Commutant of Jordan Block











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Matrices $B in mathbf{C}^{ntimes n}$ commuting with a given Jordan block $A$ are known to be upper triangular Toeplitz matrices. I have seen convincing proofs, but I wanted to derive this fact by my own method (in Dirac notation) which does not seem to work:




  1. Consider the generalized eigenbasis (Jordan basis) for A and its adjoint $A^dagger$ belonging to eigenvalue $lambda$: $|R_irangle in ker(A-lambda)^i- ker(A-lambda)^{i-1}, |L_jrangle in ker(A^dagger-lambda^*)^i- ker(A^dagger-lambda^*)^{i-1}$ giving rise to Jordan chains: $|R_{i-1}rangle = ker(A-lambda)|R_irangle, |L_{i-1}rangle = ker(A^dagger-lambda^*)|L_irangle$


  2. Express $B$ in this (right and left) basis: $B = sum_{ij} B_{ij}|R_irangle langle L_j|$


  3. Apply $A$ on left resp. right:



$AB=sum_{ij} B_{ij}A|R_irangle langle L_j|= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|$



$BA=sum_{ij} B_{ij}|R_irangle langle L_j|A= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$




  1. So we have the equality $sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|=sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$


  2. Redefining summation indices via $k:=i-1$ and $l:=j-1$ yields



$sum_{kj} B_{k+1,j}|R_kranglelangle L_j|=sum_{il} B_{i,l+1}|R_iranglelangle L_l|$




  1. Since $|R_irangle langle L_j|$ constitutes a basis for the space of matrices, this equality holds for the respective coefficients separately: $B_{i+1,j}=B_{i,j+1}$


But Toeplitz matrices are characterized by $B_{i+1,j}=B_{i,j-1}$! What is wrong here?










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    Matrices $B in mathbf{C}^{ntimes n}$ commuting with a given Jordan block $A$ are known to be upper triangular Toeplitz matrices. I have seen convincing proofs, but I wanted to derive this fact by my own method (in Dirac notation) which does not seem to work:




    1. Consider the generalized eigenbasis (Jordan basis) for A and its adjoint $A^dagger$ belonging to eigenvalue $lambda$: $|R_irangle in ker(A-lambda)^i- ker(A-lambda)^{i-1}, |L_jrangle in ker(A^dagger-lambda^*)^i- ker(A^dagger-lambda^*)^{i-1}$ giving rise to Jordan chains: $|R_{i-1}rangle = ker(A-lambda)|R_irangle, |L_{i-1}rangle = ker(A^dagger-lambda^*)|L_irangle$


    2. Express $B$ in this (right and left) basis: $B = sum_{ij} B_{ij}|R_irangle langle L_j|$


    3. Apply $A$ on left resp. right:



    $AB=sum_{ij} B_{ij}A|R_irangle langle L_j|= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|$



    $BA=sum_{ij} B_{ij}|R_irangle langle L_j|A= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$




    1. So we have the equality $sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|=sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$


    2. Redefining summation indices via $k:=i-1$ and $l:=j-1$ yields



    $sum_{kj} B_{k+1,j}|R_kranglelangle L_j|=sum_{il} B_{i,l+1}|R_iranglelangle L_l|$




    1. Since $|R_irangle langle L_j|$ constitutes a basis for the space of matrices, this equality holds for the respective coefficients separately: $B_{i+1,j}=B_{i,j+1}$


    But Toeplitz matrices are characterized by $B_{i+1,j}=B_{i,j-1}$! What is wrong here?










    share|cite|improve this question


























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      Matrices $B in mathbf{C}^{ntimes n}$ commuting with a given Jordan block $A$ are known to be upper triangular Toeplitz matrices. I have seen convincing proofs, but I wanted to derive this fact by my own method (in Dirac notation) which does not seem to work:




      1. Consider the generalized eigenbasis (Jordan basis) for A and its adjoint $A^dagger$ belonging to eigenvalue $lambda$: $|R_irangle in ker(A-lambda)^i- ker(A-lambda)^{i-1}, |L_jrangle in ker(A^dagger-lambda^*)^i- ker(A^dagger-lambda^*)^{i-1}$ giving rise to Jordan chains: $|R_{i-1}rangle = ker(A-lambda)|R_irangle, |L_{i-1}rangle = ker(A^dagger-lambda^*)|L_irangle$


      2. Express $B$ in this (right and left) basis: $B = sum_{ij} B_{ij}|R_irangle langle L_j|$


      3. Apply $A$ on left resp. right:



      $AB=sum_{ij} B_{ij}A|R_irangle langle L_j|= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|$



      $BA=sum_{ij} B_{ij}|R_irangle langle L_j|A= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$




      1. So we have the equality $sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|=sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$


      2. Redefining summation indices via $k:=i-1$ and $l:=j-1$ yields



      $sum_{kj} B_{k+1,j}|R_kranglelangle L_j|=sum_{il} B_{i,l+1}|R_iranglelangle L_l|$




      1. Since $|R_irangle langle L_j|$ constitutes a basis for the space of matrices, this equality holds for the respective coefficients separately: $B_{i+1,j}=B_{i,j+1}$


      But Toeplitz matrices are characterized by $B_{i+1,j}=B_{i,j-1}$! What is wrong here?










      share|cite|improve this question















      Matrices $B in mathbf{C}^{ntimes n}$ commuting with a given Jordan block $A$ are known to be upper triangular Toeplitz matrices. I have seen convincing proofs, but I wanted to derive this fact by my own method (in Dirac notation) which does not seem to work:




