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521–527 DOI: 10.18514/MMN.2021.3368 THE FIRST THREE LARGEST NUMBERS OF SUBUNIVERSES OF SEMILATTICES DELBRIN AHMED AND ESZTER K

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Vol. 22 (2021), No. 2, pp. 521–527 DOI: 10.18514/MMN.2021.3368

THE FIRST THREE LARGEST NUMBERS OF SUBUNIVERSES OF SEMILATTICES

DELBRIN AHMED AND ESZTER K. HORV ´ATH Received 03 June, 2020

Abstract. Let(L,∨)be a finite n-element semilattice wheren5. We prove that the first largest number of subuniverses of ann-element semilattice is 2n,while the second largest number is 28·2n−5and the third one is 26·2n−5.Also, we describe then-element semilattices with exactly 2n, 28·2n−5or 26·2n−5subuniverses.

2010Mathematics Subject Classification: 06A12; 06B99

Keywords: finite lattice, sublattice, subuniverse, finite semilattice, number of subuniverses

1. INTRODUCTION AND OUR RESULT

For a semilattice(L,∨), Sub(L,∨)will denote itssubuniverse-lattice. By a sub- universe, we mean a subsemilattice or the emptyset. All semilattices occurring in this paper will be assumed to be finite. On a semilattice(L,≤), we have a natural partial ordering defined by

x≤y ⇐⇒ x∨y=y.

Conversely, if (L,≤) is partial order in which any two elements x,y have a least upper boundx∨y, then(L,∨)is a semilattice. For anyx,yin a join-semilattice,x∧y is defined by their infimum provided it exists; if this infimum does not exist, thenx∧y is undefined. LetPandQbe posets with disjoint underlying sets. Then theordinal sum P+ordQis the poset onP∪Qwiths≤tif eithers,t∈Pands≤t; ors,t∈Q ands≤t; ors∈Pandt∈Q. To draw the Hasse diagram ofP+ordQ, we place the Hasse diagram ofQabove that ofPand then connect any minimal element ofQwith any maximal element ofP; see Figure1. IfKwith 1 andLwith 0 are finite posets, then their glued sumK+gluLis the ordinal sum of the posetsK\ {1K}, the singleton poset, andL\ {0L}, in this order; see Figure2. Note that+glu is an associative but not a commutative operation.

The semilatticesH3andH4will be used later, see Figure3.

This research was supported by grant TUDFO/47138-1/2019-ITM of the Ministry for Innovation and Technology, Hungary. This research of the second author was partially supported by NFSR of Hungary (OTKA), grant number K 115518.

© 2021 Miskolc University Press

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FIGURE1. The ordinal sumP+ordQofPandQ

FIGURE2. The glued sumK+gluLofKandL

Our result is motivated by similar results, see Ahmed and Horv´ath [1], Cz´edli [3–7] and Cz´edli and Horv´ath [8]. To obtain more information about lattice theory and semilattices we direct the reader to the bibliography indicated in [9,10] and [2], respectively.

For a natural numbern∈N+:={1,2,3, . . .}, let

NS(n):={|Sub(L)|:Lis a semilattice of size|L|=n}.

Theorem 1. If5≤n∈N+, then the following assertions hold.

(i) The largest number inNS(n) is2n=32·2n−5.Furthermore, an n-element semilattice(L,∨)has exactly2nsubuniverses if and only if(L,∨)is a chain.

(ii) The second largest number inNS(n)is28·2n−5.Furthermore, an n-element semilattice(L,∨)has exactly 28·2n−5 subuniverses if and only if (L,∨)∼= H3+gluC1or(L,∨)∼=C0+ordH3+gluC1, where C0and C1 are finite chains.

(iii) The third largest number inNS(n) is26·2n−5. Furthermore, an n-element semilattice(L,∨)has exactly 26·2n−5 subuniverses if and only if (L,∨)∼= H4+gluC1or(L,∨)∼=C0+ordH4+gluC1, where C0and C1are finite chains.

2. TWO PREPARATORY LEMMAS

An elementuof a semilatticeLis called a narrow element, or anarrowsfor short, ifu̸=1LandL=↑u∪ ↓u. That is, ifu̸=1Landx∥uholds for nox∈L.

