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Minimum number of different distances defined by a finite number of points

Albujer Brotons, Alma Luisa; Segura Gomis, Salvador

Abstract

We study the minimum number of different distances defined by a finite number of points in the following cases: a) we consider metrics different from the euclidean distance in the plane, b) we consider the euclidean distance but restricted to subsets of the plane of special interest, c) we consider other topological surfaces: the cylinder and the flat torus. All these results extend those obtained by Erdös and other mathematicians for the euclidean distance in the plane.

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Minimum numbe o di e en dis ances de ined by a ini e numbe o poin s Albuje , A. aand Segu a Gomis, S. a aDepa amen o de An´alisis Ma em´a ico, Uni e sidad de Alican e, Campus de San Vicen e del Raspeig, E-03080-Alican e, Spain Abs ac We s udy he minimum numbe o di e en dis ances de ined by a ini e numbe o poin s in he ollowing cases: a) we conside me ics di e en om he euclidean dis ance in he plane, b) we conside he euclidean dis ance bu es ic ed o subse s o he plane o special in e es , c) we conside o he opological su aces: he cylinde and he la o us. All hese esul s ex end hose ob ained by E d¨os and o he ma hema icians o he euclidean dis ance in he plane. Key wo ds: dis ances, me ics, in ege la ice, la o us, cylinde 1. In oduc ion In 1946 [4] E d¨os posed he ollowing p oblem: le (n) deno e he minimum numbe o dis inc dis ances ha can occu among he n(n−1) 2dis- ances be ween ndis inc poin s in he plane; wha can we know abou (n)? Fo small alues o ni is easy o compu e (n) and many imes he numbe (n) is a ained o di e en con igu a ions. Le us see he i s exam- ples. ............... . . . . . . . . . . . . . ................... . . . . . . . . . . . . . . ................ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . .. . . . . . . . . .............. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ............... . . . . . . . . . . . . . . . (3) = 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . ........ (4) = 2 . . . . . . . .. . . . . . . .............. .............. . . . . . . . . . . . . .. . . . . . . . . . . . . . (5) = 2 (6) = 3 E d¨os ob ained asymp o ic es ima es o (n). The i s asymp o ic es ima e was cn1/2< (n)< c n (ln n)1/2 Email add esses: [email protected] (Albuje , A.), Sal ado .Segu [email protected] (Segu a Gomis, S.). E d¨os conjec u ed ha (n)> cn1−ε o each ε > 0 and o e ed 500$ o a p oo o a disp oo . E d¨os conjec u e is s ill open. The las imp o e- men was made by Szeme ´edi (1992) who p o ed ha (n)> cn4/5([2]). (n) can be in es iga ed in dimension Rd wi h d > 2. Fo d= 3 he bes bounds a e cn4/3log log n < (n) ([5]) and (n)< n3/2+o(1) ([3]). Recen ly B aß([1]) de e mined (n) exac ly in dimension d= 4. The e a e also bounds o gene al dimensions. The aim o his communica ion is o ex end E d¨os p oblem o o he ambien spaces. a) Fi s we conside me ics di e en om he euclidean dis ance in he plane. b) Then we conside also he euclidean dis ance bu es ic ed o subse s o he plane o spe- cial in e es (poin s o he in ege la ice and poin s o a ional coo dina es). c) Finally we conside E d¨os p oblem in o he opological spaces. 