JSH has given this parametric solution to x^2 - d y^2 = 1, with d = f1
f2 + 1:
x(v) = (f1 + f2 v^2)/(f1 - f2 v^2 - 2 v) - (2 d v/(f1 - f2 v^2 - 2 v) +
1 - (f1 + f2 v^2)/(f1 - f2 v^2 - 2 v))/(d - 1)
y(v) = (2 d v/(f1 - f2 v^2 - 2 v) +
1 - (f1 + f2 v^2)/(f1 - f2 v^2 - 2 v))/(d - 1)
(For some reason, he keeps giving those, even though they can be
considerably simplified:
x(v) = (f1^2 - 2 f1 v + (1 + d) v^2) / (f1^2 - 2 f1 v - (-1 + d) v^2)
y(v) = -(2 v (-f1 + v)) / (f1^2 - 2 f1 v - (-1 + d) v^2),
but I digress).
Let's look at these for d = 2, f1 = f2 = 1. Then we have:
x(v) = (-1 + 2 v - 3 v^2) / (-1 + 2 v + v^2)
y(v) = (2 (-1 + v) v) / (-1 + 2 v + v^2)
Let's take the positive solutions of the Pell equation, x^2 - 2 y^2 = 1,
and see what values we have to set v to in order to get those solutions.
Here's the first 20 convergents of the continued fraction for sqrt(2):
1
3/2
7/5
17/12
41/29
99/70
239/169
577/408
1393/985
3363/2378
8119/5741
19601/13860
47321/33461
114243/80782
275807/195025
665857/470832
1607521/1136689
3880899/2744210
9369319/6625109
22619537/15994428
Every other one of these, starting at the second, corresponds to a
solution to the Pell equation. Here are those solutions, in the form
x,y {{v->n/m}}
which means that the solution x, y is found by setting v to n/m in JSH's
parametric solution.
3,2 {{v->1/3}}
17,12 {{v->2/5}}
99,70 {{v->7/17}}
577,408 {{v->12/29}}
3363,2378 {{v->41/99}}
19601,13860 {{v->70/169}}
114243,80782 {{v->239/577}}
665857,470832 {{v->408/985}}
3880899,2744210 {{v->1393/3363}}
22619537,15994428 {{v->2378/5741}}
Notice anything interesting there? Take a look at the numerators and
denominators of the v's, and compare to the convergents (all the
convergents, not just the half of them that give solutions).
If Pi/Qi is the i'th convergent, the v's are
P1/P2
Q2/Q3
P3/P4
Q4/Q5
...
I think this is a very pretty pattern. It's neat the way the v's are
formed from ratios of the numerators of successive convergents
alternating with the ratios of denominators of successive convergents.
I don't see any obvious pattern like that for any other d I've tried (3,
5, 15, using every possible f1 for each), so this appears like it might
be a property just of 2 (or sqrt(2), I suppose, depending on how you
look at it).
Here's the Mathematica code I used to play around with this:
ClearAll["Global`*"];
y[v_] := (2 d v/(f1 - f2 v^2 - 2 v) +
1 - (f1 + f2 v^2)/(f1 - f2 v^2 - 2 v))/(d - 1)
x[v_] := (f1 + f2 v^2)/(f1 - f2 v^2 -
2 v) - (2 d v/(f1 - f2 v^2 - 2 v) +
1 - (f1 + f2 v^2)/(f1 - f2 v^2 - 2 v))/(d - 1)
d = 2;
f1 = 1;
f2 = (d - 1)/f1;
cv = Convergents[Sqrt[d], 20]
Numerator[cv]^2 - d Denominator[cv]^2
For[i = 2, i <= 20, i += 2, tx = Numerator[cv[[i]]];
ty = Denominator[cv[[i]]];
Print[tx, ",", ty, Solve[{x[v] == tx, y[v] == ty}, v]]]

Signature
--Tim Smith
Tim Smith - 25 Feb 2009 09:47 GMT
> Let's look at these for d = 2, f1 = f2 = 1. Then we have:
>
[quoted text clipped - 3 lines]
> Let's take the positive solutions of the Pell equation, x^2 - 2 y^2 = 1,
> and see what values we have to set v to in order to get those solutions.
...
> If Pi/Qi is the i'th convergent, the v's are
>
[quoted text clipped - 3 lines]
> Q4/Q5
> ...
I took a look at this again, but instead of JSH's parameterization, I
used the simplest one that has been proposed:
x(v) = (v^2 + d) / (v^2 - d)
y(v) = (2v) / (v^2 - d)
That, of course, gives a different sequence of v values for d = 2:
3,2 {{v->2}}
17,12 {{v->3/2}}
99,70 {{v->10/7}}
577,408 {{v->17/12}}
3363,2378 {{v->58/41}}
19601,13860 {{v->99/70}}
114243,80782 {{v->338/239}}
665857,470832 {{v->577/408}}
3880899,2744210 {{v->1970/1393}}
22619537,15994428 {{v->3363/2378}}
But again, the v's are tied to the convergents for sqrt(2) in a simple
pattern:
2 Q1 / P1
P2 / Q2
2 Q3 / P3
P4 / Q4
2 Q5 / P5
...
That pattern isn't as interesting, in my opinion, as the one that arises
out of JSH's parameterization, but, on the other hand, I didn't see any
obvious pattern past d = 2 with the JSH form. With the simpler form,
there is an obvious pattern. Here's d - 5:
Convergents:
2, 9/4, 38/17, 161/72, 682/305, 2889/1292, 12238/5473, 51841/23184, \
219602/98209, 930249/416020, 3940598/1762289, 16692641/7465176, \
70711162/31622993, 299537289/133957148, 1268860318/567451585, \
5374978561/2403763488
Values of v that give Pell solutions:
9,4 {{v->5/2}}
161,72 {{v->9/4}}
2889,1292 {{v->85/38}}
51841,23184 {{v->161/72}}
930249,416020 {{v->1525/682}}
16692641,7465176 {{v->2889/1292}}
299537289,133957148 {{v->27365/12238}}
5374978561,2403763488 {{v->51841/23184}}
96450076809,43133785636 {{v->491045/219602}}
1730726404001,774004377960 {{v->930249/416020}}
Relationship of v to convergents:
5 Q1 / P1
P2 / Q2
5 Q3 / P3
P4 / Q4
5 Q5 / P5
...
Checking a few other values of d, it appears that in general, for
positive integers d where d is not a perfect square, then these are the
values of v that give the successive solutions to x^2 - d y^2 = 1:
d Q1 / P1
P2 / Q2
d Q3 / P3
P4 / Q4
...

Signature
--Tim Smith