Just derived a method to compute exact entries for powers of the (square) matrix-operator for T-tetration.
It is applicable to positive integer powers only, but for any base.
The restriction to positive integer powers lets look such solutions useless, since integer iteration-height can easily computed just using the scalar values. But I'll use this for further analysis of powerseries, series of powertowers and hopefully one time for the fractional iteration...
Let's use the following notational conventions:
Then the entries for positive integer powers of T can be finitely computed and are "exact", as far as we assume scalar logarithms and exponentials as exact:
This finding is interesting, because in my matrix-method I had to use fixpoint-shift to get exact entries even for integer powers, and since the fixpoints for T-tetration are real only for a small range of bases we had to deal with complex-valued U-matrices when considering the general case. Here we do not need a fixpoint-shift.
I did not check how this computation is related to Ioannis Galidakis' method for exact entries yet, but I think, this is interesting too.
Here is the top left of the symbolic T^2, where lambda=log(b). Each row has to be multiplied by the entry in the most left column and each column must also be multiplied by the entry in the first row.
Here is the top left of the symbolic T^3. (b^^2 means b^b). Legend as before
The difference between the symbolic computation and the simple matrixpower is interesting. I used dim=64x64, base b=sqrt(2), which provides a good approximation when the simple matrix-power is computed. Here are two (zoomed) images: very good aproximation in the leading 12 columns (abs differences to the exact values <1e-20 ), but in the columns 52 to 63 the differences grow up to absolute values greater than 1e10. Surely I "knew" that differences should occur, but I hadn't guessed, that they are so large - I just didn't investigate this in detail.
The leading first twelve columns of the matrix of differences:
The twelve rightmost columns:
The large errors are actually still relatively small for that base b=sqrt(2). A measure for the quality of approximation is, whether the resulting vector of V(x)~*T^3 = Y~ is actually vandermonde and thus Y = V(y) .
This means, that the ratios of logarithms of its entries : log(Y[k])/log(Y[1]), k=0..63, should give the exact sequence [0,1,2,3,...], because this means, that Y contains indeed the consecutive powers of Y[1].
Here is a table of that ratios. ( Remember: we check the col-sums of the third power of T, using x=1)
For base b=2 this looks already catastrophic for the "naive"-computation:
It is obvious, that we should use the "exact" (symbolic) description, if we ever explicitely consider powers of the tetration-matrix T.
It is applicable to positive integer powers only, but for any base.
The restriction to positive integer powers lets look such solutions useless, since integer iteration-height can easily computed just using the scalar values. But I'll use this for further analysis of powerseries, series of powertowers and hopefully one time for the fractional iteration...
Let's use the following notational conventions:
Code:
´
b^^h - the powertower of height h using base b
V(x) - the vandermonde-column-vector containing consecutive powers of its parameter x:
V(x) = column(1,x,x^2,x^3,...)
dV(x) - used as diagonal-matrix
T - the matrix which performs T-tetration to base b (in our forum:"exp_b°t(x)" ):
V(x)~ * T = V(b^x)~
U - the matrix which performs U-tetration to base b (in our forum:"dxp_b°t(x)" ):
V(x)~ * U = V(b^x - 1) ~
Note, that U is lower triangular.
The triangularity allows to compute exact entries for the integer matrix-powers.Then the entries for positive integer powers of T can be finitely computed and are "exact", as far as we assume scalar logarithms and exponentials as exact:
Code:
´
T^2 = U*dV(b^^0) * T*dV(b^^1)
T^3 = U*dV(b^^0) * U*dV(b^^1) * T*dV(b^^2)
...
T^h = prod_{k=0}^{h-2} (U * dV(b^^k))
* (T * dV(b^^(h-1)))I did not check how this computation is related to Ioannis Galidakis' method for exact entries yet, but I think, this is interesting too.
Here is the top left of the symbolic T^2, where lambda=log(b). Each row has to be multiplied by the entry in the most left column and each column must also be multiplied by the entry in the first row.
Here is the top left of the symbolic T^3. (b^^2 means b^b). Legend as before
The difference between the symbolic computation and the simple matrixpower is interesting. I used dim=64x64, base b=sqrt(2), which provides a good approximation when the simple matrix-power is computed. Here are two (zoomed) images: very good aproximation in the leading 12 columns (abs differences to the exact values <1e-20 ), but in the columns 52 to 63 the differences grow up to absolute values greater than 1e10. Surely I "knew" that differences should occur, but I hadn't guessed, that they are so large - I just didn't investigate this in detail.
