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Second proof: Elimination

Im Dokument Tangles and where to find them (Seite 78-84)

4.2 The tangle-tree duality theorem

4.2.2 Second proof: Elimination

Our second proof ofTheorem 1still allows for a significant weakening of The-orem 1’s assumptions, but mainly focuses on cutting down on the amount of technical preliminaries required to establish its assertion. In particular we shall be able to do without Lemma 2.5.1and [13, Lemma 6.2–6.5], which we still needed in the previous section.

As in the previous section, letU be a finite universe, SU a separation system, andF ⊆2S a set of stars such thatF is standard forS. On a high level, the fundamental strategy of this second proof is the same as the first: we collect

the set of all separations at leaves of S-tree attempts that are not, as singletons, included inF, and then construct anF-tangle from those separations. However, we will not handle these S-tree attempts directly. Instead we will alter the setF so that it includes, for each two stars in F that are ‘adjacent’ in the sense of containing different orientations of some separation, their ‘elimination’: the star obtained from their union by deleting the separation they orient differently.

It will not be difficult to show that closing F under this operation influences neither whether S is F-separable nor whether an S-tree over F exists. The effect of enriching F in this way is that for everyS-tree attempt (T, α) the set of outgoing labels of its leaves will be a star inF. For the final part of the proof we will therefore no longer need to call uponLemma 2.5.1, instead shifting stars one at a time, and neither shall we need to glue together twoS-trees, since this will also be handled by the ‘elimination’-operation.

Let us make the above ideas formal. We say that a separations0S symmet-rically emulatesrS forF ifs0emulatesr inS and for every antisymmetric starσS>rr{r} inF that has an elementr0 >r the starfrs

0 (σ) either lies in F or fails to be antisymmetric. (This definition is exactly the same as the usual ‘emulates forF’, except that we only ask thatfrs

0(σ)∈ F for stars where bothσand its image are antisymmetric.) Recall thatr inS isF-critical ifrσfor someσ∈ F, but there is noσ0 ∈ F withσ0r={r}.

We say that S is symmetrically F-separable if for all F-critical r , r0S withr 6r0 there exists an s0S with an orientation s0 that symmetrically emulatesr inS forF and such thats0symmetrically emulates r0 inS forF. SinceF is standard forS theseF-critical separations can be neither trivial nor degenerate. Clearly, ifS isF-separable thenS is symmetrically F-separable.

The strengthening ofTheorem 1we are establishing then reads as follows:

Theorem 27. LetU be a finite universe,SU a separation system, and F ⊆ 2S a set of stars such thatFis standard forSandSis symmetricallyF-separable.

Then precisely one of the following holds:

there is anS-tree overF;

there is anF-tangle of S.

Let us henceforth assume thatS is symmetricallyF-separable. For our proof ofTheorem 27we will be relying on the following two concepts.

Given stars σ and ρ, we call σ an expansion of ρ if σρ with σ being antisymmetric andσrρconsisting solely of separations that are trivial inS. If s is a separation in S and σs, σs are stars with sσs and sσs, the starσ:= (σsr{s})∪(σsr{s}) is called anelimination ofσs andσs.

The first part of our proof ofTheorem 27consists of showing that we may assume, essentially, thatF consists of antisymmetric stars and is closed under expansion and elimination. For this observe first that expansions of stars are antisymmetric by definition, and that the elimination of two antisymmetric starsσs andσs is again antisymmetric: for if there were a separationt6=swith, say,tσs andtσs, we would havet 6s as well ass 6t by the star property in those respective stars, givingt =s in violation ofσs’s antisymmetry. In fact, ifσs andσs are antisymmetric, their eliminationσ equals (σsσs)r{s , s}, and every nontrivial element ofσlies in exactly one ofσs or σs.

Let F0 ⊆ F consist of all antisymmetric stars in F. For n >1 let Fn be the set of all stars σ in S that are an expansion or an elimination of star(s)

inFn−1. Note thatFn−1 ⊆ Fn since each σ∈ Fn−1 is an expansion of itself.

Further let F0 :=S

n∈NFn; this is a set of antisymmetric stars that is closed under expansion and elimination. ClearlyF0 is standard for S.

Our first lemma says that replacingF withF0 does not change whether there is anS-tree over that set of stars:

Lemma 4.2.2. There is an S-tree over F if and only if there is an S-tree overF0.

Proof. For the forward direction observe that anyS-tree that is over F and, subject to that, contains as few nodes as possible is overF0: any node whose associated star fails to be antisymmetric can be suppressed. Alternatively one may use [13, Lemmas 6.5], which shows slightly more.

For the backward direction, sinceF0 =Fnfor somen∈N, it suffices to show that there is anS-tree overFn−1whenever there is anS-tree over Fn, forn>1.