20 h EWCG Se ille, Spain (2004) 20 h Eu opean Wo kshop on Compu a ional Geome y 2. E d¨os p oblem conside ing a bi a y dis ances in he plane In he plane we can de ine many dis ances. Le us ecall ha a dis ance in he plane is a map d:R2×R2→R such ha i) d(x, y)≥0, d(x, y) = 0 i x=y ii) d(x, y) = d(y, x) iii) d(x, z)≤d(x, y) + d(y, z) An in e es ing way o de ine a me ic in he plane is as ollows. Le us de ine he gauge unc ion g(K, x) o a closed, con ex se K ela i e o an o igin 0 as g(K, x) = in {λ:x∈λK, λ > 0} I is easy o p o e ha i Kis a p ope con- ex body and 0 ∈in K, he unc ion m(x, y) = g(K, x −y) almos de ines a dis ance in he plane. The condi ion ha is iola ed is he symme y con- di ion m(x, y) = m(y, x) ha holds only i Kis cen ally symme ic. So a closed, cen ally symme ic, con ex se K wi h 0 ∈in K de ines a me ic ([7]). All hese me ics gene a e he euclidean opol- ogy. In he pa icula case ha he se K ha induce his me ic is a squa e o he ype h(p, 0),(0, p),(−p, 0),(0,−p)i, hen we ob ain he amous axi-cab me ic which is also known as he Manha an me ic. This me ic is pa icula ly ele an o ou analysis. The axi-cab me ic can also be de ined as dT((x1, y1),(x2, y2)) = |x2−x1|+|y2−y1| We a e going i s o es ima e he minimum num- be o dis inc dis ances wi h he axi-cab me ic. We begin showing in able 1 ha he axi-cab me ic p o ides di e en alues o (n) han hose alues a ained wi h he euclidean me ic. (n) Euclidean me ic Taxi-cab me ic 3 1 1 4 2 1 5 2 2 6 3 2 7 3 2 Table 1 Some alues o (n) wi h he axi-cab me ic . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . (3) = (4) = 1 (5) = ... = (9) = 3 Now we a e going o es ima e p ecisely (n). Lemma 1 Conside ing he axi-cab me ic (n)≤ ⌈√n⌉−1 PROOF. Le Lbe he la ice gene a ed by he ec o s (1,1) and (1,-1). Le pbe an in ege numbe and le Kpbe he poin se de e mined by Kp= L∩h(0,0),(p−1,−(p−1)),(2(p−1),0),(p−1, p− 1)i. Conside K⌈√n⌉. This se con ains a leas n poin s since ⌈√n⌉ · ⌈√n⌉ ≥ √n·√n=n, so we can always choose npoin s in K⌈√n⌉. As he poin s in K⌈√n⌉de e mine ⌈√n⌉ − 1 di e en dis ances among hem, (n)≤ ⌈√n⌉−1  This es ima e is no only an uppe bound bu a p ecise de e mina ion o he minimum numbe o dis inc dis ances: Lemma 2 Conside ing he axi-cab me ic (n)≥ ⌈√n⌉−1 PROOF. We a e going o gi e a ske ch o he p oo : We conside he “me ic ci cum e ences”, which in ou case a e squa e-shaped, as he locus o he poin s ha a e a dis ance om a poin p∈R2: S(p, ) = {x∈R2:dT(p, x) = } Now we a e going o loca e he maximum num- be o poin s who de ine a mos mdis ances among Ma ch 25-26, 2004 Se ille (Spain) hem. As we a e always dealing wi h a ini e num- be o poin s, he e would be a leas wo poin s a,bsuch ha he dis ance be ween hem is he maximum possible. All he o he s poin s should be loca ed in he in e sec ion o m“me ic ci - cum e ences” cen e ed a aand m“me ic ci cum- e ences” cen e ed a b. I we do no wan o in- c ease he numbe o di e en dis ances, he adius o hese “me ic ci cum e ences” a e {id(a,b) m}m i=1. The e a e wo possible si ua ions: i) All he “me ics ci cum e ences” in e sec p ope ly. In his case as hey ha e he pseudodisc p ope y ( he e a e a mos wo p ope in e sec- ions o each pai o pseudodiscs), hen we ob ain ha he maximum numbe o possible poin s is gi en by (m+ 1)2and hey a e dis ibu ed in a ansla ed o he squa e Km+1. F om his con ig- u a ion we ob ain ou lowe bound. ii) The e a e some pai s o “me ic ci cum e - ences” ha do no in e sec p ope ly bu a e an- gen . In his case hey a e angen along a s aigh line segmen . Conside ing he ends o his s aigh line segmen and aking he “me ic ci cum e - ences” cen e ed a hese ends we conclude ha he e a e no mo e han (m+1)2possible loca ions. So we also each he same lowe es ima e.  I is easy o see ha he a gumen in he p oo o lemma 2 holds o all me ics gene a ed by he gauge unc ion o a cen ally symme ic, con ex se ; as he equali y sign is a ained in he case ha he body which gene a es he me ic is a squa e, we can conclude he ollowing co olla y: Co olla y 3 Among all me ics gene a ed by a closed, cen ally symme ic, con ex se K, he me - ics ha gi e he smalles alues o (n)a e hose in which he me ic is gene a ed by he gauge unc- ion co esponding o a squa e. Fo ins ance he axi-cab me ic o he maximum me ic de ined as d((x1, y1)(x2, y2)) = max{|x2−x1|,|y2−y1|} Co