If both Alice and Bob have access to a two-qubit "background state" then, by simulating Everett's many worlds interpretation of measurement, Alice can teleport a qubit to Bob, each using fixed unitaries. If Bob has access to only one of the background qubits, teleportation is still possible by Alice sending Bob one classical bit of information gained from a measurement of the other qubit. The Everett picture unifies unitaries, measurements, and classical communication into just unitaries, provided there are background states shared by all parties
We describe a method for nonobliviously communicating a 2l-qubit quantum state by physically transmi...
The `no communication' theorem prohibits superluminal communication by showing that any measurement ...
Quantum teleportation is one of the most important protocols in quantum information. By exploiting t...
We present a simultaneous quantum state teleportation scheme, in which receivers can not recover the...
We explicitly show a protocol in which an arbitrary two qubit state vertical bar phi >=a vertical ba...
Classical teleportation is defined as a scenario where the sender is given the classical description...
We give a description of the teleportation of an unknown quantum state which takes into account the ...
The article by Bouwmeester et al. on experimental quantum teleportation constitutes an important adv...
Several protocols for controlled teleportation were suggested by Yang, Chu, and Han [PRA 70, 022329 ...
A particularly startling discovery by Bennett et al. is the possibility for teleportation of a quant...
This is to reply to the comment of Kenigsberg and Mor on our previous work ``Efficient many-party co...
The amount of information transferred during quantum teleportation is equal to the preparation infor...
Recently, several aspects of controlled quantum communication (e.g., bidirectional controlled state ...
The controversial issue of information transfer in the quantum teleportation procedure is analyzed i...
We present a method to create a variety of interesting gates by teleporting quantum bits through spe...
We describe a method for nonobliviously communicating a 2l-qubit quantum state by physically transmi...
The `no communication' theorem prohibits superluminal communication by showing that any measurement ...
Quantum teleportation is one of the most important protocols in quantum information. By exploiting t...
We present a simultaneous quantum state teleportation scheme, in which receivers can not recover the...
We explicitly show a protocol in which an arbitrary two qubit state vertical bar phi >=a vertical ba...
Classical teleportation is defined as a scenario where the sender is given the classical description...
We give a description of the teleportation of an unknown quantum state which takes into account the ...
The article by Bouwmeester et al. on experimental quantum teleportation constitutes an important adv...
Several protocols for controlled teleportation were suggested by Yang, Chu, and Han [PRA 70, 022329 ...
A particularly startling discovery by Bennett et al. is the possibility for teleportation of a quant...
This is to reply to the comment of Kenigsberg and Mor on our previous work ``Efficient many-party co...
The amount of information transferred during quantum teleportation is equal to the preparation infor...
Recently, several aspects of controlled quantum communication (e.g., bidirectional controlled state ...
The controversial issue of information transfer in the quantum teleportation procedure is analyzed i...
We present a method to create a variety of interesting gates by teleporting quantum bits through spe...
We describe a method for nonobliviously communicating a 2l-qubit quantum state by physically transmi...
The `no communication' theorem prohibits superluminal communication by showing that any measurement ...
Quantum teleportation is one of the most important protocols in quantum information. By exploiting t...