Difference between revisions of "Pell equation"
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− | A '''Pell equation''' is a type of [[diophantine equation]] in the form <math>x^2-Dy^2 = | + | A '''Pell equation''' is a type of [[diophantine equation]] in the form <math>x^2-Dy^2 = \pm1</math> for a [[natural number]] <math>D</math>. Generally, <math>D</math> is taken to be square-free, since otherwise we can "absorb" the largest square factor <math>d^2 | D</math> into <math>y</math> by setting <math>y' = dy</math>. |
− | + | Note that if <math>D = d^2</math> is a perfect square, then this problem can be solved using [[difference of squares]]. We would have <math>x^2 - Dy^2 = (x+dy)(x-dy) = 1</math>, from which we can use casework to quickly determine the solutions. | |
− | Alternatively, | + | Alternatively, if D is a nonsquare then there are infinitely many distinct solutions to the pell equation. To prove this it must first be shown that there is a single solution to the pell equation. |
+ | |||
+ | Claim: If D is a positive integer that is not a perfect square, then the equation <math>x^2-Dy^2 = 1</math> has a solution in positive integers. | ||
+ | |||
+ | Proof: Let <math>c_{1}</math> be an integer greater than 1. We will show that there exists integers <math>t_{1}</math> and <math>w_{1}</math> such that <math>t_{1}-w_{1}\sqrt{D} < \frac{1}{c_{1}}</math> with <math>w_{1} \le c_{1}</math>. Consider the sequence <math>l_{k} = [k\sqrt{D}+1] \rightarrow 0 \le l_{k}-k\sqrt{d} \le 1</math> <math>\forall</math> <math>0 \le k \le c_{1}</math>. By the pigeon hole principle it can be seen that there exists i, j, and p such that i < j, <math>0\le i, j, p, \le c_{1}</math> and | ||
+ | |||
+ | <math>\frac{p-1}{c_{1}} < l_{i}-i\sqrt{D} \le \frac{p}{c_{1}}, \frac{p-1}{c_{1}} < l_{j}-j\sqrt{D} \le \frac{p}{c_{1}}\rightarrow (l_{j}-l_{i})-(j-i)\sqrt{D} < \frac{1}{c_{1}} \rightarrow t_{1} = l_{j}-l_{i}, w_{1} = j-i</math>. | ||
+ | |||
+ | So we now have | ||
+ | |||
+ | <math>t_{1}-w_{1}\sqrt{D} < \frac{1}{c_{1}} \rightarrow t_{1}+w_{1}\sqrt{D} < 2w_{1}\sqrt{D}+1\rightarrow t_{1}^2-Dw_{1}^2 < 2\frac{w_{1}}{c_{1}}\sqrt{D}+\frac{1}{c_{1}}<2\sqrt{D}+1</math>. | ||
+ | |||
+ | We can now create a sequence of <math>t_{n}, w_{n}, c_{n}</math> such that <math>t_{n}-w_{n}\sqrt{D} < \frac{1}{c_{n}}, t_{n}^2-Dw_{n}^2 < 2\sqrt{D}+1</math> and <math>t_{n}-w_{n}\sqrt{D} > \frac{1}{c_{n+1}}</math> which implies <math>t_{s} \not= t_{r}</math> <math>\forall</math> r and s. However we can see by the pigeon hole principle that there is another infinite sequence which will be denoted by <math>t_{y_{k}}, w_{y_{k}}</math> such that <math>t_{y_{k}}^2-Dw_{y_{k}}^2 = h < 2\sqrt{D}+1</math>. Once again, from the pigeon hole principle we can see that there exist integers f and g such that <math>t_{y_{f}}^2-Dw_{y_{f}}^2 = t_{y_{g}}^2-Dw_{y_{g}}^2 = H, t_{y_{f}} = t_{y_{g}}</math> mod H, <math>w_{y_{f}} = w_{y_{g}}</math> mod H, and <math>\frac{t_{y_{f}}}{w_{y_{f}}} \not= \frac{t_{y_{g}}}{w_{y_{g}}}</math>. Define <math>X = t_{y_{f}}t_{y_{g}}-Dw_{y_{f}}w_{y_{g}}, Y = t_{y_{f}}w_{y_{g}}-t_{y_{g}}w_{y_{f}}</math> and notice that <math>X^2-DY^2 = H^2</math>. Also note that <math>X = t_{y_{f}}t_{y_{g}}-Dw_{y_{f}}w_{y_{g}} = t_{y_{f}}^2-Dw_{y_{f}}^2 = 0</math> mod H which means that Y = 0 mod H also. We can now see that <math>\frac{X}{H}, \frac{Y}{H}</math> is a nontrivial solution to pell's equation. | ||
== Family of solutions == | == Family of solutions == | ||
− | + | Let <math>(x_{0}, y_{0})</math> be the minimal solution to the equation <math>x^2-Dy^2 = 1</math>. Note that if <math>(a,b), (c, d)</math> are solutions to this equation then <math>(a^2-Db^2)(c^2-Dd^2) = (ac+Dbd)^2-D(cb+ad)^2 = 1</math> which means <math>(ac+Dbd, cb+ad)</math> is another solution. From this we can guess that <math>(x_{n}, y_{n})</math> is obtained from <math>(x_{0}^2-Dy_{0}^2)^{n+1}</math>. This does indeed generate all the solutions to this equation. Assume there was another solution <math>(p, q)</math>. If <math>(p,q)</math> is non-minimal, then there exists some integer <math>m</math> such that | |
+ | |||
+ | <math>x_{m}+\sqrt{D}y_{m} < p+\sqrt{D}q < x_{m+1}+\sqrt{D}y_{m+1}</math> | ||
+ | |||
+ | Next, multiply the inequality by <math> x_{m}-\sqrt{D}y_{m}</math> to obtain: | ||
+ | |||
+ | <math>1 < (p+\sqrt{D}q)(x_{m}-\sqrt{D}y_{m}) = (px_{m}-Dqy_{m})+\sqrt{D}(qx_{m}-py_{m})< x_{0}+y_{0}\sqrt{D}</math>. | ||
+ | |||
+ | However, it can be seen that | ||
+ | |||
+ | <math>(px_{m}-Dqy_{m})^2-D(qx_{m}-py_{m})^2 = (p+\sqrt{D}q)(x_{m}-\sqrt{D}y_{m})(p-\sqrt{D}q)(x_{m}+\sqrt{D}y_{m}) = 1</math> | ||
