Understanding the classification of quantum states based on partial transposition: representations of the bipartite density matrixModeling energy relaxation effects with density matrix formalismHow to calculate the off-diagonal elements of a density matrix using the measurement result?How is measurement modelled when using the density operator?How do we derive the density operator of a subsystem?The classical simulation of 2D graph state and the measurement based quantum computationThe relationship between entanglement of vector states to matrix operationsWhy is a density operator defined the way it's defined?How to show a density matrix is in a pure/mixed state?Finding separable decompositions of bipartite X-states using the methodology of Li and QiaoQuantum fidelity simplified formula while both of the density matrices are single qubit states
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Understanding the classification of quantum states based on partial transposition: representations of the bipartite density matrix
Modeling energy relaxation effects with density matrix formalismHow to calculate the off-diagonal elements of a density matrix using the measurement result?How is measurement modelled when using the density operator?How do we derive the density operator of a subsystem?The classical simulation of 2D graph state and the measurement based quantum computationThe relationship between entanglement of vector states to matrix operationsWhy is a density operator defined the way it's defined?How to show a density matrix is in a pure/mixed state?Finding separable decompositions of bipartite X-states using the methodology of Li and QiaoQuantum fidelity simplified formula while both of the density matrices are single qubit states
.everyoneloves__top-leaderboard:empty,.everyoneloves__mid-leaderboard:empty,.everyoneloves__bot-mid-leaderboard:empty margin-bottom:0;
$begingroup$
I'm going through some slides on the PPT/NPT criteria along with Horodecki's paper, and I'm kind of stuck. Let's take this slide:
Firstly, why can we write a bipartite density matrix as $sum_ijklrho_kl^ij|iranglelangle j|otimes |kranglelangle l|$? What states are the index labels $i, j, k, l$ referring to?
Secondly, Horodecki says on page 21 that if a $rho_AB$ is separable then the new matrix $rho_AB^T_B$ with matrix elements can be defined in some product basis as $langle m|langle mu |rho_AB^T_B|nrangle|nurangle = langle m|langle nu|rho_AB|nrangle|murangle$. I don't quite understand where they're getting this form from. What are $|mrangle, |nrangle, |murangle, |nurangle$?
entanglement density-matrix
$endgroup$
add a comment |
$begingroup$
I'm going through some slides on the PPT/NPT criteria along with Horodecki's paper, and I'm kind of stuck. Let's take this slide:
Firstly, why can we write a bipartite density matrix as $sum_ijklrho_kl^ij|iranglelangle j|otimes |kranglelangle l|$? What states are the index labels $i, j, k, l$ referring to?
Secondly, Horodecki says on page 21 that if a $rho_AB$ is separable then the new matrix $rho_AB^T_B$ with matrix elements can be defined in some product basis as $langle m|langle mu |rho_AB^T_B|nrangle|nurangle = langle m|langle nu|rho_AB|nrangle|murangle$. I don't quite understand where they're getting this form from. What are $|mrangle, |nrangle, |murangle, |nurangle$?
entanglement density-matrix
$endgroup$
$begingroup$
What notation are you familiar with for a bipartite density matrix?
$endgroup$
– Mahathi Vempati
Jun 17 at 12:57
1
$begingroup$
I kinda thought about it and understand the first notation now. It's basically a tensor product of the outer product representation of density matrices.
$endgroup$
– Sanchayan Dutta
Jun 17 at 15:26
add a comment |
$begingroup$
I'm going through some slides on the PPT/NPT criteria along with Horodecki's paper, and I'm kind of stuck. Let's take this slide:
Firstly, why can we write a bipartite density matrix as $sum_ijklrho_kl^ij|iranglelangle j|otimes |kranglelangle l|$? What states are the index labels $i, j, k, l$ referring to?
Secondly, Horodecki says on page 21 that if a $rho_AB$ is separable then the new matrix $rho_AB^T_B$ with matrix elements can be defined in some product basis as $langle m|langle mu |rho_AB^T_B|nrangle|nurangle = langle m|langle nu|rho_AB|nrangle|murangle$. I don't quite understand where they're getting this form from. What are $|mrangle, |nrangle, |murangle, |nurangle$?
entanglement density-matrix
$endgroup$
I'm going through some slides on the PPT/NPT criteria along with Horodecki's paper, and I'm kind of stuck. Let's take this slide:
Firstly, why can we write a bipartite density matrix as $sum_ijklrho_kl^ij|iranglelangle j|otimes |kranglelangle l|$? What states are the index labels $i, j, k, l$ referring to?
Secondly, Horodecki says on page 21 that if a $rho_AB$ is separable then the new matrix $rho_AB^T_B$ with matrix elements can be defined in some product basis as $langle m|langle mu |rho_AB^T_B|nrangle|nurangle = langle m|langle nu|rho_AB|nrangle|murangle$. I don't quite understand where they're getting this form from. What are $|mrangle, |nrangle, |murangle, |nurangle$?
entanglement density-matrix
entanglement density-matrix
edited Jun 17 at 15:29
Sanchayan Dutta
asked Jun 17 at 10:06
Sanchayan DuttaSanchayan Dutta
7,8774 gold badges16 silver badges62 bronze badges
7,8774 gold badges16 silver badges62 bronze badges
$begingroup$
What notation are you familiar with for a bipartite density matrix?
