A function evaluated at a operator
Clash Royale CLAN TAG#URR8PPP
$begingroup$
If dim$(V)=n$ and $tau in mathcal L(V)$, prove that there is a nonzero polynomial $p(x)in F[x]$ for which $p(tau)=0$. I don't understand how come a function can be evaluated at a linear operator $tau$.
linear-algebra
$endgroup$
add a comment |
$begingroup$
If dim$(V)=n$ and $tau in mathcal L(V)$, prove that there is a nonzero polynomial $p(x)in F[x]$ for which $p(tau)=0$. I don't understand how come a function can be evaluated at a linear operator $tau$.
linear-algebra
$endgroup$
$begingroup$
A polynomial is not a function. :P
$endgroup$
– darij grinberg
Jan 24 at 3:03
add a comment |
$begingroup$
If dim$(V)=n$ and $tau in mathcal L(V)$, prove that there is a nonzero polynomial $p(x)in F[x]$ for which $p(tau)=0$. I don't understand how come a function can be evaluated at a linear operator $tau$.
linear-algebra
$endgroup$
If dim$(V)=n$ and $tau in mathcal L(V)$, prove that there is a nonzero polynomial $p(x)in F[x]$ for which $p(tau)=0$. I don't understand how come a function can be evaluated at a linear operator $tau$.
linear-algebra
linear-algebra
asked Jan 24 at 1:41
Jiexiong687691Jiexiong687691
825
825
$begingroup$
A polynomial is not a function. :P
$endgroup$
– darij grinberg
Jan 24 at 3:03
add a comment |
$begingroup$
A polynomial is not a function. :P
$endgroup$
– darij grinberg
Jan 24 at 3:03
$begingroup$
A polynomial is not a function. :P
$endgroup$
– darij grinberg
Jan 24 at 3:03
$begingroup$
A polynomial is not a function. :P
$endgroup$
– darij grinberg
Jan 24 at 3:03
add a comment |
4 Answers
4
active
oldest
votes
$begingroup$
First, how to evaluate a polynomial $p(x) in F[x]$ at a linear operator $tau in mathcal L(V)$? The first thing to realize is that powers of $tau$ make sense as elements of $mathcal L(V)$; e.g., for
$vec v in V, tag 1$ we have
$tau vec v in V, tag 2$
so it makes sense to take
$tau^2 vec v = tau(tau vec v); tag 3$
indeed, accepting (3), we may inductively define
$tau^k + 1 vec v = tau (tau^kvec v); tag 4$
thus we define $tau^m$ for any $m in Bbb N$; if $tau$ is represented by a matrix
$[tau_ij], tag 5$
then it is easy to see that $tau^m$ is represented by the matrix
$[(tau^m)_ij] = [tau_ij]^m. tag 6$
In any event, given $tau^m$, we see that
$(alpha tau^m)(vec v) = alpha (tau^m vec v); tag 7$
and we may also construct and evaluate expressions such as
$(alpha tau^l + beta tau^m)vec v = alpha tau^l vec v + beta tau^m vec v tag 8$
using the ordinary linearity properties of $mathcal L(V)$; continuing in this vein, we can for
$p(x) in F[x], ; p(x) = displaystyle sum_0^m p_i x^i, tag 9$
meaningfully define
$p(tau) = displaystyle sum_0^m p_i tau^i in mathcal L(V), tag10$
which is the general formula for $p(tau)$.
Now we recall that
$dim_F mathcal L(V) = n^2; tag11$
thus the set
$I, tau, tau^2, ldots, tau^n - 1, tau^n^2 - 1, tau^n^2 subset mathcal L(V), tag12$
having as it does $n^2 + 1$ elements, must be linearly dependent over $F$; hence we may find $n^2 +1$ members
$c_i in F, tag13$
not all $0$, such that
$displaystyle sum_0^n^2 c_i tau_i = 0; tag14$
$tau$ then satisfies the polynomial
$c(x) = displaystyle sum_0^n^2 c_i x^i in F[x]. tag14$
We have shown that every $tau in F[x]$ satisfies a polynomial of degree at most $n^2$, but this is far from optimal. For example, the well-known Cayley-Hamilton theorem shows that $tau$ obeys a degree-$n$ polynomial; but the proof of that result is somewhat more involved than what we have done here, and hence will be saved for yet another post.
