Zeros of an affine combination of two coprime polynomials
$begingroup$
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.
abstract-algebra complex-analysis polynomials
$endgroup$
add a comment |
$begingroup$
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.
abstract-algebra complex-analysis polynomials
$endgroup$
$begingroup$
What is $K$? And have you tried yourself?
$endgroup$
– Servaes
Jan 29 at 0:01
add a comment |
$begingroup$
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.
abstract-algebra complex-analysis polynomials
$endgroup$
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
abstract-algebra complex-analysis polynomials
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
add a comment |
$begingroup$
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
add a comment |
2 Answers
2
active
oldest
votes
$begingroup$
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 $|x-r|leqepsilon$.
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
add a comment |
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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 $|x-r|leqepsilon$.
$endgroup$
add a comment |
$begingroup$
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 $|x-r|leqepsilon$.
$endgroup$
add a comment |
$begingroup$
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 $|x-r|leqepsilon$.
$endgroup$
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 $|x-r|leqepsilon$.
edited Jan 29 at 9:03
answered Jan 29 at 8:49
Eric WofseyEric Wofsey
191k14216349
191k14216349
add a comment |
add a comment |
$begingroup$
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.
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
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.
answered Jan 31 at 21:00
LutzLLutzL
60.1k42057
60.1k42057
add a comment |
add a comment |
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$begingroup$
What is $K$? And have you tried yourself?
$endgroup$
– Servaes
Jan 29 at 0:01