So suppose that (T, α) is anS-tree overFn with as few nodes as possible whose associated star does not lie inFn−1. We claim that (T, α) is overFn−1. Suppose not; then there is a nodetofT whose associated starσ=α(t) lies inFnrFn−1, i.e. is an expansion or elimination of some star(s) inFn−1. Let us treat these two cases in turn.

Ifσis an expansion of some ρ∈ Fn−1, we can delete fromT all components ofTt whose outgoing edge totis labelled with an element ofσrρ, thereby obtaining an S-tree which has (at least) one fewer node than (T, α) whose associated star fails to lie inFn−1.

On the other hand, ifσ is the elimination of someσs, σs ∈ Fn−1, we can split the vertex t into two new verticests and ts joined by an edge labelled withs such that their associated stars are σs andσs, respectively. For this let t0 be a neighbour of t in T and C the component of Tt containing t0. Thenr :=α(t0, t) lies inσs orσs. Ifr lies in exactly one of the two, say, inσs, we lett0 be adjacent with the corresponding vertexts. Ifr lies in both of σs andσs thenr is trivial with witness s. In this case we deleteC from T and create two new verticest1andt2, maket1adjacent tots, maket2adjacent tots, and label the outgoing edge of botht1 andt2 withr. Since Fn−1 is standard forS and thus contains{r}for all suchr, the resultingS-tree will have at least one fewer vertex than (T, α) whose associated star does not lie inFn−1.

The next step is to show thatS is symmetrically F0-separable.

Lemma 4.2.3. If S is symmetrically F-separable then it is symmetrically F0 -separable.

Proof. We show thatSis symmetricallyF0-separable, and then forn>1 thatS is symmetrically Fn-separable whenever it is symmetricallyFn−1-separable.

For the first letr , r0S beF0-critical with r6r0. Then bothr andr0 are nontrivial, and consequently neither of them is co-trivial either, since that would imply that the other one is trivial. It suffices to check thatr andr0 are alsoF -critical; we shall do this forr only. We need to show that there is noσ ∈ F withσr={r}. So suppose there is such a starσ∈ F. Thenσ /∈ F0 sincer is F0-critical. Thus by definition ofF0 we know thatσ is not antisymmetric, i.e. containss and s for somesS. Byσr={r} we must haver6=s. But thenr is trivial, a contradiction.

Suppose now thatS is symmetricallyFn−1-separable forn>1 and let us show that is is symmetricallyFn-separable. For this letr , r0S be Fn-critical withr 6r0. We must verify thatr andr0 are alsoFn−1-critical. We shall do this forr; the proof forr0 is similar. Sincer isFn-critical andFn−1⊆ Fn there is noσ∈ Fn−1withσ∩r={r}. To see thatr lies in some star inFn−1letσ∈ Fn

be a star withrσ. Ifσis an expansion of someρ∈ Fn−1 thenrρsincer is nontrivial. Otherwise σis the elimination of someσs andσs inFn−1. But thenr is contained in one of the two and we are done.

We have shown thatr andr0 areFn−1-critical and can hence use that S is symmetricallyFn−1-separable. Lets0Sbe a separation with an orientations0 that symmetrically emulates r inS for Fn−1 and such thats0symmetrically emulatesr0 inS forFn−1. We show thats0ands0do so forFn as well. Let us show this fors0; the proof fors0is analogous.

For readability we writef :=frs

0. LetσS>rr{r} be a star inFn and lett be the unique element ofσwithr 6t. Iff(σ) is not antisymmetric there is nothing to show, so let us assume that it is. We need the show that f(σ) lies in Fn.

Consider first the case thatσis an expansion of someρ∈ Fn−1. Then tρ since r and hence t are nontrivial. Moreover ρσS>r r{r}, and hence f(ρ) ∈ Fn−1 by choice of s0 since f(ρ) ⊆ f(σ) is antisymmetric. For each uσ withf(u)∈f(σ)rf(ρ) we know thatu ∈(σrρ) is trivial in S, givingt6=rand thusf(t)6t by definition off. Thereforef(t) is also trivial in S, showing thatf(σ) is an expansion off(ρ).

Let us now consider the case that σ is the elimination of σs, σs ∈ Fn−1. By symmetry we may assume thatt ∈(σsr{s}), which implies thats is the unique element ofσs withr 6s. Then bothσs andσs are subsets ofS>rr{r}: otherwise r = s, which would imply either r 6 t 6 r or r 6 t 6 r, with the first violating the antisymmetry ofσs and the latter the nontriviality ofr. Thereforef(σs) andf(σs) are well-defined and stars.

If both of f(σs) and f(σs) are antisymmetric then they lie in Fn−1 by assumption, in which case f(σ) is their elimination and hence lies in Fn as required.

So suppose thatf(σs) is not antisymmetric. Sincef(σs r{s})⊆f(σ) is antisymmetric this means thatf(s) lies inf(σsr{s})⊆f(σ). Consequently every element of f(σs) apart fromf(s) and f(s) is trivial with witness f(s).

