On Sat, Jul 11, 2020 at 05:28:55AM +0300, h-x h.-x wrote:
> Thank you for your explanation!
> I followed your steps somewhat, and I'm sorry in advance for putting here
> this blob of mathcad worksheet, but
> there was no way I could handle all that manually, and I feel taking
> screenshots from a live sheet is the simplest way
> to show how I worked my way through...
> [image: image.png]
> ...at least not yet... BUT, at this point, B, which is a poly in t with
> coefficients in ???(x), will have to be a multiple of BSR?? in order to "bring
> BSR up";
> then we could collect further "around" BSR...
>
> -- and, finally, B and B' have the same degree as polynomials in exp(ix),
> and the multiple of (t??-1)(t??+1) in the second summand
> will never vanish, and we need it to vanish in order to obtain the*
> constant expression* you denoted as c (which I estimated to be 1/sqrt(2))?
>
> Do I understand you correctly?
>
> So, for this example, the only part that remains a mystery is the structure
> theorem that dictates that we shall look for the antiderivative in form
> (B/t)*BSR + W,
> both B and W from ???(x)[t], and we search for them by differentiating said
> form and checking if such polys are even possible...
>
> No possibilities for new logarithms in the answer?
Well, W contains all logarithms. Let me state basic principle
first: function that have no finite poles is of form
A + B*BSR
where BSR is as you wrote and A and B are in Q(x)[t]. Without
root this is well known, at least when you write K=Q(x) and
consider elements of K(t). Now, usual proof of this in case
of K(t) uses unique factorization in K[t]. It is known that
after extending K(t) by our square root we no longer have
unique factorization in K[t] extended by the root (which
is natural ring if one wants to ape transcendental theory).
Fortunately, for looking at poles it is enough to work
using K[t] as a base ring and consider modules over it.
To fix notation I will use L to denote K(t) extended by
square root and f to dentote integrand.
One can check that derivative of logarithm can not
have pole at t=0. Since our f have poles there,
those poles must come from derivative of element of L,
call it g. So f - g' has no pole at 0. Also, f has
no finte poles outside 0. Outside 0 logarithm give
only poles of multiplicity 1. OTOH if g has finite
pole outside 0, then g' has multiple pole. Multiple pole
can not cancel with pole of multiplicity 1. So,
g has no finite poles outside 0. Any element of L
can be written as
C + D*BSR
where BSR is the root and A, B are in K(t). In particular
g = C + D*BSR
with appropriate C and D. As we argued, g has no finite
poles outside 0. At 0 g has pole of multiplicity 1. It
is easy to see that replacing BSR by -BSR in all formulas
we will get valid equality (this replacement can be vieved
as using Galois theory, but is an easy special case).
Using such replacement one can see that C = 0. Our
argument about poles means that D has pole of multiplicity 1
at 0 and no other finite poles. Consequently,
D = t^(-1)*B
where B is in K[t]. Now, B = b + t*E where E is in K[t], so
g = b*t^(-1) + E
Differentiating E*BSR we see that it has no pole at 0, so
in order for
f - g'
to have no pole at 0, we need
f - (b*t^(-1)*BSR)'
to have no pole at 0. Now we expand both terms into powers of t.
To have on pole at 0 coefficients of t^(-1) must cancel which
leads to equation that I gave previously:
c = b' - ib/2
Solution to this equation is exponential, so not in K = Q(x).
Comparing to your argument, we do not look at higher terms in B.
In fact, in cases where we can integrate by parts (solve equation
similar to the above), we stop once we arrive at t^0 in power
series expansion. We need to do similar thing at infinity
(in practice we replace t by t^(-1) and change root to match).
This ends one stage if integration procedure. After this
stage we have reduced problem to integrand which has no poles
at 0 and at infinity and ony poles of multiplicity 1 at
other places. Now we need to determine logarithmic part.
Here, lack of unique factorization is more serious.
Explaining what to do with logarithmic would make this
message much longer, so today I stop here.
--
Waldek Hebisch