Zeros of an affine combination of two coprime polynomials












2












$begingroup$


Suppose $f, g in mathbb R[x]$ are two coprime monic polynomials with
begin{align*}
f(x) = x^n + a_{n-1} x^{n-1} + dots + a_0 \
g(x) = x^m + b_{m-1} x^{m-1} + dots + b_0,
end{align*}

and $n > m$.
Let $h(x,t) = f(x) - t g(x)$ where $t in mathbb R$. I read in a book without explanation that: If $t in [0, infty)$ and as $t to infty$, there are $n-m$ zeros of $h$ that would be asymptotically close to $n-m$ rays passing through $z = -frac{a_{n-1}-b_{m-1}}{n-m}$. As $t to infty$, the $n-m$ zeros are arbitrarily close to
begin{align*}
z = -frac{a_{n-1} - b_{m-1} }{n-m} + t^{1/(n-m)}omega_j,
end{align*}

where $omega_j$'s are the $(n-m)^{text{th}}$ roots of unity. How do we formally prove this argument?



I can only $n-m$ zeros going to infinity by Rouche's Theorem. We can compare $tg$ and $f-tg$ on a sphere that encloses all the zeros of $g$. But have not idea on where the asymptotes come from.










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$endgroup$












  • $begingroup$
    What is $K$? And have you tried yourself?
    $endgroup$
    – Servaes
    Jan 29 at 0:01
















2












$begingroup$


Suppose $f, g in mathbb R[x]$ are two coprime monic polynomials with
begin{align*}
f(x) = x^n + a_{n-1} x^{n-1} + dots + a_0 \
g(x) = x^m + b_{m-1} x^{m-1} + dots + b_0,
end{align*}

and $n > m$.
Let $h(x,t) = f(x) - t g(x)$ where $t in mathbb R$. I read in a book without explanation that: If $t in [0, infty)$ and as $t to infty$, there are $n-m$ zeros of $h$ that would be asymptotically close to $n-m$ rays passing through $z = -frac{a_{n-1}-b_{m-1}}{n-m}$. As $t to infty$, the $n-m$ zeros are arbitrarily close to
begin{align*}
z = -frac{a_{n-1} - b_{m-1} }{n-m} + t^{1/(n-m)}omega_j,
end{align*}

where $omega_j$'s are the $(n-m)^{text{th}}$ roots of unity. How do we formally prove this argument?



I can only $n-m$ zeros going to infinity by Rouche's Theorem. We can compare $tg$ and $f-tg$ on a sphere that encloses all the zeros of $g$. But have not idea on where the asymptotes come from.










share|cite|improve this question











$endgroup$












  • $begingroup$
    What is $K$? And have you tried yourself?
    $endgroup$
    – Servaes
    Jan 29 at 0:01














2












2








2





$begingroup$


Suppose $f, g in mathbb R[x]$ are two coprime monic polynomials with
begin{align*}
f(x) = x^n + a_{n-1} x^{n-1} + dots + a_0 \
g(x) = x^m + b_{m-1} x^{m-1} + dots + b_0,
end{align*}

and $n > m$.
Let $h(x,t) = f(x) - t g(x)$ where $t in mathbb R$. I read in a book without explanation that: If $t in [0, infty)$ and as $t to infty$, there are $n-m$ zeros of $h$ that would be asymptotically close to $n-m$ rays passing through $z = -frac{a_{n-1}-b_{m-1}}{n-m}$. As $t to infty$, the $n-m$ zeros are arbitrarily close to
begin{align*}
z = -frac{a_{n-1} - b_{m-1} }{n-m} + t^{1/(n-m)}omega_j,
end{align*}

where $omega_j$'s are the $(n-m)^{text{th}}$ roots of unity. How do we formally prove this argument?



