%I A117691
%S A117691 4,3,3,2,8,5,5,3,12,7,7,4,16,9,9,5,20,11,11,6,24,13,13,7,28,15,15,8,32,
%T A117691 17,17,9,36,19,19,10,40,21,21,11,44,23,23,12,48,25,25,13,52,27,27,14,56,
%U A117691 29,29,15,60,31,31,16,64,33,33,17,68,35,35,18,72,37,37,19,76,39,39,20
%N A117691 Rational numbers in F[n]=(a[m]/b[m])*F[n-1]-F[n-2] that produce harmonic
bouncing ball functions from generalized Fibonacci linear recursions.
%C A117691 This method converts a definite sequence of rational numbers into a sequence
of Integers. The sequences of the type: f[0] = a0; f[1] = b0; f[n_]
:= f[n] = (A[m]/B[m])*f[n - 1] - f[n - 2] and M = {{0, 1}, {-1, (A[m]/
B[m])}}; v[0] = {a0, bo}; v[n_] := v[n] = M.v[n - 1] are important
because they represent an integer based Hilbert space. Becuse it
should be possible to do the equivalent of Fourier expansions in
integer recursions using them. Because you can also define orthogonality
on integer sequences using them.
%C A117691 a(n)= mix A022998(n+2) , A026741(n+3) . A026741 has many links to Bernoulli
numbers (A027641/A027642 or A164555/A027642) and Rydberg-Ritz spectra
of hydrogen,in particular Balmer A061037. A022998 is linked to Balmer
A061038;see A145979. A026741(n-1)+A026741(n+1)=A022998. A022998(n+1)/
A026741(n+1)=period 2:repeat 1,4=A010685 . [From Paul Curtz (bpcrtz(AT)free.fr),
Sep 19 2009]
%F A117691 C[m]=A[m]/B[m] a(n) = {A[m],B[m]}
%t A117691 o = Table[Abs[Coefficient[ExpandAll[(x - (a + I*Sqrt[2*a + 1])/(a + 1))*(x
- ( a - I*Sqrt[2*a + 1])/(a + 1))], x]], {a, 1, 100}] rational =
Table[{Numerator[o[[n]]], Denominator[o[[n]]]}, {n, 2, 100}] Flatten[rational]
%Y A117691 Sequence in context: A120927 A117323 A016502 this_sequence A143487 A031350
A031353
%Y A117691 Adjacent sequences: A117688 A117689 A117690 this_sequence A117692 A117693
A117694
%K A117691 nonn,uned,probation
%O A117691 0,1
%A A117691 Roger L. Bagula (rlbagulatftn(AT)yahoo.com), Apr 12 2006
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