Qutrit witness from the Grothendieck constant of order four
arXiv:1707.04719 · doi:10.1103/PhysRevA.96.012113
Abstract
In this paper, we prove that , where denotes the Grothendieck constant of order . To this end, we use a branch-and-bound algorithm commonly used in the solution of NP-hard problems. It has recently been proven that . Here we prove that , which has implications for device-independent witnessing dimensions greater than two. Furthermore, the algorithm with some modifications may find applications in various black-box quantum information tasks with large number of inputs and outputs.
13 pages, 2 figures
References in corpus (16)
- Steering, Entanglement, Nonlocality, and the EPR Paradox
- Bounding the set of quantum correlations
- Testing the Hilbert space dimension
- Preparation contextuality powers parity-oblivious multiplexing
- Grothendieck's constant and local models for noisy entangled quantum states
- Unbounded violation of tripartite Bell inequalities
- More efficient Bell inequalities for Werner states
- Quantum Random Access Codes using Single -level Systems
- Local hidden--variable models for entangled quantum states
- Bounding the set of finite dimensional quantum correlations
- Generalized Clauser-Horne-Shimony-Holt inequalities maximally violated by higher dimensional systems
- Towards Grothendieck Constants and LHV Models in Quantum Mechanics
- Convex separation from convex optimization for large-scale problems
- New Bell inequalities for the singlet state: Going beyond the Grothendieck bound
- Shared randomness and device-independent dimension witnessing
- Can non-local correlations be discriminated in polynomial time?