$endgroup$
– Mahathi Vempati
Jun 17 at 12:57
1
$begingroup$
I kinda thought about it and understand the first notation now. It's basically a tensor product of the outer product representation of density matrices.
$endgroup$
– Sanchayan Dutta
Jun 17 at 15:26
add a comment |
$begingroup$
What notation are you familiar with for a bipartite density matrix?
$endgroup$
– Mahathi Vempati
Jun 17 at 12:57
1
$begingroup$
I kinda thought about it and understand the first notation now. It's basically a tensor product of the outer product representation of density matrices.
$endgroup$
– Sanchayan Dutta
Jun 17 at 15:26
$begingroup$
What notation are you familiar with for a bipartite density matrix?
$endgroup$
– Mahathi Vempati
Jun 17 at 12:57
$begingroup$
What notation are you familiar with for a bipartite density matrix?
$endgroup$
– Mahathi Vempati
Jun 17 at 12:57
1
1
$begingroup$
I kinda thought about it and understand the first notation now. It's basically a tensor product of the outer product representation of density matrices.
$endgroup$
– Sanchayan Dutta
Jun 17 at 15:26
$begingroup$
I kinda thought about it and understand the first notation now. It's basically a tensor product of the outer product representation of density matrices.
$endgroup$
– Sanchayan Dutta
Jun 17 at 15:26
add a comment |
1 Answer
1
active
oldest
votes
$begingroup$
For any orthonormal basis that you pick, call it $|e_irangle$, you can write a matrix in terms of that basis as
$$
rho=sum_i,jrho_i,j|e_iranglelangle e_j|.
$$
When you're talking about a bipartite system, a sensible basis is one based on product states, usually the tensor product between two single-system orthonormal bases. So, you might write
$$
|e_irangle=|nrangle|nurangle,
$$
splitting the sum over $i$ into two sums, over $n$ and $nu$. Hence, you can write
$$
rho=sum_n,nu,m,murho_n,nu,m,mu|nranglelangle m|otimes|nuranglelanglemu|.
$$
It just happens that they've chosen to change where the different indices are put.
As for the partial transpose, that is simply the definition of the partial transpose. It may not seem so familiar, but recall with the transpose does,
$$
langle e_i|rho|e_jrangle=langle e_j|rho^T|e_irangle.
$$
All the partial transpose does is that it only switches the left and right indices for the second subsystem, not the first.
In fact, this definition of
$$
langle n,nu|rho|m,murangle=langle n,mu|rho^T_B|m,nurangle
$$
is a general definition. It's not about whether $rho$ is separable or not. The point is that if it is separable, then $rho^T_B$ is still a valid quantum state. On the other hand, if $rho$ were not separable, there is no reason why $rho^T_B$ need be a valid quantum state. In particular, it could have negative eigenvalues.
$endgroup$
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
add a comment |
Your Answer
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1 Answer
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1 Answer
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oldest
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active
oldest
votes
$begingroup$
For any orthonormal basis that you pick, call it $|e_irangle$, you can write a matrix in terms of that basis as
$$
rho=sum_i,jrho_i,j|e_iranglelangle e_j|.
$$
When you're talking about a bipartite system, a sensible basis is one based on product states, usually the tensor product between two single-system orthonormal bases. So, you might write
$$
|e_irangle=|nrangle|nurangle,
$$
splitting the sum over $i$ into two sums, over $n$ and $nu$. Hence, you can write
$$
rho=sum_n,nu,m,murho_n,nu,m,mu|nranglelangle m|otimes|nuranglelanglemu|.
$$
It just happens that they've chosen to change where the different indices are put.
As for the partial transpose, that is simply the definition of the partial transpose. It may not seem so familiar, but recall with the transpose does,
$$
langle e_i|rho|e_jrangle=langle e_j|rho^T|e_irangle.
$$
All the partial transpose does is that it only switches the left and right indices for the second subsystem, not the first.
In fact, this definition of
$$
langle n,nu|rho|m,murangle=langle n,mu|rho^T_B|m,nurangle
$$
is a general definition. It's not about whether $rho$ is separable or not. The point is that if it is separable, then $rho^T_B$ is still a valid quantum state. On the other hand, if $rho$ were not separable, there is no reason why $rho^T_B$ need be a valid quantum state. In particular, it could have negative eigenvalues.