The leading first twelve columns of the matrix of differences:
The twelve rightmost columns:
The large errors are actually still relatively small for that base b=sqrt(2). A measure for the quality of approximation is, whether the resulting vector of V(x)~*T^3 = Y~ is actually vandermonde and thus Y = V(y) .
This means, that the ratios of logarithms of its entries : log(Y[k])/log(Y[1]), k=0..63, should give the exact sequence [0,1,2,3,...], because this means, that Y contains indeed the consecutive powers of Y[1].
Here is a table of that ratios. ( Remember: we check the col-sums of the third power of T, using x=1)
Code:
´
column symbolic "naive" difference
------------------------------------------------------------
0 -1.13831366798E-19 0.E-201 -1.13831366798E-19
1 1.00000000000 1.00000000000 0.E-202
2 2.00000000000 2.00000000000 1.11189479752E-19
3 3.00000000000 3.00000000000 2.20208219209E-19
4 4.00000000000 4.00000000000 3.27448139227E-19
....
42 42.0000000000 42.0000000000 1.19448154596E-11
43 43.0000000000 43.0000000000 3.09972987348E-11
44 44.0000000000 43.9999999999 7.77154497620E-11
45 45.0000000000 44.9999999998 1.88541576938E-10
46 46.0000000000 45.9999999996 0.000000000443257385765
47 47.0000000000 46.9999999990 0.00000000101122118773
48 48.0000000000 47.9999999978 0.00000000224146913405
49 49.0000000000 48.9999999952 0.00000000483322217091
50 50.0000000000 49.9999999899 0.0000000101495726916
51 51.0000000000 50.9999999792 0.0000000207790885254
52 52.0000000000 51.9999999585 0.0000000415151935602
53 53.0000000000 52.9999999190 0.0000000810212593226
54 54.0000000000 53.9999998454 0.000000154592714129
55 55.0000000000 54.9999997114 0.000000288630924056
56 56.0000000000 55.9999994723 0.000000527723771045
57 57.0000000000 56.9999990544 0.000000945602091679
58 58.0000000000 57.9999983383 0.00000166172556358
59 59.0000000000 58.9999971341 0.00000286585838319
60 60.0000000000 59.9999951463 0.00000485372880576
61 61.0000000000 60.9999919223 0.00000807772027087
62 62.0000000000 61.9999867825 0.0000132174922318
63 63.0000000000 62.9999787236 0.0000212764324046For base b=2 this looks already catastrophic for the "naive"-computation:
Code:
´
column symbolic "naive" difference
------------------------------------------------------------
0 -4.36636233681E-20 0.E-202 -4.36636233681E-20
1 1.00000000000 1.00000000000 0.E-202
2 2.00000000000 2.00000000000 2.46662212171E-14
3 3.00000000000 2.99999999998 2.31650095614E-11
4 4.00000000000 3.99999999669 0.00000000331064284896
5 5.00000000000 4.99999985867 0.000000141325875791
6 6.00000000000 5.99999733964 0.00000266036059669
....
50 50.0000000000 37.9413247398 12.0586752602
51 51.0000000000 38.3796009369 12.6203990631
52 52.0000000000 38.8098393554 13.1901606446
53 53.0000000000 39.2323121795 13.7676878205
54 54.0000000000 39.6472796473 14.3527203527
55 55.0000000000 40.0549905348 14.9450094652
56 56.0000000000 40.4556826502 15.5443173498
57 57.0000000000 40.8495833279 16.1504166721
58 58.0000000000 41.2369099170 16.7630900830
59 59.0000000000 41.6178702587 17.3821297413
60 60.0000000000 41.9926631496 18.0073368504
61 61.0000000000 42.3614787893 18.6385212107
62 62.0000000000 42.7244992089 19.2755007911
63 63.0000000000 43.0818986820 19.9181013180It is obvious, that we should use the "exact" (symbolic) description, if we ever explicitely consider powers of the tetration-matrix T.
Gottfried Helms, Kassel

