Can I use any basis for the spectral theorem or does it have to be the eigenbasis?

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For a Hermitian operator $A$ on a Hilbert space $H$ with eigenvalues $a_i$ and eigenvectors $v_i$ forming a complete basis, one can write $A$ as:
$$ A = sum_i a_i v_i v_i^dagger, $$
where $v^dagger$ is the Hermitian conjugate of $v$.



Suppose there is another complete basis $w_i$. Can I also use the spectral decomposition with this $w$-basis, instead of the eigenbasis $v_i$?
$$ A = sum_i a_i w_i w_i^dagger $$







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    For a Hermitian operator $A$ on a Hilbert space $H$ with eigenvalues $a_i$ and eigenvectors $v_i$ forming a complete basis, one can write $A$ as:
    $$ A = sum_i a_i v_i v_i^dagger, $$
    where $v^dagger$ is the Hermitian conjugate of $v$.



    Suppose there is another complete basis $w_i$. Can I also use the spectral decomposition with this $w$-basis, instead of the eigenbasis $v_i$?
    $$ A = sum_i a_i w_i w_i^dagger $$







    share|cite|improve this question





















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      For a Hermitian operator $A$ on a Hilbert space $H$ with eigenvalues $a_i$ and eigenvectors $v_i$ forming a complete basis, one can write $A$ as:
      $$ A = sum_i a_i v_i v_i^dagger, $$
      where $v^dagger$ is the Hermitian conjugate of $v$.



      Suppose there is another complete basis $w_i$. Can I also use the spectral decomposition with this $w$-basis, instead of the eigenbasis $v_i$?
      $$ A = sum_i a_i w_i w_i^dagger $$







      share|cite|improve this question











      For a Hermitian operator $A$ on a Hilbert space $H$ with eigenvalues $a_i$ and eigenvectors $v_i$ forming a complete basis, one can write $A$ as:
      $$ A = sum_i a_i v_i v_i^dagger, $$
      where $v^dagger$ is the Hermitian conjugate of $v$.



      Suppose there is another complete basis $w_i$. Can I also use the spectral decomposition with this $w$-basis, instead of the eigenbasis $v_i$?
      $$ A = sum_i a_i w_i w_i^dagger $$









      share|cite|improve this question










      share|cite|improve this question




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      asked Aug 2 at 7:20









      Stephan

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          No, you cannot. The point of an eigenbasis is that it diagonalises the operator; it works on each basis vector separately and independently of the others. That diagonalisation is exactly what you see in the sum.



          Take, for instance, the two-dimensional case with $A$ represented by $left[beginsmallmatrix1&0\0&2endsmallmatrixright]$ in some basis $u_i$. Then that basis is an eigenbais, and you get
          $$
          A = 1cdot u_1u_1^dagger + 2cdot u_2u_2^dagger
          $$
          If you take a new basis, say $v_1 = u_1+u_2$ and $v_2 = u_1-u_2$, then in that basis we have that $A$ is represented by $left[beginsmallmatrix1.5&-0.5\-0.5&1.5endsmallmatrixright]$. Of course, the matrix is still symmetric / Hermitian, because change of basis cannot change that fact. But if you want to decompose it in something like the above sum it's not enough with $v_1v_1^dagger$ and $v_2v_2^dagger$. You need $v_1v_2^dagger$ and $v_2v_1^dagger$ terms as well, as there are now non-zero off-diagonal elements:
          $$
          A = 1.5cdot v_1v_1^dagger + 1.5cdot v_2v_2^dagger - 0.5cdot v_1v_2^dagger - 0.5cdot v_2v_1^dagger
          $$






          share|cite|improve this answer























          • Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
            – Stephan
            Aug 2 at 7:43










          • @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
            – Arthur
            Aug 2 at 7:53











          • I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
            – Stephan
            Aug 2 at 8:03






          • 1




            @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
            – Arthur
            Aug 2 at 8:04






          • 1




            Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
            – Stephan
            Aug 2 at 8:06










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          accepted










          No, you cannot. The point of an eigenbasis is that it diagonalises the operator; it works on each basis vector separately and independently of the others. That diagonalisation is exactly what you see in the sum.