I can only $n-m$ zeros going to infinity by Rouche's Theorem. We can compare $tg$ and $f-tg$ on a sphere that encloses all the zeros of $g$. But have not idea on where the asymptotes come from.










share|cite|improve this question











$endgroup$




Suppose $f, g in mathbb R[x]$ are two coprime monic polynomials with
begin{align*}
f(x) = x^n + a_{n-1} x^{n-1} + dots + a_0 \
g(x) = x^m + b_{m-1} x^{m-1} + dots + b_0,
end{align*}

and $n > m$.
Let $h(x,t) = f(x) - t g(x)$ where $t in mathbb R$. I read in a book without explanation that: If $t in [0, infty)$ and as $t to infty$, there are $n-m$ zeros of $h$ that would be asymptotically close to $n-m$ rays passing through $z = -frac{a_{n-1}-b_{m-1}}{n-m}$. As $t to infty$, the $n-m$ zeros are arbitrarily close to
begin{align*}
z = -frac{a_{n-1} - b_{m-1} }{n-m} + t^{1/(n-m)}omega_j,
end{align*}

where $omega_j$'s are the $(n-m)^{text{th}}$ roots of unity. How do we formally prove this argument?



I can only $n-m$ zeros going to infinity by Rouche's Theorem. We can compare $tg$ and $f-tg$ on a sphere that encloses all the zeros of $g$. But have not idea on where the asymptotes come from.







abstract-algebra complex-analysis polynomials






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edited Jan 29 at 9:05









Eric Wofsey

191k14216349




191k14216349










asked Jan 28 at 23:58









user1101010user1101010

9011830




9011830












  • $begingroup$
    What is $K$? And have you tried yourself?
    $endgroup$
    – Servaes
    Jan 29 at 0:01


















  • $begingroup$
    What is $K$? And have you tried yourself?
    $endgroup$
    – Servaes
    Jan 29 at 0:01
















$begingroup$
What is $K$? And have you tried yourself?
$endgroup$
– Servaes
Jan 29 at 0:01




$begingroup$
What is $K$? And have you tried yourself?
$endgroup$
– Servaes
Jan 29 at 0:01










2 Answers
2






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oldest

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Note first that if we substitute $x+c$ for $x$ in our polynomials, $a_{n-1}$ increases by $nc$ and $b_{m-1}$ increases by $mc$ and so $-frac{a_{n-1}-b_{m-1}}{n-m}$ decreases by $c$ and the truth of the statement does not change. In particular, taking $c=-b_{m-1}/m$, we may assume $b_{m-1}=0$.



Now let $d=-frac{a_{n-1}}{n-m}$, and let $f_0(x)=f(x)-x^m(x-d)^{n-m}$ and let $g_0(x)=g(x)-x^m$. Note that $deg f_0leq n-2$ and $deg g_0leq m-2$. We have $$h(x,t)=x^m((x-d)^{n-m}-t)+f_0(x)-tg_0(x).$$ Let $r=d+t^{1/(n-m)}omega$ where $omega$ is an $(n-m)$th root of unity and observe that $r$ is a root of $H(x,t)=x^m((x-d)^{n-m}-t)$. The idea is now to show that $H(x,t)$ dominates $f_0(x)-tg_0(x)$ as $x$ goes around a loop near $r$, so that by Rouche's theorem $h(x,t)$ will have to also have a root near $r$.



Fix $epsilon>0$. We see that if $|x-r|=epsilon$ then $|x^m|$ is within a constant factor of $t^{m/(n-m)}$ for $t$ sufficiently large. Also, $$frac{(x-d)^{n-m}-t}{x-r}=frac{(t^{1/(n-m)}omega+(x-r))^{n-m}-(t^{1/(n-m)}omega)^{n-m}}{x-r}$$ is equal to the derivative of $zmapsto z^{n-m}$ at some point within $epsilon$ of $t^{1/(n-m)}omega$ by the mean value theorem. It follows that $|(x-d)^{n-m}-t|$ is within a constant factor of $t^{(n-m-1)/(n-m)}$ for $t$ sufficiently large. We thus see that for $|x-r|<epsilon$, $|H(x,t)|$ is bounded below by a constant multiple of $t^{(n-1)/(n-m)}$ for $t$ sufficiently large.



On the other hand, for $|x-r|=epsilon$, $|f_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$ and $|g_0(x)|$ is bounded above by a constant multiple of $t^{(m-2)/(n-m)}$. It follows that $|f_0(x)-tg_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$.



Thus, we see that if $t$ is sufficiently large, then $|H(x,t)|>|f_0(x)-tg_0(x)|$ for all $x$ such that $|x-r|=epsilon$. So, by Rouche's theorem, since $H(x,t)$ has a root at $x=r$, we conclude that $h(x,t)=H(x,t)+f_0(x)-tg_0(x)$ must also have a root in the disk $|x-r|leqepsilon$.