olla y 3 does no hold o gene al me ics. Fo example, le us conside he so called pos o ice me ic d((x1, y1)(x2, y2)) = d2((x1, y1),(0,0)) +d2((0,0),(x2, y2)) whe e d2s ands o he euclidean dis ance in he plane. In his case i is easy o see ha we can a ange in ini e poin s so ha each pai o hem is a dis ance one; so (n) = 1 o all n. (0,0) 3. The minimum numbe o dis inc dis ances p oblem wi h he euclidean dis ance in he in ege la ice I we conside E d¨os p oblem es ic ed o he in ege la ice we ob ained di e en alues o (n) as he ollowing able shows: (n) Plane In ege la ice 3 1 2 4 2 2 5 2 3 6 3 4 7 3 4 Table 2 Some alues o (n) in he in ege la ice In gene al, we ha e he ollowing uppe bound: Lemma 4 In he in ege la ice (n)≤(⌈√n⌉−2)(⌈√n⌉+ 1) 2 PROOF. Le Lbe he in ege la ice and le Pnbe he poin se Pn=L∩ h(0,0),(0,⌈√n⌉ − 1),(⌈√n⌉ − 1,0),(⌈√n⌉ − 1,⌈√n⌉ − 1)i.Pncon- ains a leas npoin s.We can compu e he numbe o dis inc dis ances by conside ing only he dis- ances be ween (0,0) and he he es o he poin s below he diagonal o he squa e. Then we ha e a mos 2 + 3 + ... + (⌈√n⌉ − 1) dis inc dis ances, 20 h Eu opean Wo kshop on Compu a ional Geome y ha is he sum o he e ms o an a i hme ic p o- g ession, so (n)≥2 + 3 + ... + (⌈√n⌉ − 1) = ⌈√n⌉(⌈√n⌉−1) 2−1 = (⌈√n⌉−2)(⌈√n⌉+1) 2 (0,0)  The alues o (n) i we es ic o he in ege la ice a e he same ha i we es ic o he poin s wi h a ional coo dina es because a ini e numbe o poin s wi h a ional coo dina es a e included in an in ege la ice gene a ed by he ec o s (q, 0) ,(0, q) whe e qis he leas common denomina o o he coo dina es o he poin s ha we a e conside - ing. This es ima e o (n) can be applied o com- pu e s, because he compu e sc een can be ep e- sen ed as a ini e numbe o poin s wi h a ional coo dina es. 4. E d¨os p oblem o o he opological spaces The i s ma hema icians o conside his p ob- lem in o he opological spaces we e E d¨os, Hick- e son and Pach ([6]) who s udied he case o he sphe e. We a e going o conside wo o he pa icula opological su aces: he cylinde and he la o us. As we can see in able 3, o small alues o nwe ob ain he same alues o (n) in bo h opological su aces, bu his do no occu o g ea e alues o n. (n) Plane Cylinde Fla o us 3 1 1 1 4 2 1 1 5 2 2 2 6 3 2 2 Table 3 Some alues o (n) in di e en opological su aces Now, we can gi e uppe bounds o bo h opo- logical su aces. Lemma 5 In he la o us (n)≤(⌊⌈√n⌉/2 + 1⌋+ 2)(⌊⌈√n⌉/2 + 1⌋−1) 2 Lemma 6 In he cylinde (n)≤(⌊⌈√n⌉/2 + 1⌋+ 2)(⌊⌈√n⌉/2 + 1⌋−1) 2 +(⌊⌈√n⌉/2 + 1⌋)(⌈√n⌉−⌊⌈√n⌉/2 + 1⌋) We omi he p oo s because hey a e simila o he p oo o lemma 3. We ha e o conside a pa - icula la ice and in e sec i wi h he opological su aces, as he igu e shows. Then, by some a i h- me ic compu a ions, we ob ain he bounds. Fla To us Cylinde Re e ences [1] B aß, P.: On he maximum numbe o uni dis ances among npoin s in dimension ou , In ui i e geome y (Budapes , 1995), 277–290, Bolyai Soc. Ma h. S ud., 6, J´anos Bolyai Ma h. Soc., Budapes , 1997. [2] Chung, F. R. K., Szeme di, E. and T o e , W. T.: The numbe o di e en dis ances de e mined by a se o poin s in he Euclidean plane, Disc e e Comp. Geome y 7(1992), 1–11. [3] Cla kson, K., Edelsb unne , H., Guibas, L., Sha i , M. and Welzl, E.:Combina o ial complexi y bounds o a angemen s o cu es and sphe es, Disc e e Comp. Geome y 5(1990), 90–160. [4] E d¨os, P.: On se s o dis ances o npoin s, Ame . Ma h. Mon hly 53 (1946), 248–250. [5] E d¨os, P.:On se s o dis ances o npoin s in Euclidean space, Magya Tudom´anyos Akad´emia M´a ema ikai Ku a ´o In ´eze K¨ozlem´enyei 7(1960), 165–169. [6] E d¨os, P. , Hicke son, D. and Pach J.: A p oblem o Leo Mose abou epea ed dis ances on he sphe e, Ame . Ma h. Mon hly 96 (1989), 569–575. [7] Guggenheime , H. W.: Applicable geome y, Robe E. K iege Publishing Co., Inc. , Hun ing on, New Yo k, 1977.