$endgroup$
add a comment |
$begingroup$
Hint: $mathcalL(V)$ is also a finite dimensional vector space (over what?) Thus, you can find some integer $m$ (you can even explicitly find $m$ in terms of $n$) such that:
$$1,tau, tau^2,dots tau^m$$ are linearly dependent. I think you can continue from here.
$endgroup$
add a comment |
$begingroup$
It's not a function, it's a polynomial. For polynomials, it's easy to understand:
if the polynomial is $f(x) = a_0 + a_1 x + ldots + a_n x^n$, and the operator is $tau$,
then $f(tau) = a_0 I + a_1 tau + ldots + a_n tau^n$.
This works in any algebra over a field $F$, where the polynomial has coefficients in $F$.
$endgroup$
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
add a comment |
$begingroup$
Let $p$ be the characterstic Polynomial of $tau$. Then there exist $a_0,a_1,cdots a_n-1inmathbbC$ such that $det(tau-lambda I)=p(t)=a_0+a_1 t+cdots a_n-1t^n-1=0$. Plugging $tau$ yeilds
$p(tau)=0$
$endgroup$
add a comment |
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4 Answers
4
active
oldest
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4 Answers
4
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
First, how to evaluate a polynomial $p(x) in F[x]$ at a linear operator $tau in mathcal L(V)$? The first thing to realize is that powers of $tau$ make sense as elements of $mathcal L(V)$; e.g., for
$vec v in V, tag 1$ we have
$tau vec v in V, tag 2$
so it makes sense to take
$tau^2 vec v = tau(tau vec v); tag 3$
indeed, accepting (3), we may inductively define
$tau^k + 1 vec v = tau (tau^kvec v); tag 4$
thus we define $tau^m$ for any $m in Bbb N$; if $tau$ is represented by a matrix
$[tau_ij], tag 5$
then it is easy to see that $tau^m$ is represented by the matrix
$[(tau^m)_ij] = [tau_ij]^m. tag 6$
In any event, given $tau^m$, we see that
$(alpha tau^m)(vec v) = alpha (tau^m vec v); tag 7$
and we may also construct and evaluate expressions such as
$(alpha tau^l + beta tau^m)vec v = alpha tau^l vec v + beta tau^m vec v tag 8$
using the ordinary linearity properties of $mathcal L(V)$; continuing in this vein, we can for
$p(x) in F[x], ; p(x) = displaystyle sum_0^m p_i x^i, tag 9$
meaningfully define
$p(tau) = displaystyle sum_0^m p_i tau^i in mathcal L(V), tag10$
which is the general formula for $p(tau)$.
Now we recall that
$dim_F mathcal L(V) = n^2; tag11$
thus the set
$I, tau, tau^2, ldots, tau^n - 1, tau^n^2 - 1, tau^n^2 subset mathcal L(V), tag12$
having as it does $n^2 + 1$ elements, must be linearly dependent over $F$; hence we may find $n^2 +1$ members
$c_i in F, tag13$
not all $0$, such that
$displaystyle sum_0^n^2 c_i tau_i = 0; tag14$
$tau$ then satisfies the polynomial
$c(x) = displaystyle sum_0^n^2 c_i x^i in F[x]. tag14$
We have shown that every $tau in F[x]$ satisfies a polynomial of degree at most $n^2$, but this is far from optimal. For example, the well-known Cayley-Hamilton theorem shows that $tau$ obeys a degree-$n$ polynomial; but the proof of that result is somewhat more involved than what we have done here, and hence will be saved for yet another post.
