Abstract

Quantum physics can only make statistical predictions about possible measurement outcomes, and these predictions originate from an operator algebra that is fundamentally different from the conventional definition of probability as a subjective lack of information regarding the physical reality of the system. In the present paper, I explore how the operator formalism accommodates the vast number of possible states and measurements by characterizing its essential function as a description of causality relations between initial conditions and subsequent observations. It is shown that any complete description of causality must involve non-positive statistical elements that cannot be associated with any directly observable effects. The necessity of non-positive elements is demonstrated by the uniquely defined mathematical description of ideal correlations which explains the physics of maximally entangled states, quantum teleportation and quantum cloning. The operator formalism thus modifies the concept of causality by providing a universally valid description of deterministic relations between initial states and subsequent observations that cannot be expressed in terms of directly observable measurement outcomes. Instead, the identifiable elements of causality are necessarily non-positive and hence unobservable. The validity of the operator algebra therefore indicates that a consistent explanation of the various uncertainty limited phenomena associated with physical objects is only possible if we learn to accept the fact that the elements of causality cannot be reconciled with a continuation of observable reality in the physical object.

Highlights

  • Perhaps the greatest puzzle of quantum theory is the fact that it does not provide us with any feasible model of physical reality, even though it allows us to describe a vast number of possible experimental scenarios and does provide us with accurate predictions of the statistics obtained from their outcomes

  • As we can see from the analysis presented above, the bounds of quantum statistics are related to the non-positivity in any complete description of the operator algebra

  • Operator expansions can provide a deeper insight into the difference between quantum statistics and classical statistics

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Summary

Introduction

Perhaps the greatest puzzle of quantum theory is the fact that it does not provide us with any feasible model of physical reality, even though it allows us to describe a vast number of possible experimental scenarios and does provide us with accurate predictions of the statistics obtained from their outcomes. The quantum formalism provides an alternative representation of statistics that appears to change from situation to situation, making a non-contextual description of measurement outcomes impossible This irreducible contextuality of quantum statistics has been enshrined in the form of the uncertainty principle, where it describes the relation between physical properties that have no observable joint reality. The formalism defines “elements of causality” that provide an alternative description of perfectly deterministic relations between state preparation and measurement These elements are fundamentally unobservable because they represent non-positive contributions to the statistics. Optimal quantum cloning is characterized by a well-defined contribution that represents an ideal copy of an arbitrary input All of these phenomena support the idea that complete operator expansions represent a universal description of causality in quantum physics, with the elements of any complete and orthogonal expansion serving as deterministic elements of causality. The universal causality relations that explain all of the possible phenomena associated with a physical object are necessarily expressed in terms of non-positive elements that need to be understood in relation to the uncertainty limits that apply to the possible external controls by means of which the physical object is manipulated and observed

A Compact Theory of Quantum Statistics
Precise Measurements
Tomographic Reconstructions
Statistical Moments and Quasi-Probabilities
Entanglement and Teleportation
Optimal Cloning and Ideal Copies
Elements of Causality
Conclusions
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