Power of a Jordan Normal Form












0












$begingroup$


In my notes I have that the Jordan normal form of $B^2$ is $$begin{bmatrix}
0 & 1 & 0 & 0 \
0 & 0 & 0 & 0 \
0 & 0 & 0 &1 \
0 & 0 & 0 & 0
end{bmatrix}$$
and the notes say that because of this, the only possibility for $B$ is
$$begin{bmatrix}
0 & 1 & 0 & 0\
0 & 0 & 1 & 0 \
0 & 0 & 0 & 1 \
0 & 0 & 0 & 0
end{bmatrix}$$



Can anybody explain why this is the case? How can we conclude the jordan form of B from the jordan form of B^2? Thanks for your help!










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$endgroup$

















    0












    $begingroup$


    In my notes I have that the Jordan normal form of $B^2$ is $$begin{bmatrix}
    0 & 1 & 0 & 0 \
    0 & 0 & 0 & 0 \
    0 & 0 & 0 &1 \
    0 & 0 & 0 & 0
    end{bmatrix}$$
    and the notes say that because of this, the only possibility for $B$ is
    $$begin{bmatrix}
    0 & 1 & 0 & 0\
    0 & 0 & 1 & 0 \
    0 & 0 & 0 & 1 \
    0 & 0 & 0 & 0
    end{bmatrix}$$



    Can anybody explain why this is the case? How can we conclude the jordan form of B from the jordan form of B^2? Thanks for your help!










    share|cite|improve this question









    $endgroup$















      0












      0








      0





      $begingroup$


      In my notes I have that the Jordan normal form of $B^2$ is $$begin{bmatrix}
      0 & 1 & 0 & 0 \
      0 & 0 & 0 & 0 \
      0 & 0 & 0 &1 \
      0 & 0 & 0 & 0
      end{bmatrix}$$
      and the notes say that because of this, the only possibility for $B$ is
      $$begin{bmatrix}
      0 & 1 & 0 & 0\
      0 & 0 & 1 & 0 \
      0 & 0 & 0 & 1 \
      0 & 0 & 0 & 0
      end{bmatrix}$$



      Can anybody explain why this is the case? How can we conclude the jordan form of B from the jordan form of B^2? Thanks for your help!










      share|cite|improve this question









      $endgroup$




      In my notes I have that the Jordan normal form of $B^2$ is $$begin{bmatrix}
      0 & 1 & 0 & 0 \
      0 & 0 & 0 & 0 \
      0 & 0 & 0 &1 \
      0 & 0 & 0 & 0
      end{bmatrix}$$
      and the notes say that because of this, the only possibility for $B$ is
      $$begin{bmatrix}
      0 & 1 & 0 & 0\
      0 & 0 & 1 & 0 \
      0 & 0 & 0 & 1 \
      0 & 0 & 0 & 0
      end{bmatrix}$$



      Can anybody explain why this is the case? How can we conclude the jordan form of B from the jordan form of B^2? Thanks for your help!







      jordan-normal-form






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      asked Jan 7 at 5:33









      BOlivianoperuano84BOlivianoperuano84

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      1778






















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          $begingroup$

          If $lambda$ is an eigenvalue of $B$, then $lambda^2$ is an eigenvalue of $B^2$. In the Jordan Normal Form, the eigenvalues correspond to entries on the main diagonal. Since all such entries in $B^2$ are $0$, this means that all eigenvalues are $0$ for both $B$ and $B^2$. That takes care of the diagonal entries for the Jordan form of $B$.



          We know that the entries above a Jordan block are all equal to $1$. Since we have only one block of a single eigenvalue, namely $0$, then the above-diagonal entries for the Jordan form of $B$ will be all $1$ and that gives the desired form.






          share|cite|improve this answer









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            $begingroup$

            If $lambda$ is an eigenvalue of $B$, then $lambda^2$ is an eigenvalue of $B^2$. In the Jordan Normal Form, the eigenvalues correspond to entries on the main diagonal. Since all such entries in $B^2$ are $0$, this means that all eigenvalues are $0$ for both $B$ and $B^2$. That takes care of the diagonal entries for the Jordan form of $B$.



            We know that the entries above a Jordan block are all equal to $1$. Since we have only one block of a single eigenvalue, namely $0$, then the above-diagonal entries for the Jordan form of $B$ will be all $1$ and that gives the desired form.






            share|cite|improve this answer









            $endgroup$


















              0












              $begingroup$

              If $lambda$ is an eigenvalue of $B$, then $lambda^2$ is an eigenvalue of $B^2$. In the Jordan Normal Form, the eigenvalues correspond to entries on the main diagonal. Since all such entries in $B^2$ are $0$, this means that all eigenvalues are $0$ for both $B$ and $B^2$. That takes care of the diagonal entries for the Jordan form of $B$.



              We know that the entries above a Jordan block are all equal to $1$. Since we have only one block of a single eigenvalue, namely $0$, then the above-diagonal entries for the Jordan form of $B$ will be all $1$ and that gives the desired form.






              share|cite|improve this answer









              $endgroup$
















                0












                0








                0





                $begingroup$

                If $lambda$ is an eigenvalue of $B$, then $lambda^2$ is an eigenvalue of $B^2$. In the Jordan Normal Form, the eigenvalues correspond to entries on the main diagonal. Since all such entries in $B^2$ are $0$, this means that all eigenvalues are $0$ for both $B$ and $B^2$. That takes care of the diagonal entries for the Jordan form of $B$.



                We know that the entries above a Jordan block are all equal to $1$. Since we have only one block of a single eigenvalue, namely $0$, then the above-diagonal entries for the Jordan form of $B$ will be all $1$ and that gives the desired form.






                share|cite|improve this answer









                $endgroup$



                If $lambda$ is an eigenvalue of $B$, then $lambda^2$ is an eigenvalue of $B^2$. In the Jordan Normal Form, the eigenvalues correspond to entries on the main diagonal. Since all such entries in $B^2$ are $0$, this means that all eigenvalues are $0$ for both $B$ and $B^2$. That takes care of the diagonal entries for the Jordan form of $B$.



                We know that the entries above a Jordan block are all equal to $1$. Since we have only one block of a single eigenvalue, namely $0$, then the above-diagonal entries for the Jordan form of $B$ will be all $1$ and that gives the desired form.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Jan 7 at 7:18









                EuxhenHEuxhenH

                484210




                484210






























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