Notes on Number Theory and Discrete Mathematics
Print ISSN 1310–5132, Online ISSN 2367–8275
Vol. 23, 2017, No. 4, 85–93
Some variations on Fibonacci matrix graphs
Anthony G. Shannon1 and Ömür Deveci2
1
Emeritus Professor, University of Technology Sydney, NSW 2007,
Fellow, Warrane College, University of New South Wales, Kensington NSW 2033,
Director, Academic Affairs, Australian Institute of Music, Sydney NSW 2010, Australia
e-mail:
[email protected]
2
Department of Mathematics, Faculty of Science and Letters,
Kafkas University 36100, Turkey
e-mail:
[email protected]
Received: 12 March 2016
Accepted: 29 October 2017
Abstract: Matrices are here considered in two ways: arrays containing Fibonacci numbers and
their generalizations in the cells, and arrays as graphs where the cells themselves are subgraphs. Both aspects contain ideas for further development and research.
Keywords: Fibonacci, Pell and Eulerian numbers, Pyramidal numbers, Golden section,
Spanning trees, Lattice points.
AMS Classification: 11B39, 05C62.
1
Introduction
With a slight variation of Horadam’s classic systematic and simple summary notation [4] we
consider aspects of some extensions of some of the well-known sequences in Table 1, though
what we elaborate below can be applied to any of these sequences or their generalizations.
Horadam and Mahon studied these together with Chebyshev, Gegenbauer, Humbert and
Stirling analogues [5]. The plan of this paper is to consider {wk ,n ( a, b; p, q )} for
•
arbitrary k in Section 2;
•
fixed k = 2 in Section 3;
•
variable q in Section 4;
•
k = 2 & 3 in Section 5.
85
Sequence
a
b
p
q
wn
0
1
1
–1
Fn
Fibonacci
2
1
1
–1
Ln
Lucas
0
1
2
–1
Pn
Pell
1
3
2
–1
Qn
Pell-Lucas
0
1
x+2
+1
Bn(x)
Morgan–Voyce Even Fibonacci
1
1
x+2
+1
bn(x)
Morgan–Voyce Odd Fibonacci
2
x+2
x+2
+1
Cn(x)
Morgan–Voyce Even Lucas
-1
1
x+2
+1
cn(x)
Morgan–Voyce Odd Lucas
0
1
1
–x
Jn(x)
Jacobstha–Fibonacci
2
1
1
–x
jn(x)
Jacobsthal–Lucas
0
1
x
+1
Vn(x)
Vieta–Fibonacci
2
x
x
+1
vn(x)
Vieta–Lucas
Table 1. Integer and polynomial sequences {w2,n ( a, b; p, q )}
2
A Pell variation
Consider the kth order Pell generalization
{w (1, 2,..., k ; 2, +1)}
k ,n
formed from the recurrence
relation
(2.1)
uk ,n = 2uk , n −1 − uk ,n − k , n ≥ k ,
with initial values uk,j = j, j = 0, 1, 2, 3, ... . Some examples are set out in Table 2.
k↓, n→
1
2
3
4
5
6
7
8
9
10
11
12
13
1
1
1
1
1
1
1
1
1
1
1
1
1
1
2
1
2
3
4
5
6
7
8
9
10
11
12
13
3
1
2
3
5
8
13
21
34
55
89
144
233
377
4
1
2
3
4
7
12
21
38
69
126
231
424
779
5
1
2
3
4
5
9
16
29
54
103
201
393
757
6
1
2
3
4
5
6
11
20
37
70
135
264
517
7
1
2
3
4
5
6
7
13
24
45
86
167
328
8
1
2
3
4
5
6
7
8
15
28
53
102
199
9
1
2
3
4
5
6
7
8
9
17
32
61
118
10
1
2
3
4
5
6
7
8
9
10
19
36
69
Table 2. Patterns among {wk ,n (1,2,..., k ;2,1)}
86
If we consider the elements in the backward diagonals in Table 2, then we can establish
the sequences in Table 3 with the connections with the Eulerian numbers:
E n = 2 n − n − 1, n ≥ 0.
(2.2)
k↓, m→
1
2
3
4
5
6
7
8
9
10
uk,m
m>
1
1
1
1
1
1
1
1
1
1
1
u1, m = 1
0
2
1
2
3
4
5
6
7
8
9
10
u 2,m = m
0
3
1
3
5
7
9
11
13
15
17
19
u 3, m = 2 m − 1
1
4
1
4
8
12
16
20
24
28
32
36
u 4,m = 4m − 4
1
5
1
5
13
21
29
37
45
53
61
69
u 5,m = 8m − 11
2
6
1
6
21
38
54
70
86
102
118
134
u 6, m = 16m − 26
3
7
1
7
34
69
103
135
167
199
231
263
u 7 ,m = 32m − 57
4
8
1
8
55
126
201
264
328
392
456
520
u 8,m = 64m − 120
5
9
1
9
89
231
393
517
649
777
905
1033
10
1
10
144
424
757
1014 1290 1546 1802 2058
u 9 ,m = 128m − 247
u10,m = 256m − 502
6
7
Table 3. Eulerian and generalized Pell numbers
3
Fibonacci matrix variations
The previous tables suggest realigning the columns by dropping the elements in successive
columns to produce Fibonacci rectangular and Lucas square ‘triangular’ matrices as in
Tables 4 and 5.
