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On a problem of Erdos and Hajnal

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Abstract

We address a question of Erdős and Hajnal about the ordinary partition relation ℵω+1↛(ℵω+1,(3)ℵ0)2\aleph_{ω+1}\nrightarrow(\aleph_{ω+1},(3)_{\aleph_0})^2. For θ=cf(λ)<λθ=\mathrm{cf}(λ)<λ, assuming 2λ=λ+2^λ=λ^+ they proved the negative relation λ+↛(λ+,(3)θ)2λ^+\nrightarrow(λ^+,(3)_θ)^2 and asked whether the (local instance of) GCH is indispensable. We show that this negative relation is consistent with λλ being a strong limit and 2λ>λ+2^λ>λ^+. The result can be pushed down to ℵω\aleph_ω.

2010 Mathematics Subject Classification. 03E02, 03E04, 03E55.

The research was supported by Israel Science Foundation Grant no. 1838/19 and Grant no. 2320/23. The second author’s research was supported by the Israel Science Foundation Grant no. 1963/21. This is publication 1249 (the 204th prime number) of the third author, publication 47 (the 15th prime number) of the first author and publication 37 (the 12th prime number) of the second author.

Introduction

Let G=(V,E)G=(V,E) be a graph of size λ\lambda. One may wonder whether there must be a monochromatic triangle under any edge coloring c:E→θc:E\to\theta. The answer is trivially no, since the graph can be a set of isolated vertices with no edges at all, or a triangle-free graph. Thus in order to make the above question interesting, one should assume that there are many edges (and, in particular, many triangles) in the graph. One possible way to do it uses the following concept. A set of vertices W⊆VW\subseteq V is called independent if [W]2∩E=∅[W]^2\cap E=\varnothing. If GG is of size λ\lambda and there are no independent subsets of size λ\lambda in GG, then there are many edges in the graph and the question makes more sense.

The above discussion can be formulated in the language of partition calculus, without mentioning graphs at all. The ordinary partition relation λ→(κ,(3)θ)2\lambda\to(\kappa,(3)_\theta)^2 says that for every coloring c:[λ]2→θc:[\lambda]^2\to\theta there is either A∈[λ]κA\in[\lambda]^\kappa so that c′′[A]2={0}c^{\prime\prime}[A]^2=\{0\}, or B∈[λ]3B\in[\lambda]^3 and γ∈(0,θ)\gamma\in(0,\theta) so that c′′[B]2={γ}c^{\prime\prime}[B]^2=\{\gamma\}. A particularly interesting case is when κ=λ\kappa=\lambda. In terms of graph theory, one can interpret the coloring as assigning zero to pairs of vertices with no edge, and some color γ∈(0,θ)\gamma\in(0,\theta) to edges of a given graph. The positive relation λ→(λ,(3)θ)2\lambda\to(\lambda,(3)_\theta)^2 means that either there is an independent set of size λ\lambda, or a monochromatic triangle.

Erdős, Hajnal and Rado investigated this relation in [10]. They established several results, and focused in particular on graphs whose size is a successor of a singular cardinal. A good account appears in the monograph [EHMR84], in which the following is phrased and proved:

Theorem 0.1. Assume that λ\lambda is a singular cardinal and 2λ=λ+2^\lambda=\lambda^+. Then λ+↛(λ+,(3)cf⁡(λ))2\lambda^+\nrightarrow(\lambda^+,(3)_{\operatorname{cf}(\lambda)})^2.

Actually, they proved something a bit stronger, see [EHMR84], Theorem 20.2. A natural question is whether the assumption 2λ=λ+2^\lambda=\lambda^+ is removable. Let us indicate that if one forces 2cf⁡(λ)≥λ+2^{\operatorname{cf}(\lambda)}\geq\lambda^+ then a negative result obtains, namely λ+↛(λ+,(3)cf⁡(λ))2\lambda^+\nrightarrow(\lambda^+,(3)_{\operatorname{cf}(\lambda)})^2, as mentioned in [EHMR84]. Thus we shall assume from now on that 2cf⁡(λ)<λ2^{\operatorname{cf}(\lambda)}<\lambda, and in fact we shall force the negative relation while λ\lambda is a strong limit singular cardinal. The first case, in this context, is λ=ℵω\lambda=\aleph_\omega. In a collection of unsolved problems [8], Problem 5, the pertinent question appears as follows:

Question 0.2. Can one prove without assuming GCH that the relation ℵω+1↛(ℵω+1,(3)ℵ0)2\aleph_{\omega+1}\nrightarrow(\aleph_{\omega+1},(3)_{\aleph_0})^2 holds?

