It is shown that the sequence has an amusing oscillating behavior and that there are terms that approach for a certain type of large indices

Ibstedt, Henry

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On a Smarandache Partial Perfect Additive Sequence Beary Ibstedt Abstract: The sequence defined through a2t+l=a~wl, a2t+2~I+I for ~l with al=a2=1 is studied in detail. It is proved that the sequence is neither convergent nor periodic - questions which have recently been posed. It is shown that the sequence has an amusing oscillating behavior and that there are terms that approach ± co for a certain type of large indices. Definition of Smarandache perfect ; sequence: If; is a p-ary relation on{ ah a2. a3 • .... } and ;(3i, 3i+t, 3i+2, ... 3i+p-I)= ;(8;. 8;+1, 8;+2, .... 8;+p-I) for all 3i. 8; and all p> 1. then {3n} is called a Smarandache perfect; sequence. If the defining relation is not satisfied for all 3i.8; or all p then {3n} may qualifY as a Smarandache partial perfect; sequence. The purpose of this note is to answer some questions posed in an article in the Smarandache Notions Journal, vol 11 [1] on a particular Smarandache partial perfect sequence defined in the following way: al=a2=1 a2k+l=lik+I-l, ~1 a2k+2=~+1+1, ~l Adding both sides of the defining equations results in a2k+2+a2k+I=2a.:+1 which gives Let n be of the form n=k·2m• The summation formula now takes the form 1e·2'" Ie La; =2mLa; i=1 ; 4 8 2m From this we note the special cases L a i = 4 ,L a i = 8, .... La; = 2m • i=1 i=l i=1 (1) (2) (3) (4) The author of the article under reference poses the questions: "Can you, readers, find a general expression of3n (as a function ofn)? Is the sequence periodical, or convergent or bounded?" The first 25 terms of this sequence are1: k 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 ak 1 1 0 2 -1 1 1 3 -2 0 0 2 0 2 2 4 -3 -1 -1 1 -1 1 1 3-1 1 The sequence as quoted in the article under reference is erroneous as from the thirteenth tenn. 103 It may not be possible to find a general expression for a,. in terms of n. For computational purposes, however, it is helpful to unify the two defining equations by introducing the &-function defined as follows: {-I ifn=O (mod 2) 5(n)= 1 ifn=1 (mod 2) The definition of the sequence now takes the form: aD = a 1+6(D) - o(n) (D+-2-)l2 (5) (6) A translation of this algorithm to computer language was used to calculated the first 3000 terms of this sequence. A feeling for how this sequence behaves may be best conveyed by table 1 of the first 136 terms, where the switching between positive, negative and zero terms have been made explicit. Before looking at some parts of this calculation let us make a few observations. Although we do not have a general formula for a,. we may extract very interesting information in particular cases. Successive application of (2) to a case where the index is a power of2 results in: (7) This simple consideration immediately gives the answer to the main question: The sequence is neither periodic nor convergent. We will now consider the difference 30-30-1 which is calculated using (1) and (2). It is necessary to distinguish between n even and n odd. 1. n=2k, le2. (8) 2. n=k·2m+1 where k is odd. r I-2m ifk=1 ak_2"'+1 - a k_2m = a k_2",-1+1 - 1-a k_2",-1 - 1 = ... a k+1 - a k - 2m = i (9) l2-2m ifk>1 In particular aZk+1-aZk= 0 ifk2:3 is odd. 104 Table I. The first 136 terms of the sequence n an an+l etc 1 1 1 3 0 4 2 5 -1 6 1 1 3 9 -2 10 0 0 12 2 13 0 14 2 2 4 17 -3 -1 -1 20 1 21 -1 22 1 1 3 25 -1 26 1 1 3 1 3 3 5 33 -4 -2 -2 36 0 37 -2 38 0 0 40 2 41 -2 42 0 0 44 2 45 0 46 2 2 4 49 -2 50 0 0 52 2 53 0 54 2 2 4 57 0 58 2 2 4 2 4 4 6 65 -5 -3 -3 -1 -3 -1 -1 72 1 73 -3 -1 -1 76 1 77 -1 78 1 1 3 81 -3 -1 -1 84 1 85 -1 86 1 1 3 89 -1 90 1 1 3 1 3 3 5 97 -3 -1 -1 100 1 101 -1 102 1 1 3 105 -1 106 1 1 3 1 3 3 5 113 -1 114 1 1 3 1 3 3 5 1 3 3 5 3 5 5 7 129 -6 -4 -4 -2 -4 -2 -2 136 0 105 The big drop. The sequence shows an interesting behaviour around the index 2m. We have seen that a2- = m. The next term in the sequence calculated from (9) is m+ 1-2·m=-m+ 1. This makes for the spectacular behaviour shown in diagrams 1 and 2. The sequence gradually struggles to get to a peak for n=2m where it drops to a low and starts working its way up again. There is a great similarity between the oscillating behaviour shown in the two diagrams. In diagram. 3 this behaviour is illustrated as it occurs between two successive peaks. 8.-----------------------.------------------------. 6 4 2 o -2 -4 -6 -8~----------------------------------------------~ Diagram 1. a" as a function of n around n=28 illustrating the "big drop" 10r-----------------------.------------------------. 8 6 4 2 o -2 -4 -6 -8 -10~----------------------------------------------~ Diagram 2. a" as a function of n around n=2 10 illustrating the "big drop" 106 8~-------------------------------------------------, 6 4 2 o -2 ~~------------------------------------------------~ Diagram 3. The oscillating behaviour of the sequence between the peaks for n=27 and n=28. When using the defining equations (1) and (2) to calculate elements of the sequence it is necessary to have in memory the values of the elements as far back as half the current index. We are now in a position to generate preceding and proceeding elements to a given element by using formulas based on (8) and (9), The forward formulas: r lio-l+2 30= ~ lio-l+I-2m llio-l+2-2m when n=2k, k> 1 whenn=2m+I when n=k·2m+l, k>1 Since we know that a2m = m it will also prove useful to calculate 30 from 3n+1. The reverse formulas: r3ow 2 30= ~3owl+2m l3n+I-2+2m when n=2k-l, k>1 whenn=2m when n=k·2m, k>l (10) (11) Finally let's use these formulas to calculate some terms forwards and backwards from one known value say ~o96=12 (4096=2 12), It is seen that an starts from 0 at n=4001, makes its big drop to -11 for n=4096 and remains negative until n=400I. For an even power of 2 the mounting sequence only has even values and the descending sequence only odd values. For odd powers of2 it is the other way round. Table 2. Values ofa" around n=212. 4095 4094 4093 4092 4091 4090 4089 4088 4087 4086 4085 4084 4083 4082 4081 4080 4079 4078 .. , 4001 10 10 8 10 8 8 6 10 8 8 6 8 6 6 4 10 8 8 ... 0 40964097 4098 4099 4100 4101 4102 4103 4104 4105 41064107 4108 4109411041114112 4113... 4160 12 -11 -9 -9 -7 -9 -7 -7 -5 -9 -7 -7 -5 -7 -5 -5 -3 -9 _ References: 1. M. Bencze, Smarandache Relationships and Subsequences, Smarandache Notions Journal. VoL 11, No 1-2-3, pgs 79-85. 107 

Smarandache Relationships and Subsequences,

On a Smarandache Partial Perfect Additive Sequence

https://zenodo.org/record/9375/files/SPPAdditiveSeg.pdf

On a Smarandache Partial Perfect Additive Sequence

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