Polarized relations at singulars over successors
Shimon Garti
Einstein Institute of Mathematics,
The Hebrew University of Jerusalem,
Jerusalem 91904, Israel
[email protected]
Abstract.
Erdős, Hajnal and Rado asked whether (ℵ2ℵω1)→(ℵ0ℵω1)2 and whether (ℵ2ℵω1)→(ℵ1ℵω1)2.
We shall prove that both relations are independent over ZFC.
We shall also prove that (ℵ2μ)→(ℵ2μ)2 is independent over ZF for some μ>cf(μ)=ω1.
Key words and phrases:
Polarized partition relations, generalized Martin’s axiom, scales, determinacy
2010 Mathematics Subject Classification:
03E02, 03E25, 03E60
0. Introduction
Let κ≤λ be infinite cardinals.
We shall say that (κλ)→(βα)χ iff for every coloring c:λ×κ→χ one can find A⊆λ,B⊆κ such that otp(A)=α,otp(B)=β and c↾(A×B) is constant.
The case in which λ=κ+ is of particular interest, and the strong form (κκ+)→(κκ+)2 has been investigated quite thoroughly.
It is still unknown whether the positive relation (κκ+)→(κκ+)2 is consistent when κ is a successor cardinal.
The first case is κ=ℵ1, and the possible consistency of (ℵ1ℵ2)→(ℵ1ℵ2)2 is an interesting open problem, a variant of which appeared in [6, Question 27].
In this light, Erdős, Hajnal and Rado asked whether a much weaker statement like (ℵ1ℵ2)→(ℵ1ℵ0)2 is consistent, see [8, Problem 12].
Soon after the discovery of forcing, Prikry proved in [17] that (ℵ1ℵ2)↛(ℵ1ℵ0)2 is consistent.
A few years later, Laver proved in [15] that (ℵ1ℵ2)→(ℵ1ℵ0)2 and even the much stronger relation (ℵ1ℵ2)→(ℵ1ℵ1)ω are consistent.
Hence [8, Problem 12] of Erdős, Hajnal and Rado is independent of ZFC.
A related problem arises if one replaces ℵ1 by a singular cardinal μ such that cf(μ)=ω1.
Thus one may wonder whether (ℵ2ℵω1)→(ℵ0ℵω1)2 and even whether (ℵ2ℵω1)→(ℵ1ℵω1)2 are provable, see [8, Problem 15].
We shall prove that both relations are independent of ZFC.
The above problem is phrased with respect to ℵω1, but the general question is about every μ>cf(μ)=ω1.
The ultimate relation (ℵ2μ)→(ℵ2μ)2 is far-fetched, though we do not know whether it provably fails in ZFC.
However, we will show that this relation is independent over ZF by proving the positive direction under the assumption AD+V=L(R).
Determinacy will also help us to establish a positive answer to an old problem from [6] about cube polarized relations.
Our notation is standard for the most part.
We shall follow [9] with respect to arrows notation.
We suggest [1] for background in pcf theory and [23] for background in polarized relations.
We employ the Jerusalem forcing notation, hence p≤q reads p is weaker than q.
Finally, I would like to thank the referees of the paper for a careful reading of the original manuscript and a lot of helpful suggestions.
1. Between MA and GMA
In this section we address the first part of [8, Problem 15] by proving the independence of (ℵ2ℵω1)→(ℵ0ℵω1)2.
Ahead of proving our statements let us recall that if κ≥cf(κ)>ω and one forces Martin’s axiom with 2ω>κ then one obtains (ωκ)→(ωκ)2, see [14].
In particular, Martin’s axiom with 2ω>ω1 implies (ωω1)→(ωω1)2.
Therefore, a natural attempt to get the consistency of (ℵ1ℵ2)→(ℵ1ℵ2)2 (or at least something in this direction) would be one of the generalized versions of Martin’s axiom to uncountable cardinals.
We shall see below that this attempt fails.
This will be done by proving (ℵ1ℵ2)↛(ℵ1ℵ0)2 under one of the traditional generalizations of Martin’s axiom, and in the same context we will also have (ℵ2ℵω1)↛(ℵ0ℵω1)2.
The known generalizations are similar, and we shall use Shelah’s version from [18] dubbed henceforth as the generalized Martin’s axiom.
Theorem 1.1**.**
*Generalized Martin’s Axiom.
One can force 2ℵ0=ℵ1∧2ℵ1>ℵ2, and if P is a forcing notion of size less than 2ℵ1 satisfying the following three requirements:*
- (a)
Each pair of compatible conditions has a least upper bound in P.
2. (b)
Every countable increasing sequence of conditions has a least upper bound in P.
3. (c)
If {pi:i<ℵ2}⊆P then there is a club C⊆ℵ2 and a regressive function f:ℵ2→ℵ2 so that for α,β∈C∩Sℵ1ℵ2 if f(α)=f(β) then pα∥pβ.
then there is a generic filter G⊆P which intersects any given collection of κ dense subsets, when κ<2ℵ1.
If κ satisfies α<κ⇒αℵ0<κ then the assumption ∣P∣<2ℵ1 can be omitted.