It appeared, again, in [EHMR84], Problem 20.1.1 Despite the fact that powerful methods for dealing with successors of singular cardinals are available today, the problem is still open. A recent survey by Komjáth, [Kom25], describes the progress in every problem from the list of Erdős and Hajnal, and according to this survey no progress has been made with regard to this problem. In this paper we intend to show that λ+↛(λ+,(3)cf⁡(λ))2\lambda^+ \nrightarrow(\lambda^+,(3)_{\operatorname{cf}(\lambda)})^2 is consistent with 2λ>λ+2^\lambda> \lambda^+, where λ\lambda is singular and strong limit. The current status of the question is, therefore, as follows. The negative relation is consistent with the failure of GCH, but we do not know whether it holds in ZFC.

Our strategy is to replace the hypothesis 2λ=λ+2^\lambda= \lambda^+ by pcf arguments. More specifically, we obtain unbounded sequences of regular cardinals below λ\lambda that satisfy some relevant negative arrow relation, and we make sure that the true cofinality of these sequences is λ+\lambda^+. These assumptions enable us to lift the negative relations below λ\lambda to λ+\lambda^+, even if 2λ>λ+2^\lambda> \lambda^+.

This approach is rendered here twice. Firstly, we get the negative arrow relation λi+↛(λi+,(3)cf⁡(λi))2\lambda_i^+ \nrightarrow(\lambda_i^+,(3)_{\operatorname{cf}(\lambda_i)})^2 where each λi\lambda_i is a successor of a singular cardinal, simply by assuming GCH below λ\lambda, and then we lift this relation to λ+\lambda^+. The drawback here is that λ\lambda must be a limit of singular cardinals with the same cofinality. Namely, the cofinality of λ\lambda should be the cofinality of every element in the chosen sequence of singular cardinals which tend to λ\lambda. Thus ℵω\aleph_\omega cannot be handled in this way. Secondly, we modify the negative arrow relation over each λi\lambda_i in such a way that it applies to regular cardinals even though these cardinals are not successors of singular cardinals. This strategy applies to small cardinals like the ℵn\aleph_n’s, and consequently the negative arrow relation can be forced over ℵω\aleph_\omega.

There is another possible approach towards the same negative arrow relation. This approach is based on prediction principles from the tiltan family. Suppose that diamond holds at λ+\lambda^+, in which case 2λ=λ+2^\lambda= \lambda^+. In many cases, diamond can be replaced by weaker prediction principles like tiltan or stick. The version employed in this paper is ♣(λ)\clubsuit(\lambda), and it says that there exists a sequence (Aα∣α∈λ+)(A_\alpha\mid\alpha\in\lambda^+) of elements of [λ+]λ[\lambda^+]^\lambda that guesses every A∈[λ+]λ+A \in[\lambda^+]^{\lambda^+} in the sense that Aα⊆AA_\alpha\subseteq A. Usually, these principles at λ+\lambda^+ are consistent with 2λ>λ+2^\lambda> \lambda^+. We shall prove that ♣(λ)\clubsuit(\lambda) yields the negative arrow relation λ+↛(λ+,(3)cf⁡(λ))2\lambda^+ \nrightarrow(\lambda^+,(3)_{\operatorname{cf}(\lambda)})^2. However, we do not know whether ♣(λ)\clubsuit(\lambda) is consistent with 2λ>λ+2^\lambda> \lambda^+ when λ\lambda is a strong limit singular cardinal. Recall that in ♣(λ)\clubsuit(\lambda) the size of the guessing sets is λ\lambda, and this is the main problematic issue in our context. This point will be discussed in the relevant section.

The rest of the paper contains three additional sections, and an appendix. In the first section we solve the general problem using simple arguments of pcf theory. As mentioned above, this solution does not cover the case of ℵω\aleph_\omega. In the second section we modify the pcf arguments and show how to push down the result to ℵω\aleph_\omega. Finally, in the third section we show that a special version of stick at λ+\lambda^+ yields the desired negative arrow relation. The appendix is devoted to a formal proof of the strong Prikry property with respect to the Extender-based Prikry forcing with collapses, the one that we use in our proofs.