          Take, for instance, the two-dimensional case with $A$ represented by $left[beginsmallmatrix1&0\0&2endsmallmatrixright]$ in some basis $u_i$. Then that basis is an eigenbais, and you get
          $$
          A = 1cdot u_1u_1^dagger + 2cdot u_2u_2^dagger
          $$
          If you take a new basis, say $v_1 = u_1+u_2$ and $v_2 = u_1-u_2$, then in that basis we have that $A$ is represented by $left[beginsmallmatrix1.5&-0.5\-0.5&1.5endsmallmatrixright]$. Of course, the matrix is still symmetric / Hermitian, because change of basis cannot change that fact. But if you want to decompose it in something like the above sum it's not enough with $v_1v_1^dagger$ and $v_2v_2^dagger$. You need $v_1v_2^dagger$ and $v_2v_1^dagger$ terms as well, as there are now non-zero off-diagonal elements:
          $$
          A = 1.5cdot v_1v_1^dagger + 1.5cdot v_2v_2^dagger - 0.5cdot v_1v_2^dagger - 0.5cdot v_2v_1^dagger
          $$






          share|cite|improve this answer























          • Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
            – Stephan
            Aug 2 at 7:43










          • @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
            – Arthur
            Aug 2 at 7:53











          • I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
            – Stephan
            Aug 2 at 8:03






          • 1




            @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
            – Arthur
            Aug 2 at 8:04






          • 1




            Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
            – Stephan
            Aug 2 at 8:06














          up vote
          2
          down vote



          accepted










          No, you cannot. The point of an eigenbasis is that it diagonalises the operator; it works on each basis vector separately and independently of the others. That diagonalisation is exactly what you see in the sum.



          Take, for instance, the two-dimensional case with $A$ represented by $left[beginsmallmatrix1&0\0&2endsmallmatrixright]$ in some basis $u_i$. Then that basis is an eigenbais, and you get
          $$
          A = 1cdot u_1u_1^dagger + 2cdot u_2u_2^dagger
          $$
          If you take a new basis, say $v_1 = u_1+u_2$ and $v_2 = u_1-u_2$, then in that basis we have that $A$ is represented by $left[beginsmallmatrix1.5&-0.5\-0.5&1.5endsmallmatrixright]$. Of course, the matrix is still symmetric / Hermitian, because change of basis cannot change that fact. But if you want to decompose it in something like the above sum it's not enough with $v_1v_1^dagger$ and $v_2v_2^dagger$. You need $v_1v_2^dagger$ and $v_2v_1^dagger$ terms as well, as there are now non-zero off-diagonal elements:
          $$
          A = 1.5cdot v_1v_1^dagger + 1.5cdot v_2v_2^dagger - 0.5cdot v_1v_2^dagger - 0.5cdot v_2v_1^dagger
          $$






          share|cite|improve this answer























          • Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
            – Stephan
            Aug 2 at 7:43










          • @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
            – Arthur
            Aug 2 at 7:53











          • I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
            – Stephan
            Aug 2 at 8:03






          • 1




            @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
            – Arthur
            Aug 2 at 8:04






          • 1




            Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
            – Stephan
            Aug 2 at 8:06












          up vote
          2
          down vote



          accepted







          up vote
          2
          down vote



          accepted






          No, you cannot. The point of an eigenbasis is that it diagonalises the operator; it works on each basis vector separately and independently of the others. That diagonalisation is exactly what you see in the sum.



          Take, for instance, the two-dimensional case with $A$ represented by $left[beginsmallmatrix1&0\0&2endsmallmatrixright]$ in some basis $u_i$. Then that basis is an eigenbais, and you get
          $$
          A = 1cdot u_1u_1^dagger + 2cdot u_2u_2^dagger
          $$
          If you take a new basis, say $v_1 = u_1+u_2$ and $v_2 = u_1-u_2$, then in that basis we have that $A$ is represented by $left[beginsmallmatrix1.5&-0.5\-0.5&1.5endsmallmatrixright]$. Of course, the matrix is still symmetric / Hermitian, because change of basis cannot change that fact. But if you want to decompose it in something like the above sum it's not enough with $v_1v_1^dagger$ and $v_2v_2^dagger$. You need $v_1v_2^dagger$ and $v_2v_1^dagger$ terms as well, as there are now non-zero off-diagonal elements:
          $$
          A = 1.5cdot v_1v_1^dagger + 1.5cdot v_2v_2^dagger - 0.5cdot v_1v_2^dagger - 0.5cdot v_2v_1^dagger
          $$






          share|cite|improve this answer















          No, you cannot. The point of an eigenbasis is that it diagonalises the operator; it works on each basis vector separately and independently of the others. That diagonalisation is exactly what you see in the sum.