\qed\refthmshelahgma
Our small component in the theorems below will be ℵ1, but in most of the statements we can replace ℵ1 by larger successor cardinals.
For the consistency of the negative direction (ℵ2ℵω1)↛(ℵ0ℵω1)2 we invoke a result of Prikry.
An early paper of Prikry from [17] contains a forcing construction which proves the consistency of (ω1ω2)↛(ω1ω0)2.
The theorem generalizes to (ω1κ)↛(ω1ω0)2 for every regular uncountable κ.
The proof is exactly as in [17], and for completeness we unfold it upon replacing ω2 by κ.
Let us begin with the following:
Definition 1.2**.**
Prikry matrix.
Suppose that κ=cf(κ)≥ℵ2.
A (κ×ω1)-Prikry matrix is a family (Aα,η:α∈κ,η∈ω1) of subsets of ω1 satisfying the following properties:
- (ℵ)
For every α∈κ and ζ<η<ω1,Aα,ζ∩Aα,η=∅.
2. (ℶ)
For every α∈κ,⋃{Aα,η:η∈ω1}=ω1.
3. (ℷ)
For every {αn:n∈ω}⊆κ and every sequence (ηn:n∈ω)⊆ω1,∣ω1−⋃{Aαn,ηn:n∈ω}∣≤ℵ0.
We use the set notation {αn:n∈ω} to express the fact that m=n⇒αm=αn, and the sequence notation (ηn:n∈ω) to allow repetitions.
Claim 1.3**.**
If there is a (κ×ω1)-Prikry matrix then (ℵ1κ)↛(ℵ1ℵ0)2.
Proof.
Suppose that (Aα,η:α∈κ,η∈ω1) is a (κ×ω1)-Prikry matrix.
Define c:κ×ω1→2 by c(α,β)=0 iff β∈Aα,η and η is an even ordinal.
Assume that A∈[κ]ℵ0 and B∈[ω1]ℵ1.
Enumerate the elements of A by {αn:n∈ω}.
Fix an even ordinal η∈ω1 and an odd ordinal ζ∈ω1.
Since ∣ω1−⋃{Aαn,ηn:n∈ω}∣≤ℵ0 and ∣B∣=ℵ1 we can choose an ordinal β∈B∩⋃n∈ωAαn,η, so β∈Aαn,η for some n∈ω.
It follows that c(αn,β)=0.
Similarly one can choose an ordinal γ∈B∩⋃n∈ωAαn,ζ, so γ∈Aαm,η for some m∈ω.
It follows that c(αm,γ)=1.
We conclude, therefore, that A×B is c-polychromatic as desired.
\qed\refclmneg
Our next goal is to force a (κ×ω1)-Prikry matrix.
The forcing is identical with that of [17], upon replacing ℵ2 by κ.
Definition 1.4**.**
Prikry-matrix forcing.
Let κ=cf(κ)≥ℵ2.
A condition p∈P is a pair (S,F)=(Sp,Fp) such that:
- (i)
S⊆κ×ω1×ω1,∣S∣≤ℵ0.
2. (ii)
For every α∈κ,β∈ω1 there is at most one ordinal η∈ω1 such that (α,η,β)∈S.
3. (iii)
F is a function from dom(F) into ω1, where dom(F) is countable and the elements of dom(F) are functions f:dom(f)→ω1 so that dom(f)⊆κ and ∣dom(f)∣≤ℵ0.
4. (iv)
For every β∈ω1 if there are α∈κ,η∈ω1 such that (α,η,β)∈S then for every f∈dom(F) with F(f)≤β there exists α′∈dom(f) such that (α′,f(α′),β)∈S.
If p,q∈P then p≤q iff Sp⊆Sq and Fp⊆Fq.
The following lemma shows that forcing with P preserves cardinals.
Moreover, it implies that the forcing notion P satisfies stronger properties which are parallel to the requirements of Theorem 1.1.
Lemma 1.5**.**
Let κ=cf(κ)≥ℵ2 and let P be the associated Prikry-matrix forcing.
- (ℵ)
If p,q∈P and p∥q then r=(Sp∪Sq,Fp∪Fq) is a least upper bound for p and q.
2. (ℶ)
Likewise, if (pn:n∈ω) is ≤P-increasing then its union is a least upper bound. In particular, P is ℵ1-complete.
3. (ℷ)
P* is κ-Knaster.*
Proof.
The first two parts follow directly from the definition, and the last part follows from a Delta-system argument.
\qed\reflemknaster
Observe that for ℵ2 we conclude from the above lemma that the Prikry-matrix forcing satisfies the requirements in Theorem 1.1.
We shall define now some dense subsets of P.
For every pair (α,β)∈κ×ω1 let Dα,β={p∈P:∃η∈ω1,(α,η,β)∈Sp}.
For every function f which satisfies (iii) of Definition 1.4 we let Ef={p∈P:f∈dom(Fp)}.
Lemma 1.6**.**
*Let κ=cf(κ)≥ℵ2 and let P be the associated Prikry-matrix forcing.
