Testing how different levels of entanglement affect predictability in practical setups
Autor: | M. Agüero, Myriam Nonaka, Marcelo G. Kovalsky, Alejandro A. Hnilo |
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Rok vydání: | 2021 |
Předmět: |
Hurst exponent
Kolmogorov complexity Series (mathematics) Dimension (graph theory) Statistical and Nonlinear Physics Quantum entanglement 01 natural sciences 010305 fluids & plasmas Theoretical Computer Science Electronic Optical and Magnetic Materials Photon entanglement Modeling and Simulation 0103 physical sciences Signal Processing Statistical physics Electrical and Electronic Engineering 010306 general physics Randomness Statistical hypothesis testing Mathematics |
Zdroj: | Quantum Information Processing. 20 |
ISSN: | 1573-1332 1570-0755 |
DOI: | 10.1007/s11128-021-03110-3 |
Popis: | The generation of series of random numbers is an important and difficult problem. Appropriate measurements on entangled states have been proposed as the definitive solution. In principle, this solution requires reaching the challenging “loophole-free” condition, which is unattainable in a practical situation nowadays. Yet, it is intuitive that randomness should gradually deteriorate as the setup deviates from that ideal condition. In order to test whether this trend exists or not, we prepare biphotons with three different levels of entanglement: moderately entangled ( $$S = 2.67$$ ), marginally entangled ( $$S = 2.06$$ ), and non-entangled ( $$S = 1.42$$ ) in a setup that mimics a practical situation. The indicators of randomness we use here are: a battery of standard statistical tests, Hurst exponent, an evaluator of Kolmogorov complexity, Takens’ dimension of embedding, and augmented Dickey–Fuller and Kwiatkowski–Phillips–Schmidt–Shin to check stationarity. A nonparametrical statistical ANOVA (Kruskal–Wallis) analysis reveals a strong influence of the level of entanglement with randomness when measured with Kolmogorov complexity in three time series with P-values and strength factor $$\epsilon ^2$$ : $$P = 0.0015$$ , $$\epsilon ^2 = 0.28$$ ; $$P = 4.5\times 10^{-4}$$ , $$\epsilon ^2 = 0.67$$ and $$P = 5.6\times 10^{-4}$$ , $$\epsilon ^2 = 0.16$$ . The setup is pulsed with time stamping, what allows generate different series applying different methods with the same data, even after the experimental run has ended, and to compare their raw randomness. It also allows the stroboscopic reconstruction of time variation of entanglement. |
Databáze: | OpenAIRE |
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