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The notion of a binary partial algebra is well known, but the reader can refresh his/her knowledge from [4]. Let A be a finiten-element binary partial algebra. A subuniverseofA is a subsetX ofA such that X is closed with respect to all partial operations. The set of subuniverses of A will be denoted by Sub(A).Therelative number of subuniverses ofA denoted byσk(A)is defined as follows:

σk(A) =|Sub(A)| ·2k−n.

In order to comply with [8], will usek=5. The original definition ofσkis given in the paper of Cz´edli [4], there he usedk=8.

Lemma 1. If (K,∨) is a subsemilattice and H is a subset of a finite semilattice (L,∨), then the following three assertions hold.

(i) With the notation t:=|{H∩S:S∈Sub(L,∨)}|, we have that σk(L,∨)≤t·2k−|H|.

(ii) σk(L,∨)≤σk(K,∨).

(iii) Assume, in addition, that(K,∨)has no narrows. Thenσk(L,∨) =σk(K,∨) if and only if(L,∨) is (isomorphic to) C0+ord(K,∨) +gluC1,where C1 is a chain, and C0is a chain or the emptyset.

Proof. Parts(i) and(ii)can be extracted from the proof of in Lemma 2.3 of [4].

The argument there yields a bit more than stated in (i) and (ii); namely, for later reference, note the following.

Ifσk(L,∨) =σk(K,∨), then for everyS∈Sub(K,∨)and every

subsetXofL\Kwe have thatS∪X ∈Sub(L,∨). (2.1) Next, to prove part(iii), letn:=|(L,∨)|andm:=|(K,∨)|.Letk:=5,the case of another k is analogous. Assume that (K,∨) has no narrows. First, let (L,∨) = C0+ord(K,∨) +gluC1. It is obvious that whenever X ⊆L\K and S ∈Sub(K,∨), thenS∪X ∈Sub(L,∨). SinceL\K has 2|L|−|K| subsets,|Sub(L,∨)| ≥ |Sub(K,∨)| · 2|L|−|K|. Dividing this inequality by 2n−5 =2m−5·2|L|−|K| we obtain the required equality, as the converse inequality given in part(ii).

Conversely, assume the equality in(iii). We claim that

for ally∈Kand for allx∈L\K,y∦x. (2.2) Suppose the contrary. Ify∈K, then {y} ∈Sub(K). If x∈L\K andy||x,then {y,x}is not a subuniverse ofL,contradicting (2.1).

We claim that

for allx∈L\K,x̸>1K implies that for ally∈K,x<y. (2.3) Suppose the contrary and pickxinL\K andy∈K such thatx̸>1K andx̸<y.

Using (2.2) and x̸=y,we have that y<x<1K. Let p:=W{s ∈K :s<x}; this exists by finiteness andy≤p≤x.In fact, p∈K asK is a subsemilattice of Lbut x̸∈K,soy≤p<x.Now letu∈Ksuch thatu̸≤p.We know from (2.2) thatu∦x.

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If we had u≤x (in fact, u<x since x̸∈K), thenu would be one of the joinands defining pand so u≤ pwould be a contradiction. Hencex<u,and so p<x<u implies p<u. We have seen that, for any u∈K,u̸≤ p implies p<u. In other words,K=↑Kp∪ ↓Kp,which means pis a narrows, contradicting our assumption on K.Thus, (2.3) holds. Finally, we show thatL\K is a chain. Indeed, ifL\Kis not a chain, saya||b,a∈L\Kandb∈L\K,then∅∈Sub(K)extended by{a,b} ̸∈Sub(L) would contradict (2.1). DefineC1={x∈L\K:x≥1K}; it is a chain (a subchain of L\K). LetC0= (L\K)\C1; it is either a chain or empty. IfC0 is empty, thenLis K+glueC1, as required. IfC0is nonempty, then its elements are less than any element ofKby (2.3), and soL=C0+ordK+glueC1, as required. □ The following lemma can be proved by a computer program, but for the reader’s convenience, we give its proof.

FIGURE 3. H3andH4

Lemma 2. For the join-semilattices given in Figure 3 the following assertions hold.

(i) σ5(H3) =28, (ii) σ5(H4) =26,

Proof. The notations given by Figure3will be used. For later reference, note that if(L,∨)is a chain then|Sub(L,∨)|=2|(L,∨)|.

For(i), observe that

|{S∈Sub(H3,∨):a̸∈S}|=4, (S is chain),

|{S∈Sub(H3,∨):a∈S,{b} ∩ S=∅}|=2, and

|{S∈Sub(H3,∨):a∈S,{b} ∩ S̸=∅}|=1,

whereby|Sub(H3,∨)|=4+2+1=7=28·23−5, note thatσ5(H3) =28 proves(i).