Then Dα,β is a dense open subset of P for every (α,β)∈κ×ω1, and Ef is a dense open subset of P for every f which satisfies (iii) of Definition 1.4.*
Proof.
Directly from the definitions.
\qed\reflemdensity
We can prove now the following generalization of [17]:
Theorem 1.7**.**
*Assume that κ=cf(κ)≥ℵ2 and θω=θ for every θ<κ of uncountable cofinality.
Then one can force the existence a (κ×ω1)-Prikry matrix.*
Proof.
Let P be the Prikry-matrix forcing for κ.
Since P is ℵ1-complete, it adds no ω-subsets and hence θω=θ for every θ<κ of uncountable cofinality in the generic extension.
Let G⊆P be V-generic.
We shall argue that there exists a (κ×ω1)-Prikry matrix in V[G].
Let us describe the sets in our Prikry matrix.
For every α∈κ and every η∈ω1 define:
[TABLE]
We claim that {Aα,η:α∈κ,η∈ω1} is a Prikry matrix.
Clearly, Aα,η⊆ω1 for every α∈κ,η∈ω1.
Suppose that α∈κ and ζ<η<ω1.
Assume towards contradiction that Aα,ζ∩Aα,η=∅ and choose an ordinal β∈Aα,ζ∩Aα,η.
Choose p,q∈G such that p\Vdash\check{\beta}\in\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha,\zeta} and q\Vdash\check{\beta}\in\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha,\eta}.
Since G is directed we can find r∈G such that p,q≤r.
We conclude that r\Vdash\check{\beta}\in\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha\zeta}\cap\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha,\eta} and hence (α,ζ,β),(α,η,β)∈Sr.
This is impossible, however, since ζ=η and by virtue of Definition 1.4(ii).
Fix α∈κ and β∈ω1.
By Lemma 1.6 we can choose a condition p∈G∩Dα,β.
This means that (α,η,β)∈Sp and hence p\Vdash\check{\beta}\in\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha,\eta} for some η∈ω1.
We conclude, therefore, that V[G]⊨⋃η∈ω1Aα,η=ω1.
Finally, let
A
~
be a name of an element of [κ]ℵ0 and let
η
~
be a name of an ω-sequence of ordinals from ω1.
Fix a condition p which forces these facts.
We may assume that p forces that A={αn:n∈ω} and η=⟨ηn:n∈ω⟩, since P is ℵ1-complete so one can form an ω-increasing sequence of conditions above p, each of which forces a value to another element of A and η, and then take an upper bound.
Our goal is to find a condition r∈G and an ordinal γ∈ω1 such that r⊩∀β≥γ,β∈⋃{Aαn,ηn:n∈ω}.
To do this, we define a function f as follows.
We let dom(f)={αn:n∈ω} and f(αn)=ηn for every n∈ω.
We choose a condition q∈G∩Ef, so f∈dom(Fq), and we let γ=Fq(f).
Suppose that γ≤β∈ω1.
Choose an ordinal α∈κ and extend q to a condition r∈G∩Dα,β, so (α,η,β)∈Sq.
By Definition 1.4(iv) we see that (αn,f(αn),β)∈Sq for some n∈ω.
We see that r\Vdash\check{\beta}\in\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha_{n},f(\alpha_{n})}=\mathchoice{\oalign{\displaystyle A\crcr\vbox to0.86108pt{\hbox{\displaystyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\textstyle A\crcr\vbox to0.86108pt{\hbox{\textstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}{\oalign{\scriptscriptstyle A\crcr\vbox to0.86108pt{\hbox{\scriptscriptstyle{\tilde{\mkern-3.0mu}\mkern 3.0mu}{}}\vss}}}_{\alpha_{n},\eta_{n}}, so we are done.
\qed\refthmmt2
Based on Prikry’s result, we can show that the first part of [8, Problem 15] is independent of ZFC:
Theorem 1.8**.**
The polarized relation (ℵ2ℵω1)→(ℵ0ℵω1) is independent of ZFC.
Proof.
The positive direction of (ℵ2ℵω1)→(ℵ0ℵω1) follows from the stronger relation (ℵ0ℵω1)→(ℵ0ℵω1) by monotonicity.
This stronger relation holds if one forces Martin’s axiom with 2ω>ℵω1.
For the opposite direction, let us show that (ℵ2ℵω1)↛(ℵ0ℵω1) in Prikry’s model.
So we force as in [17] and we choose a coloring c:ω2×ω1→2 which exemplifies the negative relation (ℵ1ℵ2)↛(ℵ1ℵ0)2.
Fix an increasing and continuous sequence of cardinals ⟨μγ:γ∈ω1⟩ such that ωω1=⋃γ∈ω1μγ.
For every ordinal α∈ωω1 let γ(α) be the unique ordinal in ω1 such that μγ(α)≤α<μγ(α)+1.
Given α∈ωω1 and β∈ω2 we define d(α,β)=c(β,γ(α)).
Assume that A⊆ωω1,∣A∣=ℵω1 and B⊆ω2,∣B∣=ℵ0.
We claim that d↾(A×B) is not constant.
To see this notice that the set I={γ∈ω1:∃α∈A,γ(α)=γ} is of size ℵ1 since A is unbounded in ωω1.