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    1












    $begingroup$

    To avoid the roots set $t=s^{n-m}$. Now scale the problem by setting $x=su$. Then
    $$
    s^{-n}h(su, s^{n-m})=(u^n+s^{-1}a_{n-1}u^{n-1}+...+s^{-n}a_0)-(u^m+s^{-1}b_{m-1}u^{m-1}+...+s^{-m}b_0).$$

    For $stoinftyiff ttoinfty$ the remaining polynomial $u^n-u^m$ has an $m$- fold root at $u=0$ and the other roots at the $(m-n)$th unit roots. For $sapproxinfty$ very large or $s^{-1}$ very small, the perturbation due to the next terms in
    $$
    0=u^m(u^{n-m}-1)+s^{-1}u^{m-1}(a_{n-1}u^{n-m}-b_{m-1})+O(s^{-2}u^{m-2})
    $$

    gives $m$ very small roots of size $O(s^{-1})$ close to the roots of $0=g(su)$. From each of the unperturbed unit roots $u=ω^k$, $ω^{n-m}=1$, the perturbation will result in a root $u=ω^k(1+s^{-1}v)+O(s^{-2})$, where $v$ solves
    $$
    0=ω^{mk}(n-m)v+ω^{(m-1)k}(a_{n-1}-b_{m-1})implies v=-ω^{-k}frac{a_{n-1}-b_{m-1}}{n-m}
    $$

    so that in total
    $$
    u=ω^k-s^{-1}frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-2})~~text{ or }~~ x=sω^k-frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-1})
    $$





    As an example I plotted the root locations for polynomials with $n=9,m=4$, $a_8=2$, $b_3=-3$, left for the $u$ parametrization, right for the $x$ parametrization. $s$ varies from $1$ to $50$ ($s^{-1}$ in equidistant steps). In light gray are the unit root locations resp. the asymptotic rays.



    enter image description here






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      2 Answers
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      2 Answers
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      $begingroup$

      Note first that if we substitute $x+c$ for $x$ in our polynomials, $a_{n-1}$ increases by $nc$ and $b_{m-1}$ increases by $mc$ and so $-frac{a_{n-1}-b_{m-1}}{n-m}$ decreases by $c$ and the truth of the statement does not change. In particular, taking $c=-b_{m-1}/m$, we may assume $b_{m-1}=0$.



      Now let $d=-frac{a_{n-1}}{n-m}$, and let $f_0(x)=f(x)-x^m(x-d)^{n-m}$ and let $g_0(x)=g(x)-x^m$. Note that $deg f_0leq n-2$ and $deg g_0leq m-2$. We have $$h(x,t)=x^m((x-d)^{n-m}-t)+f_0(x)-tg_0(x).$$ Let $r=d+t^{1/(n-m)}omega$ where $omega$ is an $(n-m)$th root of unity and observe that $r$ is a root of $H(x,t)=x^m((x-d)^{n-m}-t)$. The idea is now to show that $H(x,t)$ dominates $f_0(x)-tg_0(x)$ as $x$ goes around a loop near $r$, so that by Rouche's theorem $h(x,t)$ will have to also have a root near $r$.



      Fix $epsilon>0$. We see that if $|x-r|=epsilon$ then $|x^m|$ is within a constant factor of $t^{m/(n-m)}$ for $t$ sufficiently large. Also, $$frac{(x-d)^{n-m}-t}{x-r}=frac{(t^{1/(n-m)}omega+(x-r))^{n-m}-(t^{1/(n-m)}omega)^{n-m}}{x-r}$$ is equal to the derivative of $zmapsto z^{n-m}$ at some point within $epsilon$ of $t^{1/(n-m)}omega$ by the mean value theorem. It follows that $|(x-d)^{n-m}-t|$ is within a constant factor of $t^{(n-m-1)/(n-m)}$ for $t$ sufficiently large. We thus see that for $|x-r|<epsilon$, $|H(x,t)|$ is bounded below by a constant multiple of $t^{(n-1)/(n-m)}$ for $t$ sufficiently large.



      On the other hand, for $|x-r|=epsilon$, $|f_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$ and $|g_0(x)|$ is bounded above by a constant multiple of $t^{(m-2)/(n-m)}$. It follows that $|f_0(x)-tg_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$.