          Take, for instance, the two-dimensional case with $A$ represented by $left[beginsmallmatrix1&0\0&2endsmallmatrixright]$ in some basis $u_i$. Then that basis is an eigenbais, and you get
          $$
          A = 1cdot u_1u_1^dagger + 2cdot u_2u_2^dagger
          $$
          If you take a new basis, say $v_1 = u_1+u_2$ and $v_2 = u_1-u_2$, then in that basis we have that $A$ is represented by $left[beginsmallmatrix1.5&-0.5\-0.5&1.5endsmallmatrixright]$. Of course, the matrix is still symmetric / Hermitian, because change of basis cannot change that fact. But if you want to decompose it in something like the above sum it's not enough with $v_1v_1^dagger$ and $v_2v_2^dagger$. You need $v_1v_2^dagger$ and $v_2v_1^dagger$ terms as well, as there are now non-zero off-diagonal elements:
          $$
          A = 1.5cdot v_1v_1^dagger + 1.5cdot v_2v_2^dagger - 0.5cdot v_1v_2^dagger - 0.5cdot v_2v_1^dagger
          $$







          share|cite|improve this answer















          share|cite|improve this answer



          share|cite|improve this answer








          edited Aug 2 at 7:36


























          answered Aug 2 at 7:30









          Arthur

          98.2k793174




          98.2k793174











          • Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
            – Stephan
            Aug 2 at 7:43










          • @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
            – Arthur
            Aug 2 at 7:53











          • I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
            – Stephan
            Aug 2 at 8:03






          • 1




            @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
            – Arthur
            Aug 2 at 8:04






          • 1




            Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
            – Stephan
            Aug 2 at 8:06
















          • Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
            – Stephan
            Aug 2 at 7:43










          • @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
            – Arthur
            Aug 2 at 7:53











          • I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
            – Stephan
            Aug 2 at 8:03






          • 1




            @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
            – Arthur
            Aug 2 at 8:04






          • 1




            Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
            – Stephan
            Aug 2 at 8:06















          Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
          – Stephan
          Aug 2 at 7:43




          Makes sense, thank you for answering. My question arises from the solutions of an exam, where the author apparently used the spectral theorem (exam: phys.uic.edu/docs/default-source/…, solutions: phys.uic.edu/docs/default-source/…). In question 1a), the spectral theorem with a non-eigenbasis is used to show that the operator B has only positive eigenvalues. If I follow your reasoning, this solution does not make sense, does it?
          – Stephan
          Aug 2 at 7:43












          @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
          – Arthur
          Aug 2 at 7:53





          @Stephan No, that's something else. Here it's not the case that they have a $B$ and they decompose it using the eigenbasis of $A$. Rather it's that they use the eigenbasis and spectral decomposition of $A$ to construct $B$ in the first place.
          – Arthur
          Aug 2 at 7:53













          I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
          – Stephan
          Aug 2 at 8:03




          I see, but how can they argue that $|lambda_i|$ are the eigenvalues of $B$ if this is not a spectral decomposition of $B$?
          – Stephan
          Aug 2 at 8:03




          1




          1




          @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
          – Arthur
          Aug 2 at 8:04




          @Stephan It is a spectral decomposition of $B$. That's exactly what $B$ is. It's defined as the matrix with that exact spectral decomposition.
          – Arthur
          Aug 2 at 8:04




          1




          1




          Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
          – Stephan
          Aug 2 at 8:06




          Ah, I think now I get it: we define $B$ in such a way that it shares its eigenbasis with $A$. So as a corollary, $[A,B]=0$, right?
          – Stephan
          Aug 2 at 8:06












           

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