F10 × 6 =
1
1
1
0
1
2
0
0
0
0
0
0
0
0
0
0
0
0
1
1
1
3
5
8
1
2
3
0
0
1
0
0
0
0
0
0
1
1
1
1
13
21
34
55
5
8
13
21
2
3
5
8
0
1
2
3
0
0
0
0
Table 4. A Fibonacci triangular matrix
87
Thus, F5×1 = [1, 1, 1, 1, 1]T for instance. The ‘left triangle’ parts of these matrices lack
the symmetry that one finds with Pascal-type triangles of these sorts of numbers [11].
Nevertheless, the Fibonacci triangle set out in Table 4 has several properties similar to these
generalizations [9], including the following examples with a variety of row, column and
diagonal properties can be discerned.
Sums of cells:
• row sums are Fibonacci numbers;
• partial row sums {Fn +3 − 2}, j > 1;
•
rising diagonal sums {Fn +1 −
1
2
Fn+1 }.
Partial recurrence relations:
• u i , j = u i −1, j + u i − 2 , j , j > 1;
•
u i , j = u i , j −1 − u i −1, j −1 , i > 1, j > i − 1;
•
u i , j = Fi − 2 j + 4 .
Analogous variations can also be applied to the other sequences to produce companion
matrices [3] and tridiagonal matrices [2]. Instead we now outline a corresponding Lucas
illustration.
L10×10 =
1
1
1
0
2
1
0
0
2
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
1
1
1
3
4
7
1
3
4
2
1
3
0
2
1
0
0
2
0
0
0
0
0
0
0
0
0
0
0
0
1
1
1
1
11
18
29
47
7
11
18
29
4
7
11
18
3
4
7
11
1
3
4
7
2
1
3
4
0
2
1
3
0
0
2
1
0
0
0
1
Table 5. A Lucas triangular matrix
4
Golden ratio variations
Variations of the golden ratio are effectively done by looking at the sequences generated with
different values of q. A Fibonacci golden ratio family of sequences is set out in Table 6 [cf. 10],
and its Lucas counterpart in Table 7 [cf. 17].
Thus one can use Sloane’s encyclopedia for connections and creations [15]. More deeply
one can search for intersections [16] and divisibility properties [7].
88
wn (0,1;1,−q)
1
2
3
4
5
6
7
8
9
10
11
12
wn (0,1;1,0)
1
1
1
1
1
1
1
1
1
1
1
1
wn (0,1;1,−1)
1
1
2
3
5
8
13
21
34
55
89
144
wn (0,1;1,−2)
1
1
3
5
11
21
43
85
171
341
683
1365
wn (0,1;1,−3)
1
1
4
7
19
40
97
217
508
1159
2683
6160
wn (0,1;1,−4)
1
1
5
9
29
65
181
441
1165
2929
7589
19305
wn (0,1;1,−5)
1
1
6
11
41
96
301
781
2286
6191
17621
48576
wn (0,1;1,−6)
1
1
7
13
55
133
463
1261
4039
11605
35839
105469
wn (0,1;1,−7)
1
1
8
15
71
176
673
1905
6616
19951
66263
205920
Table 6. Fibonacci variations
wn (2,1;1,− q )
0
1
2
3
4
5
6
7
8
9
10
11
wn (2,1;1,0)
2
2
2
2
2
2
2
2
2
2
2
2
wn (2,1;1,−1)
2
1
3
4
7
11
18
29
47
76
123
199
wn (2,1;1,−2)
2
1
5
7
17
31
65
127
257
511
1025
2047
wn (2,1;1,−3)
2
1
7
10
31
61
154
337
799
1810
4207
9637
wn (2,1;1,−4)
2
1
9
13
49
101
297
701
1889
4693
12249
31021
wn (2,1;1,−5)
2
1
11
16
71
151
506
1261
3791
10096
29051
79531
wn (2,1;1,−6)
2
1
13
19
97
211
793
2059
6817
19171
60073
175099
wn (2,1;1,−7)
2
1
15
22
127
281
1170 3137 11327 33286 112575 345577
Table 7. Lucas variations
5
Cells in matrices
We now consider the matrix arrays as graphs in themselves. For simplicity, we start with square
matrices which are divided into sub-graphs containing 1, 4, 9, 16, ..., square matrices as
illustrated in Figure 1.