      Thus, we see that if $t$ is sufficiently large, then $|H(x,t)|>|f_0(x)-tg_0(x)|$ for all $x$ such that $|x-r|=epsilon$. So, by Rouche's theorem, since $H(x,t)$ has a root at $x=r$, we conclude that $h(x,t)=H(x,t)+f_0(x)-tg_0(x)$ must also have a root in the disk $|x-r|leqepsilon$.






      share|cite|improve this answer











      $endgroup$


















        1












        $begingroup$

        Note first that if we substitute $x+c$ for $x$ in our polynomials, $a_{n-1}$ increases by $nc$ and $b_{m-1}$ increases by $mc$ and so $-frac{a_{n-1}-b_{m-1}}{n-m}$ decreases by $c$ and the truth of the statement does not change. In particular, taking $c=-b_{m-1}/m$, we may assume $b_{m-1}=0$.



        Now let $d=-frac{a_{n-1}}{n-m}$, and let $f_0(x)=f(x)-x^m(x-d)^{n-m}$ and let $g_0(x)=g(x)-x^m$. Note that $deg f_0leq n-2$ and $deg g_0leq m-2$. We have $$h(x,t)=x^m((x-d)^{n-m}-t)+f_0(x)-tg_0(x).$$ Let $r=d+t^{1/(n-m)}omega$ where $omega$ is an $(n-m)$th root of unity and observe that $r$ is a root of $H(x,t)=x^m((x-d)^{n-m}-t)$. The idea is now to show that $H(x,t)$ dominates $f_0(x)-tg_0(x)$ as $x$ goes around a loop near $r$, so that by Rouche's theorem $h(x,t)$ will have to also have a root near $r$.



        Fix $epsilon>0$. We see that if $|x-r|=epsilon$ then $|x^m|$ is within a constant factor of $t^{m/(n-m)}$ for $t$ sufficiently large. Also, $$frac{(x-d)^{n-m}-t}{x-r}=frac{(t^{1/(n-m)}omega+(x-r))^{n-m}-(t^{1/(n-m)}omega)^{n-m}}{x-r}$$ is equal to the derivative of $zmapsto z^{n-m}$ at some point within $epsilon$ of $t^{1/(n-m)}omega$ by the mean value theorem. It follows that $|(x-d)^{n-m}-t|$ is within a constant factor of $t^{(n-m-1)/(n-m)}$ for $t$ sufficiently large. We thus see that for $|x-r|<epsilon$, $|H(x,t)|$ is bounded below by a constant multiple of $t^{(n-1)/(n-m)}$ for $t$ sufficiently large.



        On the other hand, for $|x-r|=epsilon$, $|f_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$ and $|g_0(x)|$ is bounded above by a constant multiple of $t^{(m-2)/(n-m)}$. It follows that $|f_0(x)-tg_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$.



        Thus, we see that if $t$ is sufficiently large, then $|H(x,t)|>|f_0(x)-tg_0(x)|$ for all $x$ such that $|x-r|=epsilon$. So, by Rouche's theorem, since $H(x,t)$ has a root at $x=r$, we conclude that $h(x,t)=H(x,t)+f_0(x)-tg_0(x)$ must also have a root in the disk $|x-r|leqepsilon$.






        share|cite|improve this answer











        $endgroup$
















          1












          1








          1





          $begingroup$

          Note first that if we substitute $x+c$ for $x$ in our polynomials, $a_{n-1}$ increases by $nc$ and $b_{m-1}$ increases by $mc$ and so $-frac{a_{n-1}-b_{m-1}}{n-m}$ decreases by $c$ and the truth of the statement does not change. In particular, taking $c=-b_{m-1}/m$, we may assume $b_{m-1}=0$.



          Now let $d=-frac{a_{n-1}}{n-m}$, and let $f_0(x)=f(x)-x^m(x-d)^{n-m}$ and let $g_0(x)=g(x)-x^m$. Note that $deg f_0leq n-2$ and $deg g_0leq m-2$. We have $$h(x,t)=x^m((x-d)^{n-m}-t)+f_0(x)-tg_0(x).$$ Let $r=d+t^{1/(n-m)}omega$ where $omega$ is an $(n-m)$th root of unity and observe that $r$ is a root of $H(x,t)=x^m((x-d)^{n-m}-t)$. The idea is now to show that $H(x,t)$ dominates $f_0(x)-tg_0(x)$ as $x$ goes around a loop near $r$, so that by Rouche's theorem $h(x,t)$ will have to also have a root near $r$.



