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Published:
We show that for flip operator $F$, and the family of maximally entangled states \(\operatorname{MAXE}=\{|{\Phi}\rangle||{\Phi}\rangle=\sum|{j_Aj_B}\rangle/\sqrt{d},\{|j\rangle\}\text{ is ONB}\},\) the range of the overlap between $F$ and $|{\Phi}\rangle$ depends on the parity of the dimension. Specifically, \(\{\langle{\Phi|F|\Phi}\rangle||{\Phi}\rangle\in\operatorname{MAXE}\}=\begin{cases}[-1,1]&d=2k\\ [-\frac{d-2}{d},1]&d=2k+1\end{cases}\)
Published:
We show that there is some entangled states that are far from any separable and maximally entangled states. As a consequence, there exists entanglement witness that cannot witness any maximally entangled states. At the first sight it seems to be the opposite: the maximally entangled states contains the ‘most’ entanglement in some sense, so at least one of them should be detected by a fixed entanglement witness. Unfortunately it does not hold.
Published:
Short description of portfolio item number 1
Published:
Short description of portfolio item number 2 
Published in Quantum Science and Technology, 2021
Variational method for metric estimation
Published in Phys. Rev. Applied, 2022
Variational method for entanglement analysis
Published in arXiv preprint, 2023
We can lift full-rank and projective assumptions in self-testing.
Published in Nat. Phys., 2024
We can self-test any real projective measurement in bipartite Bell scenario.
Undergraduate course, University of Copenhagen, 2022
TA.
Undergraduate course, University of Copenhagen, 2023
TA.