      1. Consider the generalized eigenbasis (Jordan basis) for A and its adjoint $A^dagger$ belonging to eigenvalue $lambda$: $|R_irangle in ker(A-lambda)^i- ker(A-lambda)^{i-1}, |L_jrangle in ker(A^dagger-lambda^*)^i- ker(A^dagger-lambda^*)^{i-1}$ giving rise to Jordan chains: $|R_{i-1}rangle = ker(A-lambda)|R_irangle, |L_{i-1}rangle = ker(A^dagger-lambda^*)|L_irangle$


      2. Express $B$ in this (right and left) basis: $B = sum_{ij} B_{ij}|R_irangle langle L_j|$


      3. Apply $A$ on left resp. right:



      $AB=sum_{ij} B_{ij}A|R_irangle langle L_j|= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|$



      $BA=sum_{ij} B_{ij}|R_irangle langle L_j|A= sum_{ij} B_{ij}lambda|R_irangle langle L_j|+sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$




      1. So we have the equality $sum_{ij} B_{ij}|R_{i-1}ranglelangle L_j|=sum_{ij} B_{ij}|R_iranglelangle L_{j-1}|$


      2. Redefining summation indices via $k:=i-1$ and $l:=j-1$ yields



      $sum_{kj} B_{k+1,j}|R_kranglelangle L_j|=sum_{il} B_{i,l+1}|R_iranglelangle L_l|$




      1. Since $|R_irangle langle L_j|$ constitutes a basis for the space of matrices, this equality holds for the respective coefficients separately: $B_{i+1,j}=B_{i,j+1}$


      But Toeplitz matrices are characterized by $B_{i+1,j}=B_{i,j-1}$! What is wrong here?







      linear-algebra abstract-algebra matrices jordan-normal-form






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      edited Nov 26 at 23:03

























      asked Nov 24 at 9:45









      quantumorsch

      1006




      1006






















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          Your error is actually fairly straightforward. It's that you've expressed $B$ with your right and left bases, but when we say that the matrices that commute with a Jordan block are Toeplitz matrices, we express those matrices inputs and outputs both in the right basis.



          The key to fixing your argument is to switch everything to the right basis at the end. It's obvious from the matrix for a Jordan block (and then taking its conjugate transpose), that $|L_jrangle = |R_{n-j}rangle$. Using this equality, your equality of matrix entries becomes $B_{i+1,n-j}=B_{i,n-(j+1)}=B_{i,n-j-1}$, and reindexing with $j=n-j$, we get $B_{i+1,j}=B_{i,j-1}$ as desired.






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            Your error is actually fairly straightforward. It's that you've expressed $B$ with your right and left bases, but when we say that the matrices that commute with a Jordan block are Toeplitz matrices, we express those matrices inputs and outputs both in the right basis.



            The key to fixing your argument is to switch everything to the right basis at the end. It's obvious from the matrix for a Jordan block (and then taking its conjugate transpose), that $|L_jrangle = |R_{n-j}rangle$. Using this equality, your equality of matrix entries becomes $B_{i+1,n-j}=B_{i,n-(j+1)}=B_{i,n-j-1}$, and reindexing with $j=n-j$, we get $B_{i+1,j}=B_{i,j-1}$ as desired.






            share|cite|improve this answer

























              up vote
              0
              down vote













              Your error is actually fairly straightforward. It's that you've expressed $B$ with your right and left bases, but when we say that the matrices that commute with a Jordan block are Toeplitz matrices, we express those matrices inputs and outputs both in the right basis.



              The key to fixing your argument is to switch everything to the right basis at the end. It's obvious from the matrix for a Jordan block (and then taking its conjugate transpose), that $|L_jrangle = |R_{n-j}rangle$. Using this equality, your equality of matrix entries becomes $B_{i+1,n-j}=B_{i,n-(j+1)}=B_{i,n-j-1}$, and reindexing with $j=n-j$, we get $B_{i+1,j}=B_{i,j-1}$ as desired.






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                up vote
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                up vote
                0
                down vote









                Your error is actually fairly straightforward. It's that you've expressed $B$ with your right and left bases, but when we say that the matrices that commute with a Jordan block are Toeplitz matrices, we express those matrices inputs and outputs both in the right basis.



                The key to fixing your argument is to switch everything to the right basis at the end. It's obvious from the matrix for a Jordan block (and then taking its conjugate transpose), that $|L_jrangle = |R_{n-j}rangle$. Using this equality, your equality of matrix entries becomes $B_{i+1,n-j}=B_{i,n-(j+1)}=B_{i,n-j-1}$, and reindexing with $j=n-j$, we get $B_{i+1,j}=B_{i,j-1}$ as desired.






                share|cite|improve this answer












                Your error is actually fairly straightforward. It's that you've expressed $B$ with your right and left bases, but when we say that the matrices that commute with a Jordan block are Toeplitz matrices, we express those matrices inputs and outputs both in the right basis.



                The key to fixing your argument is to switch everything to the right basis at the end. It's obvious from the matrix for a Jordan block (and then taking its conjugate transpose), that $|L_jrangle = |R_{n-j}rangle$. Using this equality, your equality of matrix entries becomes $B_{i+1,n-j}=B_{i,n-(j+1)}=B_{i,n-j-1}$, and reindexing with $j=n-j$, we get $B_{i+1,j}=B_{i,j-1}$ as desired.







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                answered Nov 29 at 3:01









                jgon

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