+ | |||
+ | Meaning <math>(px_{m}-Dqy_{m}, qx_{m}-py_{m})</math> is a solution smaller than the minimal solution which is a contradiction. | ||
+ | |||
+ | Therefore, such <math>(p,q)</math> cannot exist and so the method of composition generates every possible solution to Pell's equation. | ||
+ | |||
+ | For a Pell equation in form of <math>x^2-Dy^2 = 1</math>, its roots are in the form of <math>(x_{0} + \sqrt{D}y_0)^k</math>, in which <math>x_{0}</math> and <math>y_{0}</math> are the elementery roots of the Pell equation. | ||
− | + | Q.E.D. | |
== Continued fractions == | == Continued fractions == | ||
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== Generalization == | == Generalization == | ||
A '''Pell-like equation''' is a diophantine equation of the form <math>x^2 - Dy^2 = k</math>, where <math>D</math> is a natural number and <math>k</math> is an integer. | A '''Pell-like equation''' is a diophantine equation of the form <math>x^2 - Dy^2 = k</math>, where <math>D</math> is a natural number and <math>k</math> is an integer. | ||
+ | |||
+ | ==Introductory Problems== | ||
+ | |||
+ | Show that if <math>x</math> and <math>y</math> are the solutions to the equation <math>x^2 - 2y^2 = 1</math>, then <math>6\mid xy</math>. | ||
+ | |||
+ | ==Intermediate Problems== | ||
+ | *Find the largest integer <math>n</math> satisfying the following conditions: | ||
+ | :(i) <math>n^2</math> can be expressed as the difference of two consecutive cubes; | ||
+ | :(ii) <math>2n + 79</math> is a perfect square. ([[2008 AIME II Problems/Problem 15|Source]]) | ||
[[Category:Number theory]] | [[Category:Number theory]] |
Latest revision as of 09:20, 29 October 2023
A Pell equation is a type of diophantine equation in the form for a natural number . Generally, is taken to be square-free, since otherwise we can "absorb" the largest square factor into by setting .
Note that if is a perfect square, then this problem can be solved using difference of squares. We would have , from which we can use casework to quickly determine the solutions.
Alternatively, if D is a nonsquare then there are infinitely many distinct solutions to the pell equation. To prove this it must first be shown that there is a single solution to the pell equation.
Claim: If D is a positive integer that is not a perfect square, then the equation has a solution in positive integers.
Proof: Let be an integer greater than 1. We will show that there exists integers and such that with . Consider the sequence . By the pigeon hole principle it can be seen that there exists i, j, and p such that i < j, and
.
So we now have
.
We can now create a sequence of such that and which implies r and s. However we can see by the pigeon hole principle that there is another infinite sequence which will be denoted by such that . Once again, from the pigeon hole principle we can see that there exist integers f and g such that mod H, mod H, and . Define and notice that . Also note that mod H which means that Y = 0 mod H also. We can now see that is a nontrivial solution to pell's equation.
Contents
Family of solutions
Let be the minimal solution to the equation . Note that if are solutions to this equation then which means is another solution. From this we can guess that is obtained from . This does indeed generate all the solutions to this equation. Assume there was another solution . If is non-minimal, then there exists some integer such that
Next, multiply the inequality by to obtain:
.
However, it can be seen that
Meaning is a solution smaller than the minimal solution which is a contradiction.
Therefore, such cannot exist and so the method of composition generates every possible solution to Pell's equation.
For a Pell equation in form of , its roots are in the form of , in which and are the elementery roots of the Pell equation.
Q.E.D.
Continued fractions
The solutions to the Pell equation when is not a perfect square are connected to the continued fraction expansion of . If is the period of the continued fraction and is the th convergent, all solutions to the Pell equation are in the form for positive integer .
Generalization
A Pell-like equation is a diophantine equation of the form , where is a natural number and is an integer.
Introductory Problems
Show that if and are the solutions to the equation , then .
Intermediate Problems
- Find the largest integer satisfying the following conditions:
- (i) can be expressed as the difference of two consecutive cubes;
- (ii) is a perfect square. (Source)