In quantum theory, no-go theorems are important as they rule out the existence of a particular physical model under consideration. For instance, the Greenberger-Horne-Zeilinger (GHZ) theorem serves as a no-go theorem for the nonexistence of local hidden variable models by presenting a full contradiction for the multipartite GHZ states. However, the elegant GHZ argument for Bell’s nonlocality does not go through for bipartite Einstein-Podolsky-Rosen (EPR) state. Recent study on quantum nonlocality has shown that the more precise description of EPR’s original scenario is “steering”, i.e., the nonexistence of local hidden state models. Here, we present a simple GHZ-like contradiction for any bipartite pure entangled state, thus proving a no-go...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
The concept of steering was introduced by Schrodinger in 1935 as a generalization of the EPR paradox...
In a recent work [Phys. Rev. Lett. 98, 140402 (2007)] we defined "steering," a type of quantum nonlo...
Recently quantum nonlocality has been classified into three distinct types: quantum entanglement, Ei...
The Einstein-Rosen-Podolsky (EPR) paradox gives an argument for the incompleteness of quantum mechan...
We extend the Greenberger-Horne-Zeilinger (GHZ) theorem to continuous variable cases. This is enable...
In all local realistic theories worked out till now, locality is considered as a basic assumption. M...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
The concept of steering was introduced by Schrodinger in 1935 as a generalization of the EPR paradox...
In a recent work [Phys. Rev. Lett. 98, 140402 (2007)] we defined "steering," a type of quantum nonlo...
Recently quantum nonlocality has been classified into three distinct types: quantum entanglement, Ei...
The Einstein-Rosen-Podolsky (EPR) paradox gives an argument for the incompleteness of quantum mechan...
We extend the Greenberger-Horne-Zeilinger (GHZ) theorem to continuous variable cases. This is enable...
In all local realistic theories worked out till now, locality is considered as a basic assumption. M...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
Starting from the late 60’s many experiments have been performed to verify the violation Bell’s ineq...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...
In 1935, Einstein, Podolsky and Rosen (EPR) originated the famous “EPR paradox” [1]. This ...