By the choice of the coloring c we know that c↾(B×I) is not constant.
Pick up two pairs (β0,γ0),(β1,γ1)∈B×I such that c(β0,γ0)=0 and c(β1,γ1)=1.
Choose α0,α1∈A such that γ(α0)=γ0 and γ(α1)=γ1.
By definition, d(α0,β0)=c(β0,γ0)=0 and d(α1,β1)=c(β1,γ1)=1, so the proof is accomplished.
\qed\refthmehr15
As noted by one of the referees, a more general statement stands behind the above argument, and we phrase it for completeness:
Proposition 1.9**.**
*Let κ,λ and μ be cardinals.
Then (λκ)→(μκ)2 implies (λcf(κ))→(μcf(κ))2.*
Proof.
Assume that c:cf(κ)×λ→2 is a coloring.
Choose a continuous increasing sequence of cardinals (κi:i∈cf(κ)) so that κ=⋃i∈cf(κ)κi.
For every α∈κ there is a unique ordinal i∈cf(κ) such that κi≤α<κi+1, call it i(α).
Define a coloring d:κ×λ→2 by letting d(α,β)=c(i(α),β).
Since (λκ)→(μκ)2 one can find A∈[κ]κ,B∈[λ]μ so that d↾(A×B) is constantly ℓ for some ℓ∈{0,1}.
Let H={i(α):α∈A} and notice that ∣H∣=cf(κ) as A is unbounded in κ.
If γ∈H,β∈B then γ=i(α) for some α∈A and then c(γ,β)=c(i(α),β)=d(α,β)=ℓ.
Therefore, the product H×B exemplifies the relation (λcf(κ))→(μcf(κ))2 with respect to the coloring c.
Since c was arbitrary, we are done.
\qed\refpropreferee
It is interesting to compare statements over ω which can be forced by Martin’s axiom with parallel statements over ω1 under the generalized Martin’s axiom or Baumgartner’s axiom.
A systematic study in this direction is carried out in [21], and many applications of Martin’s axiom can be forced over higher cardinals.
The above theorem shows, however, that not everything is possible:
Corollary 1.10**.**
If one forces 2ω=ω1 and the generalized Martin’s axiom with 2ω1>ω2 then one obtains the negative relation (ℵ1ℵ2)↛(ℵ1ℵ0)2 and hence (ℵ1ℵ2)↛(ℵ1ℵ2)2.
Proof.
Let P be the Prikry-matrix forcing at ω2.
As mentioned before, it follows from Lemma 1.5 that P satisfies the requirements of Theorem 1.1.
Hence by forcing the generalized Martin’s axiom with 2ω1>ω2 we add a generic G⊆P which intersects every prescribed collection of ω2 dense sets.
This is sufficient for an (ω2×ω1)-Prikry matrix, so we are done.
\qed\refcorgma
We make the comment that strong positive relations of the form (ℵ1ℵ2)→A(ℵ1ℵ2)2 hold under the generalized Martin’s axiom when we take a certain collection of colorings determined by A, see [10, Theorem 2.5].
It is not clear whether a positive relation with finite sets at the large component is consistent with the generalized Martin’s axiom.
The positive relation (ℵ1ℵ2)→(ℵ12)ω has a considerable consistency strength, as proved by Donder and Levinski in [5].
Hence (ℵ1ℵ2)↛(ℵ12)ω is consistent with the generalized Martin’s axiom since it can be forced without large cardinals.
Donder and Levinski showed that (ℵ1ℵ2)→(ℵ12)ω implies (ℵ1ℵ2)→(ℵ1n)ω for every n∈ω, and a proof can be found in [4].
This invites for the following question:
Question 1.11**.**
Is it consistent that (ℵ1ℵ2)→(ℵ12)ω but (ℵ1ℵ2)↛(ℵ1ℵ0)ω?
2. Scales and saturated ideals
In this section we address the second part of [8, Problem 15] by showing that the relation (ℵ2ℵω1)→(ℵ1ℵω1)2 is independent.
The negative relation (ℵ2ℵω1)↛(ℵ1ℵω1)2 holds, for example, if one forces the generalized Martin’s axiom with 2ω1>ω2 using the results of the previous section and monotonicity.
For the consistency of the positive direction we shall need the following:
Definition 2.1**.**
Scattered families.
Assume that μ>cf(μ)=θ and let κ=μ+.
A family of sets A={Aα:α∈κ} will be called μ-scattered iff the following requirements are met:
- (α)
Aα⊆μ for every α∈κ.
2. (β)
∣Aα∣=θ for every α∈κ.
3. (γ)
If I∈[κ]κ and {aα:α∈I} satisfies aα⊆Aα,∣aα∣=θ for every α∈I then ∣⋃{aα:α∈I}∣=μ.
A scattered family will prove helpful when we try to lift polarized relations over a regular cardinal to the parallel relation with a singular cardinal sharing the same cofinality.
Claim 2.2**.**
Assume that:
- (a)
μ>cf(μ)=θ,κ=μ+,2θ<κ.