$endgroup$
add a comment |
$begingroup$
First, how to evaluate a polynomial $p(x) in F[x]$ at a linear operator $tau in mathcal L(V)$? The first thing to realize is that powers of $tau$ make sense as elements of $mathcal L(V)$; e.g., for
$vec v in V, tag 1$ we have
$tau vec v in V, tag 2$
so it makes sense to take
$tau^2 vec v = tau(tau vec v); tag 3$
indeed, accepting (3), we may inductively define
$tau^k + 1 vec v = tau (tau^kvec v); tag 4$
thus we define $tau^m$ for any $m in Bbb N$; if $tau$ is represented by a matrix
$[tau_ij], tag 5$
then it is easy to see that $tau^m$ is represented by the matrix
$[(tau^m)_ij] = [tau_ij]^m. tag 6$
In any event, given $tau^m$, we see that
$(alpha tau^m)(vec v) = alpha (tau^m vec v); tag 7$
and we may also construct and evaluate expressions such as
$(alpha tau^l + beta tau^m)vec v = alpha tau^l vec v + beta tau^m vec v tag 8$
using the ordinary linearity properties of $mathcal L(V)$; continuing in this vein, we can for
$p(x) in F[x], ; p(x) = displaystyle sum_0^m p_i x^i, tag 9$
meaningfully define
$p(tau) = displaystyle sum_0^m p_i tau^i in mathcal L(V), tag10$
which is the general formula for $p(tau)$.
Now we recall that
$dim_F mathcal L(V) = n^2; tag11$
thus the set
$I, tau, tau^2, ldots, tau^n - 1, tau^n^2 - 1, tau^n^2 subset mathcal L(V), tag12$
having as it does $n^2 + 1$ elements, must be linearly dependent over $F$; hence we may find $n^2 +1$ members
$c_i in F, tag13$
not all $0$, such that
$displaystyle sum_0^n^2 c_i tau_i = 0; tag14$
$tau$ then satisfies the polynomial
$c(x) = displaystyle sum_0^n^2 c_i x^i in F[x]. tag14$
We have shown that every $tau in F[x]$ satisfies a polynomial of degree at most $n^2$, but this is far from optimal. For example, the well-known Cayley-Hamilton theorem shows that $tau$ obeys a degree-$n$ polynomial; but the proof of that result is somewhat more involved than what we have done here, and hence will be saved for yet another post.
$endgroup$
add a comment |
$begingroup$
First, how to evaluate a polynomial $p(x) in F[x]$ at a linear operator $tau in mathcal L(V)$? The first thing to realize is that powers of $tau$ make sense as elements of $mathcal L(V)$; e.g., for
$vec v in V, tag 1$ we have
$tau vec v in V, tag 2$
so it makes sense to take
$tau^2 vec v = tau(tau vec v); tag 3$
indeed, accepting (3), we may inductively define
$tau^k + 1 vec v = tau (tau^kvec v); tag 4$
thus we define $tau^m$ for any $m in Bbb N$; if $tau$ is represented by a matrix
$[tau_ij], tag 5$
then it is easy to see that $tau^m$ is represented by the matrix
$[(tau^m)_ij] = [tau_ij]^m. tag 6$
In any event, given $tau^m$, we see that
$(alpha tau^m)(vec v) = alpha (tau^m vec v); tag 7$
and we may also construct and evaluate expressions such as
$(alpha tau^l + beta tau^m)vec v = alpha tau^l vec v + beta tau^m vec v tag 8$
using the ordinary linearity properties of $mathcal L(V)$; continuing in this vein, we can for
$p(x) in F[x], ; p(x) = displaystyle sum_0^m p_i x^i, tag 9$
meaningfully define
$p(tau) = displaystyle sum_0^m p_i tau^i in mathcal L(V), tag10$
which is the general formula for $p(tau)$.
