COMPOSITIONS, PARTITIONS, AND FIBONACCI NUMBERS

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COMPOSITIONS PARTITIONS AND FIBONACCI NUMBERS ANDREW V. SILLS Abstract. A bijective proof is given for the following theorem: the number of compositions of n into odd parts equals the number of compositions of n + into parts greater than one. Some commentary about the history of partitions and compositions is provided.. Introduction A composition of an integer n is a representation of n as a sum of positive integers for example the eight compositions of 4 are as follows: 4 3 + + 3 2 + 2 2 + + + 2 + + + 2 + + +. A partition of n is a representation of n as a sum of positive integers where the order of the summands is considered irrelevant. Thus 2 + + + 2 + and + + 2 are three distinct compositions but are all considered to be the same partition of 5. The individual summands of a composition or partition are called its parts. By convention the parts of a partition are written in wealy decreasing order. Thus the five partitions of 4 are 4 3 + 2 + 2 2 + + + + +. A composition of n with l parts may be represented graphically by n unit lengths separated by l nodes in such a way as to depict a part j by j adjacent unit lengths bounded by a node on either side in the case of an interior part) and a node on one side in the case of the first or last part). See MacMahon [0 Sec. IV Ch. p. 5 25]). Let us agree to call this representation the MacMahon graph of a composition. For example the composition 2+4+++5 of 3 has the following MacMahon graph: It is then straightforward to encode the MacMahon graph of a composition of n with l parts as a bit sequence of length n consisting of l ones and n l zeros where as we read the graph from left to right we choose a if a node is present between two unit lenghts and a 0 if no node is present. For consistency we may as well call this the MacMahon bit sequence of a composition. Thus the MacMahon bit sequence corresponding to the composition 2 + 4 + + + 5 is 0 000 0000. We have chosen to put a space after each in the bit sequence as this maes it easy to read off the corresponding composition.

2 ANDREW V. SILLS It follows from the MacMahon bit sequence that there are 2 n compositions of n since the bit sequence is of length n and each bit may tae on either of two values. Thus for n a positive integer we have the formula cn) = 2 n ) where cn) denotes the number of compositions of n. The theory of partitions began with Euler in the mid-eighteenth century. In an effort to understand certain aspects of partitions Euler introduced the idea of a generating function of a sequence {a n } that is he encoded the sequence as the coefficients of a power series n=0 a nx n. In particular Euler showed that the generating function for pn) the number of partitions of n can be expressed as an elegant infinite product: pn)x n = n=0 j= x j 2) where x < to ensure convergence if x is taen to be a complex variable. This is necessary when analytic properties of 2) are studied. When 2) is used for combinatorial purposes x may be taen to be a formal variable. Euler also showed that 2) implies the following recurrence for pn): ) )) pn) = ) p j j3j ) j3j + ) n + p n. 3) 2 2 j= We pause to remar that in contrast to the extremely simple formula ) for cn) the behavior of pn) is much more complicated. In 937 Hans Rademacher [] building on earlier wor by Hardy and Ramanujan [8] proved the following formula for pn): pn) = π 2 = A n) d dn where A n) is a Kloosterman-type sum A n) = exp and sh ) is a Dedeind sum with 0 h< gcdh)= sh ) = x)) := j= j sinh π 2 3 n 24 n 24 πish ) 2πinh ) )) )) hj { x x 2 if x Z 0 if x Z. ) ) 4) Peter Shiu adapted 4) to compute p0 6 ). See [4]) Eq. 4) was the only exact explicit formula nown for pn) until Ken Ono and Jan Bruinier amazed the mathematical community in early 20 with the announcement [2]

COMPOSITIONS PARTITIONS AND FIBONACCI NUMBERS 3 of a new formula for pn) as a finite sum of algebraic numbers. The Ono-Bruinier formula for pn) however is by no means elementary: the algebraic numbers in question are singular moduli for a Γ 0 6) weight 2 meromorphic modular form expressible in terms of the quasimodular Eisenstein series E 2 z) := 24 dq n and the Dedeind eta function ηz) := e πiz/2 n= n= d n e 2πizn ). Often one wishes to consider sets of partitions where there is some restriction on which parts may appear. Perhaps the most famous identity in the theory of partitions is Theorem Euler s partition theorem). The number of partitions of n into odd parts equals the number of partitions of n into distinct parts. For example consider the partitions of 8 into distinct parts: 8 7 + 6 + 2 5 + 3 5 + 2 + 4 + 3 +. There are six in all. Now consider the partitions of 8 into odd parts: 7 + 5 + 3 5 + + + 3 + 3 + + 3 + + + + + + + + + + + + Again there are six in all. Notice that while Theorem predicts that there are the same number of partitions of 8 into distinct parts as there are partitions of 8 into odd parts the fact that there happen to be six such partitions in each class is not predicted by Theorem. Let qn) denote the number of partitions of n into odd parts or into distinct parts. THen qn) may be computed via the recurrence { if n = mm + )/2 qn) + ) q n 3 + )) + q n 3 )) = 0 otherwise = which is Theorem in [3]. Euler proved Theorem in a boo published in 748 [4 p. 275] using generating functions. The first bijective proof of Theorem was given by J. W. L. Glaisher [5] in 883. For a thorough yet gentle exposition of these two proofs of Theorem please see Chapters 5 and 2 respectively of Andrews and Erisson s boo Integer Partitions []. It would seem natural to see an analogous identity involving compositions of n with odd parts. We offer: Theorem 2. The number of compositions of n into odd parts equals the number of compositions of n + into parts greater than one.

