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The Continuum Hypothesis - Logic at Harvard

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forced to fail. <strong>The</strong> challenge for the advoc<strong>at</strong>e of this approach is to modifythe generic-multiverse conception of truth in such a way th<strong>at</strong> it counts ϕ asdetermin<strong>at</strong>e and yet counts CH as indetermin<strong>at</strong>e.In summary: <strong>The</strong>re is evidence th<strong>at</strong> the only way out is the fourth wayoutandthisplaces theburden back onthepluralist—the pluralist must comeup with a modified version of the generic multiverse.Further Reading: FormoreontheconnectionbetweenΩ-logicandthegenericmultiverse and the above criticism of the generic multiverse see Woodin(2011a). For the bearing of recent results in inner model theory on thest<strong>at</strong>us of the Ω Conjecture see Woodin (2011b).5 <strong>The</strong> Local Case RevisitedLet us now turn to a second way in which one might resist the local case forthe failure of CH. This involves a parallel case for CH. In Section 5.1 we willreview the main fe<strong>at</strong>ures of the case for ¬CH in order to compare it with theparallel case for CH. In Section 5.2 we will present the parallel case for CH.In Section 5.3 we will assess the comparison.5.1 <strong>The</strong> Case for ¬CHRecall th<strong>at</strong> there are two basic steps in the case presented in Section 3.3.<strong>The</strong> first step involves Ω-completeness (and this gives ¬CH) and the secondstep involves maximality (and this gives the stronger 2 ℵ 0= ℵ 2 ). For ease ofcomparison we shall repe<strong>at</strong> these fe<strong>at</strong>ures here:<strong>The</strong> first step is based on the following result:<strong>The</strong>orem 5.1 (Woodin). Assume th<strong>at</strong> there is a proper class of Woodincardinals and th<strong>at</strong> the Strong Ω Conjecture holds.(1) <strong>The</strong>re is an axiom A such th<strong>at</strong>(i) ZFC+A is Ω-s<strong>at</strong>isfiable and(ii) ZFC+A is Ω-complete for the structure H(ω 2 ).(2) Any such axiom A has the fe<strong>at</strong>ure th<strong>at</strong>ZFC+A |= Ω “H(ω 2 ) |= ¬CH”.27

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