Asymptotic behavior of coefficients

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SUMMARY

The discussion focuses on the asymptotic behavior of coefficients in a three-term recurrence relation defined by \(a_0=1\), \(a_1=p_1(1)a_0\), and \(a_n=p_1(n)a_{n-1}+p_2(n)a_{n-2}\) for \(n \ge 2\). The functions \(p_1(n)\) and \(p_2(n)\) are specified as \(p_1(n)=\frac{\delta^2/\alpha\gamma}{(n+k)^2-\beta^2/\alpha^2}\) and \(p_2(n)=-\frac{1}{(n+k)^2-\beta^2/\alpha^2}\) respectively, where \(k=\pm\frac{\beta}{\alpha}\). The asymptotic forms of the coefficients \(a_n^{(1)}\) and \(a_n^{(2)}\) are derived by treating \(p_1(n)\) and \(p_2(n)\) as constants for large \(n\), leading to the solution \(a_n \sim \left(\frac{\delta^2}{\alpha\gamma}\right)^n\).

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I have a three term recurrence relation

[itex] \[<br /> a_0=1,<br /> \]<br /> \[<br /> a_1=p_1(1)a_0,<br /> \]<br /> \begin{equation}\label{recurr}<br /> \begin{array}{ccc}<br /> a_{n}=p_1(n) a_{n-1}+p_2(n) a_{n-2}, && n\ge2.\\<br /> \end{array}<br /> \end{equation}<br /> [/itex]

where

[itex] \[<br /> p_1(n)=\frac{\delta^2/\alpha\gamma}{(n+k)^2-\beta^2/\alpha^2}<br /> \][/itex]

and

[itex] \[<br /> p_2(n)=-\frac{1}{(n+k)^2-\beta^2/\alpha^2},<br /> \][/itex]

with
[itex] \[<br /> k=\pm\frac{\beta}{\alpha}<br /> \][/itex]

I'm interested in the asymptotic behavior of the coefficients

[itex] \[<br /> a_n^{(1)}\sim ?<br /> \][/itex]

and

[itex] \[<br /> a_n^{(2)}\sim ?<br /> \][/itex]

when

[itex] n\mapsto\infty<br /> [/itex]

Any ideas?
 
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Here's a trick that's often used in such problems. Take n large, then treat p0(n) and p1(n) as constants. You get a recurrence relation with constant coefficients, and it's possible to solve it by taking
[itex]a_n \sim \lambda^n[/itex]
and solving the resulting equation for [itex]\lambda[/itex]:

[itex]\lambda^2 = p_1 \lambda + p_0[/itex]
where
[itex]p_1 \sim \frac{\delta^2/\alpha\gamma}{n^2}[/itex]
[itex]p_2 \sim - \frac{1}{n^2}[/itex]

The solution is our old friend the quadratic formula:
[itex]\lambda = \frac{p_1 \pm \sqrt{p_1^2 + p_2}}{2} = - \frac{2p_2}{p_1 \mp \sqrt{p_1^2 + p_2}}[/itex]
which has these approximate solutions when n is small:
[itex]\lambda \sim p_1 \ll 1[/itex]
and
[itex]\lambda \sim \frac{p_2}{p_1} \sim \frac{\delta^2}{\alpha\gamma}[/itex]
So
[itex]a_n \sim \left(\frac{\delta^2}{\alpha\gamma}\right)^n[/itex]
 
Thank you for the reply.
 

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