The Quantum Reverse Shannon Theorem states that any quantum channel can be simulated by an unlimited amount of shared entanglement and an amount of classical communication equal to the channel’s entanglement assisted classical capacity. In this paper, we provide a new proof of this theorem, which has previously been proved by Bennett, Devetak, Harrow, Shor, and Winter. Our proof has a clear structure being based on two recent information-theoretic results: one-shot Quantum State Merging and the Post-Selection Technique for quantum channels
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The fully quantum reverse Shannon theorem establishes the optimal rate of noiseless classical commun...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The Quantum Reverse Shannon Theorem states that any quantum channel can be simulated by an unlimited...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The entanglement cost of a quantum channel is the minimal rate at which entanglement (between sender...
The entanglement cost of a quantum channel is the minimal rate at which entanglement (between sender...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymp-totically simul...
Dual to the usual noisy channel coding problem, where a noisy (classical or quantum) channel is used...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
We study and solve the problem of classical channel simulation with quantum side information at the ...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
In this paper, we give tradeoffs between classical communication, quantum communication, and entangl...
The fully quantum reverse Shannon theorem establishes the optimal rate of noiseless classical commun...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The fully quantum reverse Shannon theorem establishes the optimal rate of noiseless classical commun...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The Quantum Reverse Shannon Theorem states that any quantum channel can be simulated by an unlimited...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The entanglement cost of a quantum channel is the minimal rate at which entanglement (between sender...
The entanglement cost of a quantum channel is the minimal rate at which entanglement (between sender...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymp-totically simul...
Dual to the usual noisy channel coding problem, where a noisy (classical or quantum) channel is used...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
We study and solve the problem of classical channel simulation with quantum side information at the ...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
In this paper, we give tradeoffs between classical communication, quantum communication, and entangl...
The fully quantum reverse Shannon theorem establishes the optimal rate of noiseless classical commun...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...
The fully quantum reverse Shannon theorem establishes the optimal rate of noiseless classical commun...
We show that quantum-to-classical channels, i.e., quantum measurements, can be asymptotically simula...