2. (b)
A={Aα:α∈κ}* is μ-scattered.*
3. (c)
χ<θ* and (θθ+)→(θθ)χ.*
*Then (θ+μ)→(θμ)χ.
If one assumes the stronger relation (θθ+)→(θθ+)χ and 2θ+<κ then one obtains the stronger conclusion (θ+μ)→(θ+μ)χ.*
Proof.
Let c:μ×θ+→χ.
For every α∈κ let cα=c↾(Aα×θ+).
Since (θθ+)→(θθ)χ which can also be written as (θ+θ)→(θθ)χ we see that for every α∈κ there are aα∈[Aα]θ and bα∈[θ+]θ such that cα↾(aα×bα) is homogeneous with the color iα∈χ.
Since κ=cf(κ)>2θ and χ<θ we see that there are I∈[κ]κ,b∈[θ+]θ and a fixed i∈χ such that α∈I⇒bα=b∧iα=i.
Let a=⋃{aα:α∈I} and notice that ∣a∣=μ since A is μ-scattered.
We claim that c↾(a×b) is constantly i.
To see this, suppose that σ∈a and τ∈b.
Choose α∈κ such that σ∈aα.
It follows that c(σ,τ)=cα(σ,τ)=iα=i and hence (θ+μ)→(θμ)χ.
Moreover, if one assumes that the stronger relation (θθ+)→(θθ+)χ holds then the same argument yields (θ+μ)→(θ+μ)χ, but we need 2θ+<κ in order to unify the bαs into the same b, thus the proof is accomplished.
\qed\refclmscattered
Our next objective is to show that scattered families exist.
We need a few basic concepts from pcf theory.
Suppose that μ>cf(μ)=θ and (μγ:γ∈θ) is an increasing sequence of regular cardinals such that μ=⋃γ∈θμγ.
If f,g∈∏γ∈θμγ and J is an ideal over θ then we shall say that f<Jg iff {γ∈θ:g(γ)≤f(γ)}∈J.
Usually, our ideal J will be Jθbd, the ideal of bounded subsets of θ.
A scale (fα:α∈κ) in the product (∏γ∈θμγ,J) is a sequence of elements of ∏γ∈θμγ such that α<β⇒fα<Jfβ and for every h∈∏γ∈θμγ there is an ordinal α∈κ such that h<Jfα.
By a fundamental theorem of Shelah’s pcf theory, if μ>cf(μ)=θ and κ=μ+ then there exists an increasing sequence (μγ:γ∈θ) of regular cardinals such that μ=⋃γ∈θμγ and there is a scale (fα:α∈κ) in (∏γ∈θμγ,Jθbd).
A proof can be found in [19] or in [1, Theorems 2.23 and 2.26].
Proposition 2.3**.**
If μ is a singular cardinal then there exists a μ-scattered family.
Proof.
Let θ=cf(μ) and κ=μ+.
Choose an increasing sequence (μγ:γ∈θ) of regular cardinals such that μ=⋃γ∈θμγ.
Let (fα:α∈κ) be a scale in (∏γ∈θμγ,Jθbd).
For every α∈κ let Aα=rang(fα), so Aα⊆μ for every α∈κ.
Without loss of generality the range of each fα is unbounded in μ and hence ∣Aα∣=θ for every α∈κ.
Fix a set I∈[κ]κ and a collection {aα:α∈I} so that aα∈[Aα]θ for every α∈I.
Let a=⋃{aα:α∈I}.
If there is a set y∈[θ]θ such that ∣a∩μγ∣=μγ for every γ∈y then ∣a∣=∣⋃γ∈yμγ∣=μ and we are done.
By way of contradiction assume that no such y exists.
Hence there is an ordinal γ0∈θ such that γ∈(γ0,θ)⇒ηγ=sup(a∩μγ)<μγ.
Define h∈∏γ∈θμγ by h(γ)=0 when γ≤γ0 and h(γ)=ηγ when γ>γ0.
Choose an ordinal α∈I such that h<Jθbdfα.
For some δ0∈θ we see that if δ0≤δ<θ then h(δ)<fα(δ).
Since Aα=rang(fα) and aα is unbounded in Aα we can choose a sufficiently large δ so that γ0<δ<θ and h(δ)<fα(δ)∈aα.
However, sup(aα∩μδ)≤sup(a∩μδ)=ηδ=h(δ)<fα(δ), a contradiction.
\qed\refpropscattexist
Recall that if Martin’s axiom holds and 2ω>ω1 then (ωω1)→(ωω1)2.
If θ is supercompact then one can force sθ>θ+ and obtain (θθ+)→(θθ+)2.
For this result see [12, Theorem 2.4], which is based on [11, Claim 1.2].
If θ is a successor of a regular cardinal and there exists a huge cardinal above θ then one can force (θθ+)→(θθ)2, see [10, Theorem 3.2].
These facts justify the following:
Proposition 2.4**.**
Assume that μ>cf(μ)=θ.
- (ℵ)
If θ=ℵ0 or θ is supercompact then one can force (θ+μ)→(θμ)2.
2. (ℶ)
If θ is a successor of a regular cardinal and there is a huge cardinal above θ then one can force (θ+μ)→(θμ)2.
