Entanglement capability of self-inverse Hamiltonian evolution
arXiv:quant-ph/0212035 · doi:10.1103/PhysRevA.68.014301
Abstract
We determine the entanglement capability of self-inverse Hamiltonian evolution, which reduces to the known result for Ising Hamiltonian, and identify optimal input states for yielding the maximal entanglement rate. We introduce the concept of the operator entanglement rate, and find that the maximal operator entanglement rate gives a lower bound on the entanglement capability of a general Hamiltonian.
4 pages, no figures. Version 3: small changes
References in corpus (11)
- The entangling power of passive optical elements
- Quantum dynamics as a physical resource
- Characterization of non-local gates
- Optimal Entanglement Generation from Quantum Operations
- Interaction cost of non-local gates
- Quantum entanglement of unitary operators on bi-partite systems
- Entangling power and operator entanglement in qudit systems
- Optimal conversion of non--local unitary operations
- Entanglement generation and Hamiltonian simulation in Continuous-Variable Systems
- Simulation of many-body interactions by conditional geometric phases
- Relations for classical communication capacity and entanglement capability of two-qubit operations
Cited by in corpus (11)
- Entanglement as a signature of quantum chaos
- Upper bounds on entangling rates of bipartite Hamiltonians
- Matrix realignment and partial transpose approach to entangling power of quantum evolutions
- Capacity of Entanglement for Non-local Hamiltonian
- Entanglement changing power of two-qubit unitary operations
- Almost All Quantum States Have Low Entropy Rates for Any Coupling to the Environment
- Reversible simulation of bipartite product Hamiltonians
- Entanglement rates for Renyi, Tsallis and other entropies
- Entanglement rates for bipartite open systems
- Optimal entanglement generation in GHZ-type states
- Matrix rearrangement approach for the entangling power with mixed qudit systems