4 ANDREW V. SILLS Theorem 2 is an immediate consequence of two older results: Cayley [3] showed that the number of compositions of n + into parts greater than one equals the nth Fibonacci number F n. That the number of compositions of n into odd parts equals F n is observed a number of places in the literature. The earliest reference this author found was in Volume of Richard Stanley s Enumerative Combinatorics [5 p. 46 ex. 4] which was published in 986. However it seems liely that the result is much older. Here we define F n by F 0 = 0 F = and F n = F n + F n 2 when n 2. Our objective in the next section is to provide a bijective proof of Theorem 2. But before doing so we need to introduce the conjugate of a composition. The conjugate c of a composition c is the composition obtained from c by taing the bit complement of the MacMahon bit sequence of c i.e. change all of the zeros to ones and vice versa. Thus the conjugate of the composition 2 + 4 + + + 5 is + 2 + + + 4 + + + + because the MacMahon bit sequence of the former is while that of the latter is 000 0 0000 0 000. 2. Bijective proof of Theorem 2 with a guiding example Let us begin with a composition a of n into l parts a + a 2 + + a l in which each each part a i is odd. We wish to map a to a composition of n + in which all parts are greater than. As we proceed let us visualize an example. Let us tae a to be +++9+++5+3 which has MacMahon bit sequence 00000000 0000 00. Notice that because all of the parts in a are odd the corresponding MacMahon bit sequence must have zeros appear in strings of even length. Let us now map a to its conjugate composition a which is a composition of n of length n l +. The number of parts in a must be odd as n and l must be of the same parity from the elementary fact that the sum of an even number resp. odd number) of odd integers is even resp. odd). Recalling that the MacMahon bit sequence of a has all of its zeros appearing in strings of even length the MacMahon bit sequence for a must have the property that all of its ones appear in strings of even length. In our example we have the MacMahon bit sequence of a as 000 000 0 so in our example a is 4 + + + + + + + + 4 + + + + 2 + +. That the bit sequence of a consists of pairs of ones sometimes separated by some zeros) means that every even index part i.e. the second fourth sixth etc. part must be a.

COMPOSITIONS PARTITIONS AND FIBONACCI NUMBERS 5 Thus let us map a to the composition b obtained from a +a 2+ +a n l+ by summing adjacent pairs of parts i.e. let b i = a 2i + a 2i for i = 2... n l; and let the last part of b equal the last part of 2 a : b n l 2 + = a n l+. So in our example we have b given by 5 + 2 + 2 + 2 + 5 + 2 + 3 +. Thus we see that b is almost our target; it is a composition of n where all parts other than the last part are greater than. But this is easily fixed. Simply map b to the composition c obtained from b by increasing the last part of b by one. Thus c is a composition of n + in which all parts are greater than one as desired. In our example we have that the image of + + + 9 + + + 5 + 3 is 5 + 2 + 2 + 2 + 5 + 2 + 3 + 2. The steps are easily reversible: begin with a composition of n + into parts greater than one reduce the last part by split each part j other than the last part) into the pair of parts j and conjugate the resulting composition. The final composition is a composition of n with all parts odd. 3. Commentary on enumeration Theorem 2 tells us that the number of compositions of n into odd parts equals the number of compositions of n + into parts greater than one but does not indicate how many such compositions there are for a given n. Liewise Euler s Theorem indicates that there are as many partitions of n into odd parts as there are partitions of n into distinct parts but does not indicate how many such partitions there are for a given n. The first to find an exact explicit formula for the number qn) of partitions of n into odd parts was Loo-Keng Hua [9 p. 95]. Later Peter Hagis [7] gave the following Rademacher-type convergent series representation for qn). where qn) = and once again π 24n + 2 th ) = h< gcdh)= j= x)) := exp πi th ) 2nh )) )) 2j h2j ) 2 { x x 2 if x Z 0 if x Z ) ) I π 48n + 2 2 ) 5) and I z) is the modified Bessel function of order [6 p. 77 Eq. 2)]. In contrast letting Qn) denote the number of compositions into odd parts we have the very simple formula Qn) = F n. 6)