3. (ℷ)
In particular, if there is a huge cardinal then one can force the relation (ℵ2ℵω1)→(ℵ1ℵω1)2.
Proof.
Begin with a singular cardinal μ>cf(μ)=θ so that 2θ<μ (or even 2θ+<μ for a stronger conclusion).
Such a cardinal satisfies part (a) of Claim 2.2, and part (b) follows from Proposition 2.3.
Part (c) can be forced as described in the paragraph before the statement of this proposition.
Applying Claim 2.2 we are done.
\qed\refcorehr15
Along with the results of the previous section we obtain a full answer to the original question of [8].
One may wonder, however, if the strongest relation (ℵ2ℵω1)→(ℵ2ℵω1)2 is provably false in ZFC.
We shall discuss such relations in the next section, but we drop the axiom of choice in order to obtain strong positive relations.
3. Strong relations without choice
The possible consistency of (ℵ1ℵ2)→(ℵ1ℵ2)2 with ZFC is still open.
However this positive relation is provable under the axiom of determinacy, and more is provable under the additional assumption that V=L(R).
Other variations of the polarized relation under AD appear in the literature, see e.g. [2].
We shall also use determinacy in order to address the cube problem, which formally is still open in ZFC.
Theorem 3.1**.**
Assume AD.
- (ℵ)
(ℵ1ℵ2)→(ℵ1ℵ2)2ℵ0.
2. (ℶ)
(ℵ2ℵ1ℵ0)→(ℵ2ℵ1ℵ0)n* for every n∈ω.*
3. (ℷ)
If one assumes AD+V=L(R) then
(ℵ2μ)→(ℵ2μ)2ℵ0 for some μ>cf(μ)=ω1.
Proof.
Recall that ℵ1 and ℵ2 are measurable under AD, as proved first by Solovay.
Likewise, ACℵ0 holds under AD, and we shall use these facts below.
We shall prove a general claim which will be helpful for all three statements.
Fix an ℵ1-complete ultrafilter U over ℵ1 and an ℵ2-complete ultrafilter V over ℵ2.
The claim is that if we are given a sequence (cn:n∈ω) where cn:ω2×ω1→2 for every n∈ω then there are A∈V,B∈U so that cn↾(A×B) is constant for every n∈ω simultaneously.
Suffice it to prove that for every n∈ω there are An∈V,Bn∈U so that cn↾(An×Bn) is constantly in for some in∈{0,1}.
Indeed, if we prove this statement then we can define A=⋂{An:n∈ω} and B=⋂{Bn:n∈ω}.
Thus we have A∈V,B∈U by the completeness of these ultrafilters.
But now we see that cn↾(A×B) is constantly in for every n∈ω simultaneously.
Remark that we use here ACℵ0, as we must choose An and Bn, but ACℵ0 is at our disposal under AD.
So fix n∈ω and focus on the coloring cn.
For every β∈ω1 let jβ∈{0,1} be such that Sβjβ={α∈ω2:cn(α,β)=jβ}∈V.
For some Bn∈U and a fixed in∈{0,1} we will have β∈Bn⇒jβ=in.
Define An=⋂{Sβin:β∈Bn}, and conclude that An∈V by ℵ2-completeness.
Now cn↾(An×Bn) is constantly in as desired.
We proceed to part (ℵ) of our theorem.
We may identify 2ℵ0 with the collection of ω-sequences of [math] and 1, so assume that c:ω2×ω1→ω2 is given.
For every n∈ω let cn:ω2×ω1→2 be the nth place of c, to wit cn(α,β) is the nth place in the sequence c(α,β) for every α∈ω2,β∈ω1.
Let A∈V,B∈U be such that cn′′(A×B)={in} for every n∈ω.
Here we use the general claim proved above.
Let η=(in:n∈ω), so η∈ω2.
By definition, c↾(A×B) is constantly η, so the first statement of the theorem is proved.
Part (ℶ) is basically the same.
For notational simplicity we focus on the case in which n=2, the general proof for every n∈ω is just the same.
We are given now a coloring d:ω2×ω1×ω→2.
For every n∈ω we define dn:ω2×ω1→2 by letting dn(α,β)=d(α,β,n).
For every n∈ω there are An∈V,Bn∈U and in∈{0,1} so that cn′′(An×Bn)={in}.
Let C∈[ω]ω be such that n∈C⇒in=i for some fixed i∈{0,1}.
Finally, let A=⋂n∈CAn,B=⋂n∈CBn so A∈V and B∈U.
One can verify that d↾(A×B×C) is constantly i, so the second part has been established.
Finally, we wish to prove that (ℵ2μ)→(ℵ2μ)2ℵ0 under AD+V=L(R) for some μ>cf(μ)=ω1.
Suffice it to prove that (ℵ2μ)→(ℵ2μ)2 since then we can use ACω to get 2ℵ0 colors by the general claim from the beginning of the proof.
We emphasize that the strengthening to 2ℵ0 colors using the general claim is based on the fact that ℵ1 is measurable, which is correct under AD+V=L(R).