          Fix $epsilon>0$. We see that if $|x-r|=epsilon$ then $|x^m|$ is within a constant factor of $t^{m/(n-m)}$ for $t$ sufficiently large. Also, $$frac{(x-d)^{n-m}-t}{x-r}=frac{(t^{1/(n-m)}omega+(x-r))^{n-m}-(t^{1/(n-m)}omega)^{n-m}}{x-r}$$ is equal to the derivative of $zmapsto z^{n-m}$ at some point within $epsilon$ of $t^{1/(n-m)}omega$ by the mean value theorem. It follows that $|(x-d)^{n-m}-t|$ is within a constant factor of $t^{(n-m-1)/(n-m)}$ for $t$ sufficiently large. We thus see that for $|x-r|<epsilon$, $|H(x,t)|$ is bounded below by a constant multiple of $t^{(n-1)/(n-m)}$ for $t$ sufficiently large.



          On the other hand, for $|x-r|=epsilon$, $|f_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$ and $|g_0(x)|$ is bounded above by a constant multiple of $t^{(m-2)/(n-m)}$. It follows that $|f_0(x)-tg_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$.



          Thus, we see that if $t$ is sufficiently large, then $|H(x,t)|>|f_0(x)-tg_0(x)|$ for all $x$ such that $|x-r|=epsilon$. So, by Rouche's theorem, since $H(x,t)$ has a root at $x=r$, we conclude that $h(x,t)=H(x,t)+f_0(x)-tg_0(x)$ must also have a root in the disk $|x-r|leqepsilon$.






          share|cite|improve this answer











          $endgroup$



          Note first that if we substitute $x+c$ for $x$ in our polynomials, $a_{n-1}$ increases by $nc$ and $b_{m-1}$ increases by $mc$ and so $-frac{a_{n-1}-b_{m-1}}{n-m}$ decreases by $c$ and the truth of the statement does not change. In particular, taking $c=-b_{m-1}/m$, we may assume $b_{m-1}=0$.



          Now let $d=-frac{a_{n-1}}{n-m}$, and let $f_0(x)=f(x)-x^m(x-d)^{n-m}$ and let $g_0(x)=g(x)-x^m$. Note that $deg f_0leq n-2$ and $deg g_0leq m-2$. We have $$h(x,t)=x^m((x-d)^{n-m}-t)+f_0(x)-tg_0(x).$$ Let $r=d+t^{1/(n-m)}omega$ where $omega$ is an $(n-m)$th root of unity and observe that $r$ is a root of $H(x,t)=x^m((x-d)^{n-m}-t)$. The idea is now to show that $H(x,t)$ dominates $f_0(x)-tg_0(x)$ as $x$ goes around a loop near $r$, so that by Rouche's theorem $h(x,t)$ will have to also have a root near $r$.



          Fix $epsilon>0$. We see that if $|x-r|=epsilon$ then $|x^m|$ is within a constant factor of $t^{m/(n-m)}$ for $t$ sufficiently large. Also, $$frac{(x-d)^{n-m}-t}{x-r}=frac{(t^{1/(n-m)}omega+(x-r))^{n-m}-(t^{1/(n-m)}omega)^{n-m}}{x-r}$$ is equal to the derivative of $zmapsto z^{n-m}$ at some point within $epsilon$ of $t^{1/(n-m)}omega$ by the mean value theorem. It follows that $|(x-d)^{n-m}-t|$ is within a constant factor of $t^{(n-m-1)/(n-m)}$ for $t$ sufficiently large. We thus see that for $|x-r|<epsilon$, $|H(x,t)|$ is bounded below by a constant multiple of $t^{(n-1)/(n-m)}$ for $t$ sufficiently large.



          On the other hand, for $|x-r|=epsilon$, $|f_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$ and $|g_0(x)|$ is bounded above by a constant multiple of $t^{(m-2)/(n-m)}$. It follows that $|f_0(x)-tg_0(x)|$ is bounded above by a constant multiple of $t^{(n-2)/(n-m)}$.



