consider. The quantum theory (QT) and new stochastic approaches have no deterministic prediction for a hit measurement or for a hit measure -series of events observed for a trapped ion electron or any other individual physical system. The predictions of QT being of probabilistic engrave apply to the statistical distribution of the results obtained in various experiments. The probability distribution is not an evaluate of a cut but it is a characteristic of a whole random experiment : " rolling a dice" and statistical long range correlations between two random variables X and Y are not a proof of any causal relation between these variable. Moreover any probabilistic copy used to exposit a random investigate is consistent only with a specific protocol telling how the random experiment has to be performed. In this sense the quantum theory is a statistical and contextual theory of phenomena. In this paper we discuss these important topics in some dilate. Besides we discuss in historical perspective various prerequisites used in the proofs of attach and CHSH inequalities concluding that the violation of these inequalities in go around polarization correlation experiments is neither a create of the completeness of QT nor of its nonlocality. The question whether QT is predictably complete is comfort open and it should be answered by a careful and unconventional analysis of the experimental data. It is sufficient to analyze more in detail the existing experimental data by using various non-parametric purity tests and other specific statistical tools invented to study the fine structure of the time-series. The change by reversal understanding of statistical and contextual character of QT has far reaching consequences for the quantum information and quantum computing.
mention. 16 pages. 59 references,the contribution to the conference QTRF-4 held in Vaxjo. Sweden. 11-16 june 2007. To be published in the Proceedings
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http://eprintweb.org/S/article/quant-ph/0710.3510
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