Necessary and sufficient condition for non-zero quantum discord
arXiv:1004.0190 · doi:10.1103/PhysRevLett.105.190502
Abstract
Quantum discord characterizes "non-classicality" of correlations in quantum mechanics. It has been proposed as the key resource present in certain quantum communication tasks and quantum computational models without containing much entanglement. We obtain a necessary and sufficient condition for the existence of non-zero quantum discord for any dimensional bipartite states. This condition is easily experimentally implementable. Based on this, we propose a geometrical way of quantifying quantum discord. For two qubits this results in a closed form of expression for discord. We apply our results to the model of deterministic quantum computation with one qubit, showing that quantum discord is unlikely to be the reason behind its speedup.
minor changes, published version
References in corpus (9)
- Quantum discord and the power of one qubit
- Experimental quantum computing without entanglement
- On the quantum, classical and total amount of correlations in a quantum state
- No-local-broadcasting theorem for quantum correlations
- Quantum discord and quantum phase transition in spin chains
- Vanishing quantum discord is necessary and sufficient for completely positive maps
- On the role of entanglement and correlations in mixed-state quantum computation
- Completely Positive Maps and Classical Correlations
- Quantum discord and local demons
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- Quantum discord for general two--qubit states: Analytical progress
- Linking Quantum Discord to Entanglement in a Measurement
- Quantum discord and geometry for a class of two-qubit states
- Optimal measurements to access classical correlations of two-qubit states
- Frozen discord in non-Markovian dephasing channels
- Detecting Multipartite Classical States and their Resemblances
- Measurement-induced disturbance and thermal entanglement in spin models
- Witness to detect quantum correlation of bipartite states in arbitrary dimension