          Thus, we see that if $t$ is sufficiently large, then $|H(x,t)|>|f_0(x)-tg_0(x)|$ for all $x$ such that $|x-r|=epsilon$. So, by Rouche's theorem, since $H(x,t)$ has a root at $x=r$, we conclude that $h(x,t)=H(x,t)+f_0(x)-tg_0(x)$ must also have a root in the disk $|x-r|leqepsilon$.







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          share|cite|improve this answer



          share|cite|improve this answer








          edited Jan 29 at 9:03

























          answered Jan 29 at 8:49









          Eric WofseyEric Wofsey

          191k14216349




          191k14216349























              1












              $begingroup$

              To avoid the roots set $t=s^{n-m}$. Now scale the problem by setting $x=su$. Then
              $$
              s^{-n}h(su, s^{n-m})=(u^n+s^{-1}a_{n-1}u^{n-1}+...+s^{-n}a_0)-(u^m+s^{-1}b_{m-1}u^{m-1}+...+s^{-m}b_0).$$

              For $stoinftyiff ttoinfty$ the remaining polynomial $u^n-u^m$ has an $m$- fold root at $u=0$ and the other roots at the $(m-n)$th unit roots. For $sapproxinfty$ very large or $s^{-1}$ very small, the perturbation due to the next terms in
              $$
              0=u^m(u^{n-m}-1)+s^{-1}u^{m-1}(a_{n-1}u^{n-m}-b_{m-1})+O(s^{-2}u^{m-2})
              $$

              gives $m$ very small roots of size $O(s^{-1})$ close to the roots of $0=g(su)$. From each of the unperturbed unit roots $u=ω^k$, $ω^{n-m}=1$, the perturbation will result in a root $u=ω^k(1+s^{-1}v)+O(s^{-2})$, where $v$ solves
              $$
              0=ω^{mk}(n-m)v+ω^{(m-1)k}(a_{n-1}-b_{m-1})implies v=-ω^{-k}frac{a_{n-1}-b_{m-1}}{n-m}
              $$

              so that in total
              $$
              u=ω^k-s^{-1}frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-2})~~text{ or }~~ x=sω^k-frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-1})
              $$





              As an example I plotted the root locations for polynomials with $n=9,m=4$, $a_8=2$, $b_3=-3$, left for the $u$ parametrization, right for the $x$ parametrization. $s$ varies from $1$ to $50$ ($s^{-1}$ in equidistant steps). In light gray are the unit root locations resp. the asymptotic rays.



              enter image description here






              share|cite|improve this answer









              $endgroup$


















                1












                $begingroup$

                To avoid the roots set $t=s^{n-m}$. Now scale the problem by setting $x=su$. Then
                $$
                s^{-n}h(su, s^{n-m})=(u^n+s^{-1}a_{n-1}u^{n-1}+...+s^{-n}a_0)-(u^m+s^{-1}b_{m-1}u^{m-1}+...+s^{-m}b_0).$$

                For $stoinftyiff ttoinfty$ the remaining polynomial $u^n-u^m$ has an $m$- fold root at $u=0$ and the other roots at the $(m-n)$th unit roots. For $sapproxinfty$ very large or $s^{-1}$ very small, the perturbation due to the next terms in
                $$
                0=u^m(u^{n-m}-1)+s^{-1}u^{m-1}(a_{n-1}u^{n-m}-b_{m-1})+O(s^{-2}u^{m-2})
                $$

                gives $m$ very small roots of size $O(s^{-1})$ close to the roots of $0=g(su)$. From each of the unperturbed unit roots $u=ω^k$, $ω^{n-m}=1$, the perturbation will result in a root $u=ω^k(1+s^{-1}v)+O(s^{-2})$, where $v$ solves
                $$
                0=ω^{mk}(n-m)v+ω^{(m-1)k}(a_{n-1}-b_{m-1})implies v=-ω^{-k}frac{a_{n-1}-b_{m-1}}{n-m}
                $$

                so that in total
                $$
                u=ω^k-s^{-1}frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-2})~~text{ or }~~ x=sω^k-frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-1})
                $$





                As an example I plotted the root locations for polynomials with $n=9,m=4$, $a_8=2$, $b_3=-3$, left for the $u$ parametrization, right for the $x$ parametrization. $s$ varies from $1$ to $50$ ($s^{-1}$ in equidistant steps). In light gray are the unit root locations resp. the asymptotic rays.