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For(ii), let us compute

|{S∈Sub(H4,∨):c̸∈S}|=7, by(i),

|{S∈Sub(H4,∨):c∈S,{a,b} ∩ S=∅}|=2,and

|{S∈Sub(H4,∨):c∈S,{a,b} ∩ S̸=∅}|=4.

Hence,|Sub(H4,∨)|=7+2+4=13=26·24−5, whileσ5(H4) =26 proves(ii).

Remark1. For counting subsemilattices, a computer program is available on G.

Cz´edli’s webpage: http://www.math.u-szeged.hu/˜czedli/

3. THE REST OF THE PROOF

Proof of Theorem1. Part(i)is trivial. For part(ii)let(L,∨)be ann-element sem- ilattice. We know from Lemma1 (iii)that if

(L,∨)∼=H3+gluC1or(L,∨)∼=C0+ordH3+gluC1, whereC0andC1 are chains, (3.1) then σ5(L) =σ5(H3) =28, indeed. Conversely, assume that σ5(L) =28. Then it follows from part(i)thatLis not a chain. SoLhas two incomparable elements,aand b. Clearly,{a,b,a∨b}is a join-subsemilattice isomorphic toH3. Butσ5(H3)is also 28 by Lemma2 (i). Thus, Lemma1 (iii)immediately yields thatLis of the desired form. By this we completed the proof of part(ii)of Theorem1.

We prove part(iii).

Assume that(L,∨)is of the given form, thenσ5(L,∨) =26 is clear from Lemma 2 (ii)and Lemma1 (iii). In order to prove the converse, that is, the nontrivial im- plication, assume thatσ5(L,∨) =26. By Theorem1 (i),(L,∨)has two incomparable elements, a and b. By part Theorem 1 (ii), {a,b} is not the only 2-element anti- chain inLsince otherwiseσ5(L,∨)would be 28. To complete the proof, consider the following cases.

Case 1: There is an antichain {c,d} disjoint from {a,b}, where the elements a, b, c, d are distict. Let x:=a∨b and y:=c∨d. There are cases depending ont:=|{a,b,c,d,x,y}|, which is 4, 5, or 6. The number of possible cases can be reduced by symmetry:aandbplay a symmetric role, so docandd,and so do{a,b}

and{c,d}and thus x and y. We consider three sub-cases as we will see below:

Sub-case 1a:Nowt=6. Take the partial algebraU1={a,b,c,d,x,y}witha∨b= x andc∨d=y. This six-element partial algebra has σ5(U1) =24.5, this can be checked by the mentioned computer program. By Lemma 2.3 from [4] we obtain thatσ5(L)≤σ5(U1)≤24.5, contradictingσ5(L) =26. Thus, this case is excluded.

Sub-case 1b:Nowt=5. By symmetry,y=c∨dis not a new element, soy=c∨d is eitherxora. The casey=bneed not be considered becauseais symmetric tob.

Therefore, this sub-case 1b is split in two cases as follows:

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First, where y =x, this case is captured by taking the partial algebra U2 = {a,b,c,d,x}witha∨b=x,c∨d=x. It hasσ5(U2) =25 by the mentioned computer program. Like above, this impliesσ5(L)≤σ5(U2)≤25, contradictingσ5(L) =26.

Second, where y=a, this case is captured by taking the partial algebra U3 = {a,b,c,d,x}witha∨b=x,c∨d=a. This five-element partial algebra hasσ5(U3) = 24<26, and we get a contradiction as above.

By the above we can note that the sub-case 1b is excluded since so are both of its subcases.

Sub-case 1c:Heret=4. Thenx=a∨bis one ofcandd. By symmetry, we can assume thata∨b=c. However, thena<c<c∨d,b<c<c∨d, wherebyy=c∨d is none of the elementsa,b,c,d,contradictingt=4. So this case is excluded.

After having all of its sub-cases excluded, we obtain that Case 1 is excluded. That is, no two-element antichain is disjoint from{a,b}. But remember that there is an- other two-element antichain, whereby, by a-b symmetry, we considerCase 2: there is an elementcsuch thata andc are incomparable. Again there are two sub-cases according to the position ofbandc.