Our notation is coherent with [EHM R84]. We shall use the Jerusalem forcing notation, namely we force upwards. A function f:E→P(E)f:E\to\mathcal{P}(E) is a set mapping if x∉f(x)x \notin f(x) whenever x∈Ex \in E. A subset X⊆EX \subseteq E is free for ff iff f(y)∩X=∅f(y) \cap X = \varnothing whenever y∈Xy \in X. If κ=cf⁡(κ)<λ\kappa= \operatorname{cf}(\kappa) < \lambda then we let Sκλ={δ∈λ∣cf⁡(δ)=κ}S^\lambda_\kappa= \{\delta\in\lambda\mid\operatorname{cf}(\delta) = \kappa\}. If ℵ0<cf⁡(λ)\aleph_0 < \operatorname{cf}(\lambda) then SκλS^\lambda_\kappa is a stationary subset of λ\lambda. A cardinal κ\kappa is γ\gamma-supercompact if there exists an elementary embedding j:V→Mj : V \to M such that κ=crit⁡(j)\kappa= \operatorname{crit}(j) and γM⊆M{}^{\gamma}M \subseteq M. One says that κ\kappa is supercompact if κ\kappa is γ\gamma-supercompact for every ordinal γ\gamma.

Supercompactness can be characterized by the following (global) property. Suppose that κ≤λ\kappa\leq\lambda. An ultrafilter U\mathcal{U} over Pκλ\mathcal{P}_\kappa\lambda is fine if {x∈Pκλ∣α∈x}∈U\{x \in\mathcal{P}_\kappa\lambda\mid\alpha\in x\} \in\mathcal{U} whenever α∈λ\alpha\in\lambda. One says that U\mathcal{U} is normal if every ∈\in-regressive function on a set AA from U\mathcal{U} is constant on a set B⊆AB \subseteq A, B∈UB \in\mathcal{U}. Using these definitions, κ\kappa is λ\lambda-supercompact if there exists a fine and normal measure over Pκλ\mathcal{P}_\kappa\lambda, and κ\kappa is supercompact if κ\kappa is λ\lambda-supercompact for every λ≥κ\lambda\geq\kappa.

We shall use the idea of indestructibility (at supercompact cardinals) as appeared in the seminal work of Laver, [20]. It is shown there that a supercompact cardinal κ\kappa can be made indestructible under any generic extension by κ\kappa-directed-closed forcing notions. In our context, we need a modification of Laver’s proof, applicable to strategically-closed forcing notions. This version will be phrased and proved below.

For basic background concerning Prikry type forcings we refer to [13], and to the papers of Magidor [21] and [22] in which the basic method of Prikry forcing with interleaved collapses was introduced. We also refer to [Hay23] in this context. For background in pcf theory we suggest [1], [4] and [She94].

A negative relation from simple pcf arguments

In this section we suggest our first approach for proving the negative relation λ+↛(λ+,(3)cf⁡(λ))2\lambda^{+} \nrightarrow(\lambda^{+},(3)_{\operatorname{cf}(\lambda)})^{2} where λ\lambda is a strong limit singular cardinal and 2λ>λ+2^{\lambda} > \lambda^{+}. The idea is to assume the negative relation at an unbounded sequence of cardinals below λ\lambda (by assuming GCH at these cardinals) and to obtain the negative relation at λ+\lambda^{+} by means of pcf theory.

Let J\mathcal{J} be an ideal over θ\theta, and let (λi∣i∈θ)(\lambda_i \mid i \in\theta) be a sequence of regular cardinals. Let (fα∣α∈μ)(f_{\alpha} \mid\alpha\in\mu) be a sequence of functions in ∏i∈θλi\prod_{i \in\theta}\lambda_i. One says that this sequence is J\mathcal{J}-increasing if {i∈θ∣fα(i)≥fβ(i)}∈J\{i \in\theta\mid f_{\alpha}(i) \ge f_{\beta}(i)\} \in\mathcal{J} whenever α<β<μ\alpha< \beta< \mu. The sequence is cofinal if for every g∈∏i∈θλig \in\prod_{i \in\theta}\lambda_i there exists α∈μ\alpha\in\mu so that g≤Jfαg \le_{\mathcal{J}} f_{\alpha}. Occasionally, J\mathcal{J} will be the ideal of bounded subsets of θ\theta, denoted Jθbd\mathcal{J}^{\mathrm{bd}}_{\theta}. Recall that tcf⁡(∏i∈θλi,J)=κ\operatorname{tcf}(\prod_{i \in\theta}\lambda_i,\mathcal{J}) = \kappa iff there is a J\mathcal{J}-cofinal and increasing sequence in the product ∏i∈θλi\prod_{i \in\theta}\lambda_i, and κ\kappa is the minimal length of such a sequence. We commence with the combinatorial theorem, followed by a description of the ways to force the assumptions in this theorem.