Figure 1. Matrices with 1, 4, 9, 16 cells
Immediately we observe that the number of squares contained in each matrix is 1, 5, 14,
30, 55, ..., the square pyramidal numbers, generated by n(n + 1)(2n + 1)/6, where n2 is the
number of cells contained with the whole matrix. There is a wealth of literature on pyramidal
numbers [17: M3844] which we do not plan to pursue here. Rather we continue to consider
aspects of these subgraphs.
89
Connections with Fibonacci matrices and graphs occur through spanning trees and the
complexity of a graph [6, 12, 14], but many problems remain. For instance, by extending the
squares in Figure 1 through their diagonals, we obtain the planar representation of a trellis (or
wire mesh) fence consists of sets of ‘crosses’ or ‘squares’ as shown in Figure 2.
Figure 2. Representation of a section of trellis (wire-mesh)
Immediately a number of non-trivial questions arise, such as how many squares? symmetric crosses? rectangles? lattice points? crosses (symmetric or asymmetric)? spanning trees?
Attempts to solve the problems are probably best illustrated by construction. In general,
one would expect the solutions to be functions of the numbers of edges and vertices. We define
a trellis of a given size and position in the plane as even or odd:
• an even trellis, fn,m, is the set of integer lattice points {( x, y ) : x + y is even,
0 ≤ x ≤ 2n, 0 ≤ y ≤ 2m};
an odd trellis, gn,m, is the set of integer lattice points {( x, y ) : x + y is odd,
0 ≤ x ≤ 2n, 0 ≤ y ≤ 2m}.
Figures 3 (a), (b), (c), (d) show the cases for ‘fences’ f1,m, f2,m, f3,m , m = 1, 2, 3, respectively,
where {fn,m} represents the set of single-edged symmetric crosses of fences with ‘height’ n and
‘length’ m. Thus in Figure 2, {f2,m}, m = 1, 2, 3, is the set of 3 single-edged symmetric crosses
of height 2 such crosses.
•
(a) f 1,m
(b) f 2,m
(c) f 3,m
(d) g 3, 2
Figure 3. Representation of fences
90
Let en,m be the number of edges in fn,m. Then, since fn,m is constructed by an n × m lattice
of crosses and each cross contributes four edges, it follows that
fn,m = 4nm.
(5.1)
See the black dots in Figure 4 and the entries in Table 8.
Figure 4. f 2 ,3
n↓ m→
1
2
3
4
1
4
8
12
16
2
8
16
24
32
3
12
24
36
48
4
16
32
48
64
5
20
40
60
80
Table 8. e n ,m
Similarly let v n ,m ∈ f n ,m and wn ,m ∈ g n ,m be the corresponding numbers of vertices (Table 9).
n↓ m→
1
2
3
4
1
5
8
11
14
2
8
13
18
23
3
11
18
25
32
4
14
23
32
41
5
17
28
39
50
Table 9. v n ,m
For v n ,m there are nm black dots and (n+1)(m+1) white dots for a total of
v n , m = nm + (n + 1)(m + 1) = 2nm + n + m + 1.
91
(5.2)
Figure 5. g3,6
6
Concluding comments
Various other extensions and generalizations of the sequences in Table 1 can be readily
investigated. For example, just as for the second-order Pell sequences
{P } ≡ {w (0,1;2,−1)}, {Q } ≡ {w (1,3;2,−1)}
2,n
2,n
2,n
2 ,n
there is the connection
(4.1)
Q2 ,n = P2,n + P2,n +1
so too for the corresponding third-order Pell sequences
{P } ≡ {w (0,0,1;2,−1)}, {Q } ≡ {w (1,1,3;2,−1)}
3,n
3, n
3, n
3, n
there is also the connection
Q3, n = P3,n −1 + P3, n + P3,n +1
(5.2)
where the third-order recurrence relation is
w3,n = w3,n −1 + w3,n − 2 , n ≥ 2.
While at one level almost any desired elegant identity can be obtained by a suitable
choice of initial values, the selection can be determined by us with the use of “basic” sequences
and corresponding matrices. At order k, there will be k basic fundamental sequences and one
primordial sequence, and corresponding matrices [13].
More fundamentally though, these ideas provide a source of multitudes of undergraduate
exercises which students generally seem to enjoy both computationally and symbolically, the
latter helping to cultivate a feeling for notation as a tool of thought, not only in mathematics but
also in music [8], two disciplines which share much in common with the creative processes
both in doing and in discovering [1].
92
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[3]
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Journal of Advances in Mathematics, 17(2), 10–24.
[4]
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[5]
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[7]
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93