Sub-case 2a: Herebandcare also incomparable. Here, we have to investigate, how many of a∨b, a∨c, and b∨c are equal toa∨b∨c. Since the answer could be 0,1,2 or 3 (and using symmetry), it suffices to consider only the following four join-semilattices. The first join-semilattice isK0={a,b,c,z,x,y,1}with edgesax, bx,by,cy,az, cz,x1,y1,z1 and equalitiesa∨b=x,b∨c=y,a∨c=z; this gives σ5(K0) =15.25. The second join-semilattice isK1={a,b,c,x,y,1}with edgesax, bx,by,cy,x1,y1 and equalitiesa∨b=x,b∨c=y,a∨c=1; this givesσ5(K1) =18.5.

The third is K2={a,b,c,x,1} with edges ax,bx,x1,c1 and constraints a∨b=x, a∨c=1, b∨c=1 ; this gives σ5(K2) =22. The fourth is K3 ={a,b,c,1} with edges a1,b1,c1, and equalities a∨b=1, a∨c=1, b∨c=1; this givesσ5=24.

Since one ofK0,K1,K2, andK3is a subsemilattice ofLand all the fourσ5values of these join-semilattices are smaller than 26, therefore sub-case 2a is excluded.

Sub-case 2b: Herebandcare comparable in addition to thataandcare incom- parable and so do aandb. At present, bandc play a symmetric role. So we can assume thatb<c. Suppose, for contradiction, thatx:=a∨b<a∨c=: 1. By the incomparabilities assumed, |{a,b,c,x,1}|=5; for example if x=a∨b=c is im- possible since it would yielda<c. The mentioned constraints are definingK.Now σ5(K) =23<26 gives a contradiction. Soa∨b<a∨cfails buta∨b≤a∨csince b<c. Therefore, with 1=a∨b=a∨c,{a,b,c,1}is a subsemilattice (isomorphic to)H4.

Now that all other possibilities have been excluded, we know that H4 is a join- subsemilattice of (L,∨). Observe thatH4 has no narrows. Therefore, by Lemma 1 (iii),(L,∨)is of the desired form. By this, the proof of Theorem1is completed.

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REFERENCES

[1] D. Ahmed and E. K. Horv´ath, “Yet two additional large numbers of subuniverses of finite lattices,”

Discussiones Mathematicae - General Algebra and Applications, vol. 39, no. 2, p. 251, 2019, doi:

10.7151/dmgaa.1309.

[2] I. Chajda, R. Halaˇs, and J. K¨uhr,Semilattice structures. Heldermann Lemgo, 2007, vol. 30.

[3] G. Cz´edli, “A note on finite lattices with many congruences,”Acta Univ. M. Belii Ser. Math., pp.

22–28, 2018.

[4] G. Cz´edli, “Eighty-three sublattices and planarity,”Algebra universalis, vol. 80, no. 4, p. 45, 2019, doi:10.1007/s00012-019-0615-3.

[5] G. Cz´edli, “Finite semilattices with many congruences,”Order, vol. 36, no. 2, pp. 233–247, 2019, doi:10.1007/s11083-018-9464-5.

[6] G. Cz´edli, “Lattices with many congruences are planar,”Algebra universalis, vol. 80, no. 1, p. 16, 2019, doi:10.1007/s00012-019-0589-1.

[7] G. Cz´edli, “One hundred twenty-seven subsemilattices and planarity,”Order, pp. 1–11, 2019, doi:

/10.1007/s11083-019-09519-x.

[8] G. Cz´edli and E. K. Horv´ath, “A note on lattices with many sublattices,”Miskolc Mathematical Notes, vol. 20, no. 2, p. 839–848, 2019, doi:10.18514/MMN.2019.2821.

[9] G. Gr¨atzer,Lattice theory: foundation. Springer Science & Business Media, 2011.

[10] I. Rival and R. Wille, “Lattices freely generated by partially ordered sets: which can be” drawn”?”

Journal f¨ur die reine und angewandte Mathematik, vol. 1979, no. 310, pp. 56–80, 1979, doi:

10.1515/crll.1979.310.56.

Authors’ addresses

Delbrin Ahmed

University of Szeged, Bolyai Institute, Aradi v´ertan´uk tere 1, 6720 Szeged, Hungary E-mail address:delbrin@math.u-szeged.hu

Eszter K. Horv´ath

(Corresponding author) University of Szeged, Bolyai Institute, Aradi v´ertan´uk tere 1, 6720 Szeged, Hungary

E-mail address:horeszt@math.u-szeged.hu

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