                enter image description here






                share|cite|improve this answer









                $endgroup$
















                  1












                  1








                  1





                  $begingroup$

                  To avoid the roots set $t=s^{n-m}$. Now scale the problem by setting $x=su$. Then
                  $$
                  s^{-n}h(su, s^{n-m})=(u^n+s^{-1}a_{n-1}u^{n-1}+...+s^{-n}a_0)-(u^m+s^{-1}b_{m-1}u^{m-1}+...+s^{-m}b_0).$$

                  For $stoinftyiff ttoinfty$ the remaining polynomial $u^n-u^m$ has an $m$- fold root at $u=0$ and the other roots at the $(m-n)$th unit roots. For $sapproxinfty$ very large or $s^{-1}$ very small, the perturbation due to the next terms in
                  $$
                  0=u^m(u^{n-m}-1)+s^{-1}u^{m-1}(a_{n-1}u^{n-m}-b_{m-1})+O(s^{-2}u^{m-2})
                  $$

                  gives $m$ very small roots of size $O(s^{-1})$ close to the roots of $0=g(su)$. From each of the unperturbed unit roots $u=ω^k$, $ω^{n-m}=1$, the perturbation will result in a root $u=ω^k(1+s^{-1}v)+O(s^{-2})$, where $v$ solves
                  $$
                  0=ω^{mk}(n-m)v+ω^{(m-1)k}(a_{n-1}-b_{m-1})implies v=-ω^{-k}frac{a_{n-1}-b_{m-1}}{n-m}
                  $$

                  so that in total
                  $$
                  u=ω^k-s^{-1}frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-2})~~text{ or }~~ x=sω^k-frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-1})
                  $$





                  As an example I plotted the root locations for polynomials with $n=9,m=4$, $a_8=2$, $b_3=-3$, left for the $u$ parametrization, right for the $x$ parametrization. $s$ varies from $1$ to $50$ ($s^{-1}$ in equidistant steps). In light gray are the unit root locations resp. the asymptotic rays.



                  enter image description here






                  share|cite|improve this answer









                  $endgroup$



                  To avoid the roots set $t=s^{n-m}$. Now scale the problem by setting $x=su$. Then
                  $$
                  s^{-n}h(su, s^{n-m})=(u^n+s^{-1}a_{n-1}u^{n-1}+...+s^{-n}a_0)-(u^m+s^{-1}b_{m-1}u^{m-1}+...+s^{-m}b_0).$$

                  For $stoinftyiff ttoinfty$ the remaining polynomial $u^n-u^m$ has an $m$- fold root at $u=0$ and the other roots at the $(m-n)$th unit roots. For $sapproxinfty$ very large or $s^{-1}$ very small, the perturbation due to the next terms in
                  $$
                  0=u^m(u^{n-m}-1)+s^{-1}u^{m-1}(a_{n-1}u^{n-m}-b_{m-1})+O(s^{-2}u^{m-2})
                  $$

                  gives $m$ very small roots of size $O(s^{-1})$ close to the roots of $0=g(su)$. From each of the unperturbed unit roots $u=ω^k$, $ω^{n-m}=1$, the perturbation will result in a root $u=ω^k(1+s^{-1}v)+O(s^{-2})$, where $v$ solves
                  $$
                  0=ω^{mk}(n-m)v+ω^{(m-1)k}(a_{n-1}-b_{m-1})implies v=-ω^{-k}frac{a_{n-1}-b_{m-1}}{n-m}
                  $$

                  so that in total
                  $$
                  u=ω^k-s^{-1}frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-2})~~text{ or }~~ x=sω^k-frac{a_{n-1}-b_{m-1}}{n-m}+O(s^{-1})
                  $$





                  As an example I plotted the root locations for polynomials with $n=9,m=4$, $a_8=2$, $b_3=-3$, left for the $u$ parametrization, right for the $x$ parametrization. $s$ varies from $1$ to $50$ ($s^{-1}$ in equidistant steps). In light gray are the unit root locations resp. the asymptotic rays.



                  enter image description here







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Jan 31 at 21:00









                  LutzLLutzL

                  60.1k42057




                  60.1k42057






























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