References

  1. [1]Uri Abraham and Menachem Magidor. Cardinal arithmetic. In Handbook of set theory. Vols. 1, 2, 3, pages 1149–1227. Springer, Dordrecht, 2010.DOI
  2. [2]Hosea Ben Be’eri. The book of Hosea. In Prophets. 727 B.C.E.
  3. [3]Tom Benhamou, Shimon Garti, and Alejandro Poveda. Negating the Galvin property. J. Lond. Math. Soc. (2), 108(1):190–237, 2023.
  4. [4]Maxim R. Burke and Menachem Magidor. Shelah’s pcf theory and its applications. Ann. Pure Appl. Logic, 50(3):207–254, 1990.
  5. [5]William Chen, Shimon Garti, and Thilo Weinert. Cardinal characteristics of the continuum and partitions. Israel J. Math., 235(1):13–38, 2020.DOI
  6. [6]James Cummings. A model in which GCH holds at successors but fails at limits. Trans. Amer. Math. Soc., 329(1):1–39, 1992.
  7. [7]James Cummings. Iterated forcing and elementary embeddings. In Handbook of set theory. Vols. 1, 2, 3, pages 775–883. Springer, Dordrecht, 2010.DOI
  8. [8]P. Erdős and A. Hajnal. Unsolved problems in set theory. In Axiomatic Set Theory (Proc. Sympos. Pure Math., Vol. XIII, Part I, Univ. California, Los Angeles, Calif., 1967), pages 17–48. Amer. Math. Soc., Providence, R.I., 1971.DOI
  9. [10]P. Erdős, A. Hajnal, and R. Rado. Partition relations for cardinal numbers. Acta Math. Acad. Sci. Hungar., 16:93–196, 1965.DOI
  10. [11]Moti Gitik. The negation of the singular cardinal hypothesis from o(κ) = κ⁺⁺. Ann. Pure Appl. Logic, 43(3):209–234, 1989.DOI
  11. [12]Moti Gitik. The strength of the failure of the singular cardinal hypothesis. Ann. Pure Appl. Logic, 51(3):215–240, 1991.DOI
  12. [13]Moti Gitik. Prikry-type forcings. In Handbook of set theory. Vols. 1, 2, 3, pages 1351–1447. Springer, Dordrecht, 2010.DOI
  13. [14]Moti Gitik. On density of old sets in Prikry type extensions. Proc. Amer. Math. Soc., 145(2):881–887, 2017.DOI
  14. [15]Moti Gitik. Private communication. 2025.
  15. [16]Shimon Garti and Saharon Shelah. A strong polarized relation. J. Symbolic Logic, 77(3):766–776, 2012.DOI
  16. [18]András Hajnal and Attila Máté. Set mappings, partitions, and chromatic numbers. In Logic Colloquium ’73 (Bristol, 1973), volume Vol. 80 of Stud. Logic Found. Math., pages 347–379. North-Holland, Amsterdam-Oxford, 1975.DOI
  17. [20]Richard Laver. Making the supercompactness of κ indestructible under κ-directed closed forcing. Israel J. Math., 29(4):385–388, 1978.DOI
  18. [21]Menachem Magidor. On the singular cardinals problem. I. Israel J. Math., 28(1-2):1–31, 1977.DOI
  19. [22]Menachem Magidor. On the singular cardinals problem. II. Ann. of Math. (2), 106(3):517–547, 1977.DOI
  20. [23]Carmi Merimovich. Mathias like criterion for the extender based Prikry forcing. Ann. Pure Appl. Logic, 172(9):Paper No. 102994, 6, 2021.DOI
  21. [24]A. J. Ostaszewski. On countably compact, perfectly normal spaces. J. London Math. Soc. (2), 14(3):505–516, 1976.DOI

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