaw and Tarski and appear here in print for the first time.
116
APPENDIX B
r,
auxiliary theorems B.10-B.13) remain valid if we replace in them CT by ST, 2" by and +" by +' everywhere.
THEOREM B.18. (i)
We have (CT,
+") z (ST,+'),
(RT,
+") z
and hence also
(ii)
PROOF:Each of the two systems (CT, +") and (ST, + 8 ) is easily seen to be isomorphic to the system of all cardinal numbers with the ordinary addition of cardinals; hence (i) follows at once. By €3.15 and B.17 we have (RT, +") g (CT, +c)l(cT) and
for every relation type oc E RT. As is easily seen, / ( a )E I ( X T ) and g ( a ) E I(CT) for every 01 E RT. Also, if 01, fi E RT and 0 1 # f i , then f(oc)#f(b) and g(a)#g(/3) by B.lS(ii) and B.17. Consequently, f maps I(CT) onto a subset of I(ST), and g maps I(ST) onto a subset of I(C'T),both in a one-to-one way, and it follows by the Cantor-Bernstein theorem that there exists a function h which maps I(CT)onto I ( S T )in a one-to-one way; in fact, we can easily give an explicit definition of such a function. This completes the proof.
It may be noted that Theorem B.15 and the analogous result for square addition (implicitly stated in B.17) remain valid if and +' are replaced in them by and respectively; the same applies to Theorem B.18. The statements thus obtained clearly generalize the original theorems and imply the latter as particular cases. These generalizations presuppose, of course, that the notion of a cardinal (direct) power has been extended to
+"
r,
DECOMPOSITION T E E O RE M FOR RELATIONAL A D D ITION
117
algebraic systems ( A , 2) where 2 is an operation which is performable on arbitrary systems of elements of A and yields new elements of A . As a third example of a set of relation types to which B.9 applies we want to mention the set OT of all order types. The relation types indecomposable under OT, i.e., the elements of I(OT), coincide with the indecomposable types as defined in Chapter 2 of this monograph (see the remarks preceding 2.12). The set A =OT clearly satisfies all the premises of B.9; hence, by applying B.9 to this set, we obtain the unique decomposition theorem stated in Chapter 2 as 2.12. However, the binary ordinal addition + discussed in Chapter 2 is not commutative, and the same applies a fortiori to the general ordinal addition, i.e., to the relational addition over a simply ordering relation R. Therefore the unique decomposition theorem for ordinal addition cannot be given the simple form in which the analogous result for cardinal addition was stated in B.14, and it does not yield any consequences as powerful as B.15; in particular, the system (RT,+) is not isomorphic to a cardinal power of (OT,+). (A remote analogue of B.15 is mentioned in Chapter 2, p. 83). Speaking loosely, Theorem 2.12 is very helpful in extending to arbitrary relation types results which have been obtained for order types (compare, e.g., the proof of 2.13), but, as opposed to B.14, it does not seem to provide us with a general and automatic method of extending such results. It should be noted that the cardinal addition +', the square addition +", and the ordinal addition + are the only binary operations which we obtain from general relational addition by restricting ourselves to relations R whose field consists of exactly two elements. In fact, from the definition of relational addition it easily follows that no generality is lost by taking R to be reflexive, and a reflexive relation whose field consists of two elements is clearly either a cardinal relation, a square relation, or a simply ordering relation. (We disregard here the dual ordinal addition + * ; cf. 1.2 or 1.3(5).)Among the three binary operations two, +c and $-', are commutative while the third, +, is not. The
x,R~i
x,R~i
118
APPENDIX B
arithmetics of +’ and (based mainly upon B.15 and the analogous result for square addition) are simple ; the arithmetic of +, which constitutes the main topic of this monograph, is rather involved and difficult. In this connection the following metamathematical result has been obtained by Tarski : Assume that by the elementary theory of an operation we understand the totality of laws which hold for this operation and are formulated within the first-order predicate logic ; then the elementary theories of +’ and +‘ are decidable while the elementary theory of + is undecidable. I n other words, there is a mechanical method which permits us to decide in each particular case whether a given elementary statement holds for the operation +’ or +#; however, no such method exists or will ever be found for the operation + . 20) I n addition to the sets discussed so far, there are many other sets of reflexive relation types which have the properties (a)-(d) listed in B.9. As examples we may mention the three sets consisting, respectively, of the types of all reflexive and transitive relations, all reflexive and symmetric relations, and all reflexive and antisymmetric relations. Obviously, the intersection of two or more sets having the properties in question again has these properties. This leads to two further examples, the set of all types of equivalence relations and the set of all types of partially ordering relations. The question naturally arises how many sets there are which satisfy the hypothesis of €3.9. The answer is given in the following theorem, which is a joint result of Chang and the author of this appendix :
THEOREM B.19. The family C of all subsets A of RT which satisfy conditions (a)-(d) of B.9 has the power of the continuum. For notions involved in the last remarks consult [19]. Instead of 20) “the elementary theory of a n operation” the term “the arithmetic of an operation” is also employed; throughout this monograph, however, the term “arithmetic” is used in a wider and looser sense. In view of R.15 and B.18 the decidability of the theories of and easily reduces t o the results in [lo], 1111, and [12]; the undecidability of the elementary theory of can be derived from a joint result of W. Szmielew and Tarski stated in [19], pp. 86 f., by means of a general method developed in Part I of [19].
+’
+”
+
DECOb4POSITION THEOREM FOR RELATIONAL ADDITION
119
PROOF:Let F be the set of all finite relation types, From B.g(c) it clearly follows that, for any sets A and B in C , the formula A n F = B n F implies A = B. Hence C has the same power as a family of subsets of F . Since the set P is denumerable, the family of all its subsets has the power of the continuum, and therefore C has a t most the power of the continuum. 21) It remains to be shown that C has at least the power of the continuum. To this end, given any finite ordinal v, we denote by (xv the type of the relation consisting of the couple ( v + 2 , 0) and of all the couples <,u,p) w i t h p ~ v f 2and