Homework Help: Quantum Information Theory 1

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The discussion focuses on the properties of a positive operator X in quantum information theory and its relation to superoperators. It defines X using a sum over basis states and discusses the Schur product, noting that the superoperator preserves the trace of X. The trace is expressed in terms of the inner products involving the operator P and X. The conversation raises a question about proving that the operator ΛP(X) is completely positive (CP) based on the non-negativity of the trace and the properties of the involved operators. The conclusion emphasizes the need to establish that the product of the inner products remains non-negative to support the claim of complete positivity.
maomao
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Homework Statement
Given a vector space ##X = \mathbb{C}^\Sigma##, with a standard basis ##\left\{ |a\rangle, a \in \Sigma \right\}##. Given two operators ##V, W \in \mathcal{L}(\mathcal{X})##, the Schur product of ##V## and ##W##, denoted by ##V \odot W \in \mathcal{L}(\mathcal{X})##, is defined as the operator whose components respect to the standard basis are:
##\langle a| V \odot W |b \rangle = \langle a| V |b \rangle \langle a| W |b\rangle , \forall a, b \in \Sigma##.
Given a positive semidefinite operator ##P \in \text{Pos}(\mathcal{X}) ##, the associated Schur superoperator to ##P##, denoted ##\Lambda_P \in \text{T}(\mathcal{X})##, is defined as ##\Lambda_P (X) = P \odot X, \forall X \in \mathcal{L}(\mathcal{X})##.
Prove that ##\Lambda_P (X) \in \text{CP}(\mathcal{X})##.
Relevant Equations
The relevant points I have to prove that a superoperator is completely positive (CP) ##\Phi \in \text{T}(\mathcal{X},\mathcal{Y})##, where ##\mathcal{X}## and ##\mathcal{Y}## are complex Euclidean spaces, are the following statements:
1. ##\Phi## is CP, e.g., ##\Phi \in \text{CP}(\mathcal{X}, \mathcal{Y})##.

2. ##\Phi \otimes \mathbb{I}_{\mathcal{L}(\mathcal{X})}## is positive.

3. ##J(\Phi) \in \text{Pos}(\mathcal{Y} \otimes \mathcal{X}) ##.

4. ##A_1, \cdots , A_N \in \mathcal{L}(\mathcal{X},\mathcal{Y})## exist so that,
## \Phi (X) = \sum_{k=1}^N A_k X A^{\dagger}_k , \forall X \in \mathcal{L}(\mathcal{X})##

5. Point 4. holds for ##N = \text{rank} [J( \Phi)]##.

6. There exists a complex Euclidean space ##\mathcal{Z}## and an operator ##A \in \mathcal{L}(\mathcal{X}, \mathcal{Y} \otimes \mathcal{Z})## such that:
## \Phi (X) = \text{Tr}_{\mathcal{Z}} (AXA^\dagger) , \forall X \in \mathcal{L}(\mathcal{X})##

7. Point 6. holds for ##\text{dim} \mathcal{Z} = \text{rank} [J(\Phi)]##.
I considered an operator ##X \in \mathcal{L}(\mathcal{X} \otimes \mathcal{K})##, that is positive, ##X \geq 0##. And I defined it as it follows:
##X = \sum_{i,j} a_{ij} ∣x_i \rangle \langle x_i ∣ \otimes ∣k_j \rangle \langle k_j∣ ##​
Where ##x_i## are basis for ##\mathcal{X}## and ##k_j## basis for ##\mathcal{Y}##. Then, we remember the Schur product for the operator: ##\Lambda_P (X) = P \odot X##.
Another important point is that a superoperator ##\Phi## preserves the trace: ##\text{Tr} [\Phi (X)] = \text{Tr} (X), \forall X \in \mathcal{L}(\mathcal{X})##, and since the trace is ##\text{Tr}(A) = \sum_i \langle i ∣ A ∣i \rangle##, then,

##\text{Tr} [\Phi (X)] = \text{Tr} [ P \odot X ] = \sum_k \langle k∣ P \odot X ∣k \rangle = \langle k∣ P ∣k \rangle \hspace{1mm} \sum_k \langle k∣ X ∣k \rangle##​

The sum in ##k## represents the Trace of ##X##, ##\text{Tr}(X)##, and this is why ##\langle k∣ P ∣k \rangle = 1##, but I am not sure how could this prove that ##\Lambda_P (X)## is CP.
I understand that, since X is semi-definite positive, ##\langle k∣ X ∣k \rangle \geq 0##. Then, if ##\langle k∣ P ∣k \rangle##, which I already said that it has to be equal to ##1## to hold the equality, is also non-negative, the product ##\langle k∣ P ∣k \rangle \langle k∣ X ∣k \rangle## will also be non-negative. Is this enough to prove that ##\Lambda_P (X) \geq 0##?
 
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At first, I derived that: $$\nabla \frac 1{\mu}=-\frac 1{{\mu}^3}\left((1-\beta^2)+\frac{\dot{\vec\beta}\cdot\vec R}c\right)\vec R$$ (dot means differentiation with respect to ##t'##). I assume this result is true because it gives valid result for magnetic field. To find electric field one should also derive partial derivative of ##\vec A## with respect to ##t##. I've used chain rule, substituted ##\vec A## and used derivative of product formula. $$\frac {\partial \vec A}{\partial t}=\frac...