6 ANDREW V. SILLS It is an easy exercise to establish Eq. 6) combinatorially as in [6]. Of course Binet s formula immediately implies ) n ) n + 5 5 Qn) = 2 n 5 giving us a direct non-recursive formula for Qn) that is much simpler than anything nown for qn). However this formula for Qn) is not useful for large values of n because of the roundoff error generated in computing ± 5) n. The theory of partitions has a longer and more varied literature than that of compositions. Perhaps this is due to mathematicians feeling that the theory of partitions is deeper and hence more interesting than that of compositions. After all the generating function for pn) is a certain infinite product which up to a trivial multiple) just so happens to be a modular form. On the other hand the generating function for cn) can easily be seen using ) and then summing the geometric series to be cn)x n = n= n= 2 n x n = x 2x a mere rational function. But before we too hastily dismiss compositions as the less worthy relatives of partitions let us turn bac to Euler s partition theorem Theorem ) for some further inspiration. Because Theorem involves partitions into odd parts we considered compositions into odd parts. But Theorem also involves partitions into distinct parts. So what about compositions into distinct parts? These are not so easily dealt with. We can mae a start by observing that for any partition into l distinct parts there corresponds l! compositions into l distinct parts. Using ideas that follow from Euler s it can be shown that the generating function for partitions into l distinct parts is x ll+)/2 x) x 2 ) x 3 ) x l ) and thus the generating function for compositions into l distinct parts is x ll+)/2 l! x) x 2 ) x 3 ) x l ) and thus the generating function for compositions into distinct parts is x ll+)/2 l! x) x 2 ) x 3 ) x l ) l=0 a far cry from the simplicity of the generating function for cn). In fact in a 995 paper [2] entitled Compositions with distinct parts Bruce Richmond and Arnold Knopfmacher remar that their analysis is more complicated than is usual for compositions problems. The results imply however that the behaviour of these functions is of comparable complexity to partition problems.

COMPOSITIONS PARTITIONS AND FIBONACCI NUMBERS 7 Acnowledgements The author thans George Andrews for suggesting that he loo for a bijective proof of Theorem 2. The author also thans the referee for maing a number of helpful suggestions. References [] G. E. Andrews and K. Erisson Integer Partitions Cambridge University Press 2004. [2] J. Bruiner and K. Ono Algebraic formulas for the coefficients of half-integral weight harmonic wea Maass forms preprint 20. http://www.aimath.org/news/partition/brunier-ono [3] A. Cayley Theorems in trigonometry and on partitions Collected Mathematical Papers vol. 0 6. [4] L. Euler Introduction to Analysis of the Infinite: Boo I translation of Introductio in Analysin Infinitorum 748) to English from the original Latin by J. D. Blanton Springer-Verlag 988. [5] J. W. L. Glaisher A theorem in partitions Messenger of Math. 2 883) 58 70. [6] R. P. Grimaldi Compositions with odd summands Congressus numerantium 42 2000) 3 27. [7] P. Hagis Partitions into odd summands Amer. J. Math. 85 963) 23 222. [8] G. H. Hardy and S. Ramanujan Asymptotic formulae in combinatory analysis Proc. London Math Soc. 2) 7 98) 75 5. [9] L.-K. Hua On the partitions of a number into unequal parts Trans. Amer. Math. Soc. 5 942) 94 20. [0] P. A. MacMahon Combinatory Analysis vol. Cambridge: at the University Press 95. [] H. Rademacher On the partition function pn) Proc. London Math Soc. 2) 37 937) 24 254. [2] B. Richmond and A. Knopfmacher Compositions with distinct parts Aequationes Math. 49 995) 86-97. [3] K. Ono N. Robbins and B. Wilson Some recurrences for arithmetical functions J. Indian Math. Soc. 62 996) 29 5. [4] P. Shiu Computations of the partition function Math. Gazette 8 997) 45 52. [5] R. P. Stanley Enumerative Combinatorics vol. Wadsworth 986; reissued Cambridge 999. [6] G. N. Watson A Treatise on the Theory of Bessel Functions 2nd ed. Cambridge Univ. Press 966. AMS Classification Numbers: B39 05A7 Department of Mathematical Sciences Georgia Southern University Statesboro Georgia 30460-8093 USA E-mail address: asills@georgiasouthern.edu