Now we recall that
$dim_F mathcal L(V) = n^2; tag11$
thus the set
$I, tau, tau^2, ldots, tau^n - 1, tau^n^2 - 1, tau^n^2 subset mathcal L(V), tag12$
having as it does $n^2 + 1$ elements, must be linearly dependent over $F$; hence we may find $n^2 +1$ members
$c_i in F, tag13$
not all $0$, such that
$displaystyle sum_0^n^2 c_i tau_i = 0; tag14$
$tau$ then satisfies the polynomial
$c(x) = displaystyle sum_0^n^2 c_i x^i in F[x]. tag14$
We have shown that every $tau in F[x]$ satisfies a polynomial of degree at most $n^2$, but this is far from optimal. For example, the well-known Cayley-Hamilton theorem shows that $tau$ obeys a degree-$n$ polynomial; but the proof of that result is somewhat more involved than what we have done here, and hence will be saved for yet another post.
$endgroup$
First, how to evaluate a polynomial $p(x) in F[x]$ at a linear operator $tau in mathcal L(V)$? The first thing to realize is that powers of $tau$ make sense as elements of $mathcal L(V)$; e.g., for
$vec v in V, tag 1$ we have
$tau vec v in V, tag 2$
so it makes sense to take
$tau^2 vec v = tau(tau vec v); tag 3$
indeed, accepting (3), we may inductively define
$tau^k + 1 vec v = tau (tau^kvec v); tag 4$
thus we define $tau^m$ for any $m in Bbb N$; if $tau$ is represented by a matrix
$[tau_ij], tag 5$
then it is easy to see that $tau^m$ is represented by the matrix
$[(tau^m)_ij] = [tau_ij]^m. tag 6$
In any event, given $tau^m$, we see that
$(alpha tau^m)(vec v) = alpha (tau^m vec v); tag 7$
and we may also construct and evaluate expressions such as
$(alpha tau^l + beta tau^m)vec v = alpha tau^l vec v + beta tau^m vec v tag 8$
using the ordinary linearity properties of $mathcal L(V)$; continuing in this vein, we can for
$p(x) in F[x], ; p(x) = displaystyle sum_0^m p_i x^i, tag 9$
meaningfully define
$p(tau) = displaystyle sum_0^m p_i tau^i in mathcal L(V), tag10$
which is the general formula for $p(tau)$.
Now we recall that
$dim_F mathcal L(V) = n^2; tag11$
thus the set
$I, tau, tau^2, ldots, tau^n - 1, tau^n^2 - 1, tau^n^2 subset mathcal L(V), tag12$
having as it does $n^2 + 1$ elements, must be linearly dependent over $F$; hence we may find $n^2 +1$ members
$c_i in F, tag13$
not all $0$, such that
$displaystyle sum_0^n^2 c_i tau_i = 0; tag14$
$tau$ then satisfies the polynomial
$c(x) = displaystyle sum_0^n^2 c_i x^i in F[x]. tag14$
We have shown that every $tau in F[x]$ satisfies a polynomial of degree at most $n^2$, but this is far from optimal. For example, the well-known Cayley-Hamilton theorem shows that $tau$ obeys a degree-$n$ polynomial; but the proof of that result is somewhat more involved than what we have done here, and hence will be saved for yet another post.
answered Jan 24 at 2:54
Robert LewisRobert Lewis
46.2k23066
46.2k23066
add a comment |
add a comment |
$begingroup$
Hint: $mathcalL(V)$ is also a finite dimensional vector space (over what?) Thus, you can find some integer $m$ (you can even explicitly find $m$ in terms of $n$) such that:
$$1,tau, tau^2,dots tau^m$$ are linearly dependent. I think you can continue from here.
$endgroup$
add a comment |
$begingroup$
Hint: $mathcalL(V)$ is also a finite dimensional vector space (over what?) Thus, you can find some integer $m$ (you can even explicitly find $m$ in terms of $n$) such that:
$$1,tau, tau^2,dots tau^m$$ are linearly dependent. I think you can continue from here.
$endgroup$
add a comment |
$begingroup$
Hint: $mathcalL(V)$ is also a finite dimensional vector space (over what?) Thus, you can find some integer $m$ (you can even explicitly find $m$ in terms of $n$) such that:
$$1,tau, tau^2,dots tau^m$$ are linearly dependent. I think you can continue from here.