From f(s) ∈ f(σ) we infer that f(σs) ⊆ f(σ), giving f(σs) ∈ Fn−1 by the antisymmetry off(σ). Since everyu inf(σ)rf(σs) lies inf(σs) withu6=f(s), and is hence trivial, we have that f(σ) is an expansion off(σs)∈ Fn−1 and thus lies inFn.

Analogously, if f(σs) is not antisymmetric, then f(σ) is an expansion off(σs)∈ Fn−1.

We remark that the proof ofLemma 4.2.3becomes much shorter if one only wants to proveTheorem 1 and does not care for the differences between ‘F -separable’ and ‘symmetricallyF-separable’.

We are now ready to proveTheorem 27.

Proof of Theorem 27. It is easy to see there there cannot be both anF-tangle ofS and anS-tree overF. We must therefore show that at least one of the two exists. So suppose that there is noS-tree over F. Then, byLemma 4.2.2, there

is noS-tree overF0 either. We shall construct anF0-tangle ofS. This will then be anF-tangle as well since it avoids all non-antisymmetric stars by definition.

Let P be the set of all rS with {r} ∈ F/ 0. Suppose first that we can findP ⊆ P such thatP is a consistent and antisymmetric set that contains, for each star in F0, the inverse of some element of that star. ThenP contains no co-trivial separation sinceF0 is standard forS. We can thus applyLemma 2.4.1 toP to obtain a consistent orientationOP ofS. ThisO is then anF0-tangle:

for each starσ∈ F0 the orientationO contains somes withsσ, and hence avoids σ.

So let us show that we can find such a setP ⊆ P. For this pick aP⊆ P that is minimal with respect to inclusion subject to the conditions thatP contains for each star inF0the inverse of some element of that star, and thatPis down-closed inP, that is, such thatpP for all p∈ P withp 6q for someqP. Such a P exists since P itself is a candidate: if, for some σ ∈ F0 there would be nos ∈ Pwithsσ, then theS-tree obtained fromσwould be overF0.

We claim that thisP is antisymmetric and consistent. Suppose for a con-tradiction that this is not the case. Then there arer 6=s inP withr 6s. In particular we can taker ands to be maximal elements ofP. Neither r nors can be co-trivial inS sinceF0 is standard forS andr , s ∈ P. Therefore neither of the two can be trivial or degenerate either, since this would imply that the other one is co-trivial.

By picking r and s among the maximal elements of P we ensure that bothPr{r} andPr{s}are still down-closed in P. Thus, by the minimality of P, there are starsσr and σs in F0 whose only elements with inverse in P are r ands, respectively. By choosing σr andσs inclusion-minimal with this property we can ensure that{t}∈ F/ 0 for each elementt of those stars other than r ands, respectively: for iftσr witht 6=r, say, and{t} ∈ F0, then the eliminationσrr{t}ofσr and{t} still hasr as the only element withrP.

We claim thatr isF-critical. Since we have rσr it suffices to show that there is noσ∈ Fwithσ∩r={r}. Suppose that there is such a starσ. Consider the eliminationρ:= (σrσ)rrof these two stars. We haveρ∈ F0 by definition, and hence P contains some t withtρ. Thent 6=r, and by choice ofσrwe have t /σr. But thentσ, which also contains r, givingr 6t by the star property. This contradicts the maximality ofr inP.

A similar argument shows thats isF0-critical. By the assumption thatS is symmetrically F0-separable we thus find ans0S with an orientations0that symmetrically emulatesr inS forF0and such thats0symmetrically emulatess in S for F0. Let σr0 :=frs

0 (σr) and σs0 := fss

0 (σs). Sincer 6s06s we have s0σr0 ands0σs0.

Suppose now thatσr0 is not antisymmetric. Sincer is nontrivial and hence so is s0>r, we must haves0σr0. There is thus sometσr withts0= frs

0(t) =s0. Thent 6s06s, with the latter lying inP. By the minimality ofσrwe havet ∈ P. ThereforetP sinceP is down-closed inP, contrary to the assumption thatr is the only element ofP whose inverse lies inσr.

A similar argument shows thatσ0sis antisymmetric. We hence haveσr0, σs0 ∈ F0.

Lett be an element ofσrother thanr. Thent ∈ PrP by minimality ofσr. SinceP is down-closed inP, andt 6ts0=frs

0 (t), the latter cannot lie in P either. ThereforeP contains no separation whose inverse lies inσr0 rs0.

A similar argument shows thatP contains no separation whose inverse lies inσ0srs0 either. But then the eliminationσ0 := (σ0rσs0)rs0 is a star inF0 with no element whose inverse lies inP, a contradiction. This concludes the proof that P is consistent and antisymmetric.

Im Dokument Tangles and where to find them (Seite 78-84)