$endgroup$
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
add a comment |
$begingroup$
For any orthonormal basis that you pick, call it $|e_irangle$, you can write a matrix in terms of that basis as
$$
rho=sum_i,jrho_i,j|e_iranglelangle e_j|.
$$
When you're talking about a bipartite system, a sensible basis is one based on product states, usually the tensor product between two single-system orthonormal bases. So, you might write
$$
|e_irangle=|nrangle|nurangle,
$$
splitting the sum over $i$ into two sums, over $n$ and $nu$. Hence, you can write
$$
rho=sum_n,nu,m,murho_n,nu,m,mu|nranglelangle m|otimes|nuranglelanglemu|.
$$
It just happens that they've chosen to change where the different indices are put.
As for the partial transpose, that is simply the definition of the partial transpose. It may not seem so familiar, but recall with the transpose does,
$$
langle e_i|rho|e_jrangle=langle e_j|rho^T|e_irangle.
$$
All the partial transpose does is that it only switches the left and right indices for the second subsystem, not the first.
In fact, this definition of
$$
langle n,nu|rho|m,murangle=langle n,mu|rho^T_B|m,nurangle
$$
is a general definition. It's not about whether $rho$ is separable or not. The point is that if it is separable, then $rho^T_B$ is still a valid quantum state. On the other hand, if $rho$ were not separable, there is no reason why $rho^T_B$ need be a valid quantum state. In particular, it could have negative eigenvalues.
$endgroup$
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
add a comment |
$begingroup$
For any orthonormal basis that you pick, call it $|e_irangle$, you can write a matrix in terms of that basis as
$$
rho=sum_i,jrho_i,j|e_iranglelangle e_j|.
$$
When you're talking about a bipartite system, a sensible basis is one based on product states, usually the tensor product between two single-system orthonormal bases. So, you might write
$$
|e_irangle=|nrangle|nurangle,
$$
splitting the sum over $i$ into two sums, over $n$ and $nu$. Hence, you can write
$$
rho=sum_n,nu,m,murho_n,nu,m,mu|nranglelangle m|otimes|nuranglelanglemu|.
$$
It just happens that they've chosen to change where the different indices are put.
As for the partial transpose, that is simply the definition of the partial transpose. It may not seem so familiar, but recall with the transpose does,
$$
langle e_i|rho|e_jrangle=langle e_j|rho^T|e_irangle.
$$
All the partial transpose does is that it only switches the left and right indices for the second subsystem, not the first.
In fact, this definition of
$$
langle n,nu|rho|m,murangle=langle n,mu|rho^T_B|m,nurangle
$$
is a general definition. It's not about whether $rho$ is separable or not. The point is that if it is separable, then $rho^T_B$ is still a valid quantum state. On the other hand, if $rho$ were not separable, there is no reason why $rho^T_B$ need be a valid quantum state. In particular, it could have negative eigenvalues.
$endgroup$
For any orthonormal basis that you pick, call it $|e_irangle$, you can write a matrix in terms of that basis as
$$
rho=sum_i,jrho_i,j|e_iranglelangle e_j|.
$$
When you're talking about a bipartite system, a sensible basis is one based on product states, usually the tensor product between two single-system orthonormal bases. So, you might write
$$
|e_irangle=|nrangle|nurangle,
$$
splitting the sum over $i$ into two sums, over $n$ and $nu$. Hence, you can write
$$
rho=sum_n,nu,m,murho_n,nu,m,mu|nranglelangle m|otimes|nuranglelanglemu|.
$$
It just happens that they've chosen to change where the different indices are put.
As for the partial transpose, that is simply the definition of the partial transpose. It may not seem so familiar, but recall with the transpose does,
$$
langle e_i|rho|e_jrangle=langle e_j|rho^T|e_irangle.
$$
All the partial transpose does is that it only switches the left and right indices for the second subsystem, not the first.
In fact, this definition of
$$
langle n,nu|rho|m,murangle=langle n,mu|rho^T_B|m,nurangle
$$
is a general definition. It's not about whether $rho$ is separable or not. The point is that if it is separable, then $rho^T_B$ is still a valid quantum state. On the other hand, if $rho$ were not separable, there is no reason why $rho^T_B$ need be a valid quantum state. In particular, it could have negative eigenvalues.
edited Jun 17 at 17:23
Sanchayan Dutta
7,8774 gold badges16 silver badges62 bronze badges
7,8774 gold badges16 silver badges62 bronze badges
answered Jun 17 at 15:39
DaftWullieDaftWullie
18.2k1 gold badge7 silver badges46 bronze badges
18.2k1 gold badge7 silver badges46 bronze badges
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
add a comment |
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
Thanks, btw I think there was a small typo...edited it. :)
$endgroup$
– Sanchayan Dutta
Jun 17 at 17:25
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
$begingroup$
@SanchayanDutta indeed :)
$endgroup$
– DaftWullie
Jun 17 at 17:55
add a comment |
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$begingroup$
What notation are you familiar with for a bipartite density matrix?
$endgroup$
– Mahathi Vempati
Jun 17 at 12:57
1
$begingroup$
I kinda thought about it and understand the first notation now. It's basically a tensor product of the outer product representation of density matrices.
$endgroup$
– Sanchayan Dutta
Jun 17 at 15:26