Recall that under AD+V=L(R) one can prove that Θ is regular, and it is a limit of measurable cardinals.
In fact, if κ<Θ is regular then κ is measurable.
Moreover, for every such κ the filter generated by the ω-closed unbounded subsets of κ is a κ-complete ultrafilter over κ.
A proof of all these facts appears in [20, Theorem 8.27].
Let (κα:α∈ω1) be an increasing sequence of measurable cardinals and let μ=⋃α∈ω1κα.
Notice that μ>cf(μ)=ω1.
We claim that (ℵ2μ)→(ℵ2μ)2.
To see this, suppose that c:μ×ω2→2 is a coloring.
Let U be an ℵ2-complete ultrafilter over ℵ2.
For every α∈ω1 let cα=c↾(κα×ω2).
For every α∈ω1 let Wα be the ultrafilter generated by the ω-closed unbounded subsets of κα.
As in the first part of the proof, let (Aα,Bα,iα) be so that Aα∈Wα,Bα∈U,iα∈{0,1} and cα↾(Aα×Bα) is constantly iα.
Observe that the triple (Aα,Bα,iα) is determined by the coloring c and by the ultrafilters, so we do not use choice while creating the sequence ⟨(Aα,Bα,iα):α∈ω1⟩.
Fix a set I⊆ω1,∣I∣=ℵ1 and i∈{0,1} such that α∈I⇒iα=i.
Define A=⋃{Aα:α∈I} and B=⋂{Bα:α∈I}.
Notice that ∣A∣=μ and B∈U since U is ℵ2-complete.
In particular, ∣B∣=ℵ2.
One can verify that c′′(A×B)={i}, so the proof is accomplished.
\qed\refthmadcube
The above theorem shows that (ℵ2μ)→(ℵ2μ)2 is independent over ZF for some μ>cf(μ)=ω1, where the positive direction has been proved in models without choice and the negative direction holds in models of ZFC.
For example, the model of the generalized Martin’s axiom with 2ω1>ω2 satisfies the negative relation.
We indicate, however, that the negative relation may hold even if the axiom of choice fails.
Indeed, all the relations of Theorem 3.1 fail in Gitik’s model [13], as every uncountable cardinal has countable cofinality in this model.
The number of colors in the above theorem is optimal.
The trivial example of c:ω2×ω1→ω1 defined by c(α,β)=β shows that one cannot improve 2ℵ0 to ω1 in the first statement.
Similarly, one cannot get infinitely many colors in the second part (though the statement holds with every finite number of colors).
Finally, by slicing μ>cf(μ)=ω1 to ω1-many segments, each of which is of size less than μ, one can show that (ℵ2μ)↛(ℵ2μ)ω1.
Ahead of dealing with the cube problem, we raise the possibility that the last part of the above theorem holds at μ=ℵω1.
It is not clear whether one can prove (ℵ2ℵω1)→(ℵ2ℵω1)2 under AD, but it seems that one can obtain this relation in ZF using the methods of [3].
For this end, one has to force ℵα+1 to be measurable for every countable limit ordinal α∈ω1, along with DCℵ1 and ℵ2 being measurable.
Unlike AD in which we know who is the normal ultrafilter (so there is no need to choose it), if we force with the method of [3] we must choose our measurable ultrafilter over each ℵα+1, and hence DCℵ1 is needed.
Question 3.2**.**
Is it consistent relative to ZF that (ℵ2ℵω1)→(ℵ2ℵω1)2?
We move now to the cube problem.
The cube version of the polarized relation is denoted by (αβγ)→(δεζ)θ and stipulates that for every coloring c:α×β×γ→θ there are A⊆α,B⊆β and C⊆γ such that otp(A)=δ,otp(B)=ε,otp(C)=γ and c↾(A×B×C) is constant.
Positive cube relations seem harder to achieve than the parallel relations applied to pairs.
In particular, it is unknown whether (ℵ1ℵ1ℵ1)→(ℵ0ℵ0ℵ0)2 is consistent.
In this case, it is also unknown whether the corresponding negative (ℵ1ℵ1ℵ1)↛(ℵ0ℵ0ℵ0)2 is consistent.
This problem is labeled as Question 28 in [6], and it appears in the generalized form as to whether (κ+κ+κ+)→(κκκ)2 in [23, p. 110].
As noted by one of the referees, the status of this Question in ZFC is somewhat vague. It is claimed in several places that the answer is negative in ZFC, e.g. [22], [7] and [16, Chapter 4].
However, no formal proof is available.
We shall try to prove positive instances of the cube relation under AD.
More precisely, we need the fact that κ+ is a measurable cardinal and this holds at many places under determinacy assumptions, though it can also be forced without determinacy.
Theorem 3.3**.**
*if κ+ is measurable then (κ+κ+κ+)→(κκκ)2.
Moreover, (κ+κ+κ+)→(κκκ+)2.*
Proof.
We prove the second statement, which of course implies the first one.
For this end, let U be a κ+-complete ultrafilter over κ+.
We define U2 over κ+×κ+ as follows.
If S⊆κ+×κ+ and β∈κ+ then we let Sβ={γ∈κ+:(β,γ)∈S}.
