Re: tetration and logaritms
- From: lwalke3@xxxxxxxxx
- Date: Thu, 10 Jul 2008 01:18:05 -0700 (PDT)
On Jul 9, 11:59 am, amy666 <tommy1...@xxxxxxxxxxx> wrote:
we all know the taylor series for log(1+x) which holds for all real x between -1 and 1.
this series starts with 0 + x - x^2/2 + ...
and from looking at the first terms of this taylor series we see that we can get series reversion which of course gives exp(x) - 1.
fractional iterations can be done for exp(x)-1 since its a taylor series with f(0) = 0. ( and its unique )
and thus also for log(1+x) , either directly since log(1) = 0 or from the series reversion of the fractional iterations of exp(x)-1.
Hmmm, this looks interesting.
Let us return to the U-tetration notation first introduced by
Gottfried Helms. In this notation:
exp(x)-1 = U_e(x,1)
I see no reason why we can't write:
log(1+x) = U_e(x,-1)
and start using negative values for the second parameter of
U_e (which Gottfried calls "h" for "height").
Then tommy1729 is really asking for U_e(x,-1/2). So now I
wonder whether the same matrix that Gottfried would use to
find, say, U_e(x,1/2) would work for U_e(x,-1/2) as well.
I don't have Gottfried's full matrix method available (he's
explained it but it's a bit too complex to follow), but here's
a simpler version that only works for base e. (This is because
Gottfried has discovered that the Taylor coefficients are a
bivariate polynomial that evaluates to 0/0 when the base is
either e or 1/e. But L'Hopital's Rule can be used in this case
to give a polynomial in the single variable h. This trick simply
gives us this polynomial in h.)
Suppose we only want the first five terms of our Taylor
series for U_e(x,h). So we begin with a 6x6 matrix with zeros
everywhere, except on the superdiagonal where it is one. This
matrix corresponds to U_e(x,0) = x, the identity function.
To find the matrix for U_e(x,1), we take the Taylor series for
exp(x)-1 (which is x+x^2/2+x^3/6+x^4/24+x^5/120), plug in the
previous matrix for x. Naturally, this gives us a strictly upper
triangular matrix with 1 on the superdiagonal, then 1/2 on the
diagonal above that, then 1/6 on the next diagonal, and finally
1/24 and 1/120 in the upper-left corner. This tells us that
U_e(x,1) is x+x^2/2+x^3/6+x^4/24+x^5/120 (but this is trivial).
We then repeat the process by plugging in the new matrix for
x in the series for exp(x)-1, to find U_e(x,2). Here we find that
not only does the superdiagonal contain 1, but so does the
diagonal above it. The next diagonal has the value 5/6, and
finally 5/8 and 13/30 in the upper-left corner. So we have that
U_e(x,2) = x+x^2+5x^3/6+5x^4/8+13x^5/120.
Continuing in this manner, we find:
U_e(x,3) = x+3x^2/2+2x^3+5x^4/2+179x^5/60
U_e(x,4) = x+2x^2+11x^3/3+77x^4/12+163x^5/15
We could continue like this forever, but this is all we need
to find the polynomials in h. We simply take the coefficients
for the x, x^2, x^3, ..., terms, view them as functions of h,
and then take the Lagrange interpolating polynomial.
The x terms are trivial: 1, 1, 1, 1, 1. So we see that the
linear coefficient is always 1.
The x^2 terms is also easy. Starting with U_e(x,0) they
form the patten 0, 1/2, 1, 1/2, 2. So the x^2 coefficients
must be h/2.
For x^3 we have 0, 1/6, 5/6, 2, 11/3. The x^3 coefficients
work out to be h^2/4-h/12.
For x^4 we have 0, 1/24, 5/8, 5/2, 77/12. The x^4 coefficients
work out to be h^3/8-5h^2/48+h/48.
For x^5 we have 0, 1/120, 13/30, 179/60, 163/15. The x^5
work out to be h^4/64-13h^3/144-h^2/24-h/180.
Notice that the polynomial for x^n always works out to be a
polynomial in h of degree n-1.
Putting this together, we have the Taylor polynomial
U_e(x,h) = x+(h/2)x^2+(h^2/4-h/12)x^3+(h^3/8-5h^2/48+h/48)x^4
+(h^4/64-13h^3/144-h^2/24-h/180)x^5.
And this seems to work for any _positive_ value of h that
Gottfried chose. So for h = 1/2:
U_e(x,1/2) = x+x^2/4+x^3/48+x^5/3840
And so there's nothing stopping us from letting h be negative:
U_e(x,-1) = x-x^2/2+x^3/3-x^4/4+x^5/5
And this of course is the well-known Taylor series for log(1+x)
that tommy1729 already mentioned in his post. Finally, h=-1/2:
U_e(x,-1/2) = x-x^2/4+5x^3/48-5x^4/96+109x^5/3840
.
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