$endgroup$
Hint: $mathcalL(V)$ is also a finite dimensional vector space (over what?) Thus, you can find some integer $m$ (you can even explicitly find $m$ in terms of $n$) such that:
$$1,tau, tau^2,dots tau^m$$ are linearly dependent. I think you can continue from here.
answered Jan 24 at 2:00
dezdichadodezdichado
6,3711929
6,3711929
add a comment |
add a comment |
$begingroup$
It's not a function, it's a polynomial. For polynomials, it's easy to understand:
if the polynomial is $f(x) = a_0 + a_1 x + ldots + a_n x^n$, and the operator is $tau$,
then $f(tau) = a_0 I + a_1 tau + ldots + a_n tau^n$.
This works in any algebra over a field $F$, where the polynomial has coefficients in $F$.
$endgroup$
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
add a comment |
$begingroup$
It's not a function, it's a polynomial. For polynomials, it's easy to understand:
if the polynomial is $f(x) = a_0 + a_1 x + ldots + a_n x^n$, and the operator is $tau$,
then $f(tau) = a_0 I + a_1 tau + ldots + a_n tau^n$.
This works in any algebra over a field $F$, where the polynomial has coefficients in $F$.
$endgroup$
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
add a comment |
$begingroup$
It's not a function, it's a polynomial. For polynomials, it's easy to understand:
if the polynomial is $f(x) = a_0 + a_1 x + ldots + a_n x^n$, and the operator is $tau$,
then $f(tau) = a_0 I + a_1 tau + ldots + a_n tau^n$.
This works in any algebra over a field $F$, where the polynomial has coefficients in $F$.
$endgroup$
It's not a function, it's a polynomial. For polynomials, it's easy to understand:
if the polynomial is $f(x) = a_0 + a_1 x + ldots + a_n x^n$, and the operator is $tau$,
then $f(tau) = a_0 I + a_1 tau + ldots + a_n tau^n$.
This works in any algebra over a field $F$, where the polynomial has coefficients in $F$.
answered Jan 24 at 2:25
Robert IsraelRobert Israel
323k23212466
323k23212466
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
add a comment |
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
$begingroup$
Note that in this context, the powers of $x$ are evaluated by repeated composition of $tau$ with itself, while the coefficients of the polynomial are treated as scalar multiples of those powers. Finally the terms of the polynomial are added together as one adds linear mappings to get a linear mapping as a result.
$endgroup$
– hardmath
Jan 24 at 2:37
add a comment |
$begingroup$
Let $p$ be the characterstic Polynomial of $tau$. Then there exist $a_0,a_1,cdots a_n-1inmathbbC$ such that $det(tau-lambda I)=p(t)=a_0+a_1 t+cdots a_n-1t^n-1=0$. Plugging $tau$ yeilds
$p(tau)=0$
$endgroup$
add a comment |
$begingroup$
Let $p$ be the characterstic Polynomial of $tau$. Then there exist $a_0,a_1,cdots a_n-1inmathbbC$ such that $det(tau-lambda I)=p(t)=a_0+a_1 t+cdots a_n-1t^n-1=0$. Plugging $tau$ yeilds
$p(tau)=0$
$endgroup$
add a comment |
$begingroup$
Let $p$ be the characterstic Polynomial of $tau$. Then there exist $a_0,a_1,cdots a_n-1inmathbbC$ such that $det(tau-lambda I)=p(t)=a_0+a_1 t+cdots a_n-1t^n-1=0$. Plugging $tau$ yeilds
$p(tau)=0$
$endgroup$
Let $p$ be the characterstic Polynomial of $tau$. Then there exist $a_0,a_1,cdots a_n-1inmathbbC$ such that $det(tau-lambda I)=p(t)=a_0+a_1 t+cdots a_n-1t^n-1=0$. Plugging $tau$ yeilds
$p(tau)=0$
answered Jan 24 at 2:16
John TalosJohn Talos
14
14
add a comment |
add a comment |
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$begingroup$
A polynomial is not a function. :P
$endgroup$
– darij grinberg
Jan 24 at 3:03