Now we define S∈U2 iff {β∈κ+:Sβ∈U}∈U.
It is routine to check that U2 is an ultrafilter and it is κ+-complete.
Suppose that c:κ+×κ+×κ+→2 is a coloring.
For every α∈κ+,i∈{0,1} let Sαi={(β,γ):c(α,β,γ)=i}.
Notice that (Sα0,Sα1) is a partition of κ+×κ+ for every α∈κ+.
Hence for each α∈κ+ there is a unique i(α)∈{0,1} such that Sαi(α)∈U2.
Consequently, there is a set A⊆κ+,∣A∣=κ+ and there is a fixed color i∈{0,1} such that α∈A⇒i(α)=i.
Choose a∈[A]κ.
For every α∈a let Bαi={β∈κ+:(Sαi)β∈U}, so Bαi∈U.
Define B=⋂{Bαi:α∈a} and conclude that B∈U since U is κ+-complete.
Choose b∈[B]κ and define E=⋂{(Sαi)β:α∈a,β∈b}.
Again, E∈U so in particular ∣E∣=κ+.
Let us show that c′′(a×b×E)={i}.
Indeed, if α∈a,β∈b and γ∈E then γ∈(Sαi)β.
By the definition of these sets we see that (β,γ)∈Sαi.
By the definition of the coloring we see that c(α,β,γ)=i, so the proof is accomplished.
\qed\refthmcube
We can derive the following:
Corollary 3.4**.**
*Assume AD.
Then (ℵ1ℵ1ℵ1)→(ℵ0ℵ0ℵ1)2 and (ℵω+1ℵω+1ℵω+1)→(ℵωℵωℵω+1)2.*
\qed\refcorad
Remark that similar statements can be proved for n-copies of the same measurable cardinal where 3<n∈ω, using Un−1 instead of U2.
Likewise, the order type of the first two components can be a bigger ordinal since we can choose a,b such that otp(a),otp(b)≥δ for every δ∈κ+.
So actually we have, under AD and in these parameters, the optimal cube relation (ℵ1ℵ1ℵ1)→(ττℵ1)2 for every τ∈ω1.
Naturally, there are other interesting questions in the vicinity of the above results. Questions with infinite exponent were studies under AD in our context, see [2].
One of the referees posed an interesting question which lurks right around the corner, and we conclude the paper with an answer which shows the discrepancy between AD and weak fragments of choice.
Theorem 3.5**.**
Under AD we have (ω1ω1ω)→(ω1τω)m for every m∈ω and every τ∈ω1, but if ACℵ1 holds then (ω1ω1ω)↛(ω1ωω)2.
Proof.
For the first statement all we need is just the measurability of ℵ1, so under AD we can use Solovay’s theorem.
Let U be an ℵ1-complete ultrafilter over ℵ1.
For simplicity we assume that m=2 and we indicate that the proof works at any finite number of colors.
Fix a countable ordinal τ∈ω1.
For every n∈ω let cn=c↾ω1×ω1×{n}, so one can think of cn as a function from ω1×ω1 into {0,1}.
For every n∈ω and for every β∈ω1 there is iβn∈{0,1} such that Aβn={α∈ω1:cn(α,β)=iβn}∈U.
Hence for each n∈ω there is a set Bn∈U and some in∈{0,1} for which β∈Bn⇒iβn=in.
For m=n it is possible that im=in, but one can find a set C∈[ω]ω and a fixed i∈{0,1} so that n∈C⇒in=i.
Let B=⋂n∈ωBn, so B∈U by ℵ1-completeness.
Let Bτ be the set which consists of the first τ elements of B.
Define A=⋂{Aβn:n∈C,β∈Bτ} and notice again that A∈U since U is ℵ1-complete.
If α∈A,β∈Bτ and n∈C then c(α,β,n)=cn(α,β)=iβn since A⊆Aβn.
But iβn=in since β∈Bτ⊆B⊆Bn and in=i since n∈C.
Therefore, c↾(A×B×C) is constantly i, as desired.
To appreciate the above result suppose that ACℵ1 holds and choose a one-to-one function gτ:τ→ω for every τ∈ω1.
We define c:ω1×ω1×ω→2 as follows.
Given α,β∈ω1 we let τ=τα,β=max{α,β} and σ=σα,β=min{α,β}.
Now if α,β∈ω1 and n∈ω we define c(α,β,n)=0 iff σ<τ and gτ(σ)≤n.
Suppose that A∈[ω1]ω1,B∈[ω1]ω and C∈[ω]ω.
Choose α∈A and β∈B such that α>β.
Let ℓ=gα(β).
Since C is unbounded in ω one can find n∈C so that n≥ℓ and then c(α,β,n)=0.
Now fix α∈A such that α>sup(B).
For every β∈B we have τα,β=α and hence σα,β=β.
Fix n∈C.
Since gα:α→ω is one-to-one, the set {gα(β):β∈B} is an infinite subset of ω.
Hence one can find β∈B for which gα(β)>n and then c(α,β,n)=1.
The negative relation is, therefore, established.
\qed\refthmrefereeq