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consistent histories

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consistent histories
NameConsistent histories
FieldQuantum mechanics, Quantum foundations
RelatedQuantum decoherence, Many-worlds interpretation, Copenhagen interpretation

consistent histories. The consistent histories approach, also known as the decoherent histories interpretation, is a framework for quantum mechanics that provides an interpretation of quantum theory without invoking a fundamental wave function collapse. It was developed in the 1980s by Robert B. Griffiths, and later expanded by Roland Omnès and Murray Gell-Mann with James Hartle. This formalism uses the standard mathematical tools of quantum theory, particularly density matrices and projection operators, to assign probabilities to sequences of quantum events, provided those sequences satisfy specific consistency conditions.

Introduction

The framework emerged from efforts to apply quantum mechanics to cosmology and the description of closed systems like the entire universe, where the traditional Copenhagen interpretation with its external observer is problematic. It seeks to answer questions about the history of a quantum system, such as whether a particle went through a specific slit in the double-slit experiment, by defining sets of possible histories. Pioneering work was done by Robert B. Griffiths in 1984, with significant contributions later from Roland Omnès and the collaboration between Murray Gell-Mann and James Hartle at the Santa Fe Institute. The approach is closely related to the concept of quantum decoherence, which explains the emergence of classicality.

Formulation

The formalism describes a system via its density matrix, typically the initial state. A history is defined as a time-ordered sequence of propositions, represented by projection operators acting at successive times, drawn from the Heisenberg picture. The central mathematical object is the decoherence functional, which assigns a complex number to any pair of histories. For a set of histories to be consistent (or decoherent), the off-diagonal elements of this functional must vanish, ensuring the probabilities for mutually exclusive histories add according to the rules of classical probability theory. This consistency condition allows one to use the Born rule to assign probabilities to individual histories within that set.

Interpretation and implications

In this interpretation, quantum mechanics is viewed as a generalized probability theory for histories. There is no single, predetermined history of the universe; instead, different consistent sets of histories provide equally valid but complementary descriptions of reality, a concept reminiscent of Niels Bohr's principle of complementarity. The framework does not require a distinct process of wave function collapse or the existence of an external observer, making it applicable to the early universe as studied in quantum cosmology. It shows a deep connection with the many-worlds interpretation, as decoherent histories can be seen as describing branches within a universal wave function, and it aligns with the Copenhagen interpretation in appropriate measurement situations.

Criticisms and controversies

A major criticism, notably advanced by David Mermin and others, is that the framework allows for multiple, incompatible consistent sets of histories, leading to questions about which set describes "real" events. This has been labeled the "set selection problem." Detractors argue this introduces a form of perspectivism that undermines objective reality. Furthermore, some physicists, like Anthony Leggett, have questioned whether the consistency conditions are too restrictive or too permissive in actual physical scenarios. Debates often center on the interpretation's ontological commitments and its empirical equivalence to other interpretations like the many-worlds interpretation or Bohmian mechanics.

Applications and examples

Beyond foundational discussions, the formalism has been applied to practical problems in quantum chaos, the study of emergent classical mechanics from quantum theory, and quantum cosmology at the Planck scale. It is used to analyze the transition from quantum to classical behavior in systems like a particle undergoing Brownian motion or the origin of cosmic microwave background anisotropies in the early universe. The approach also provides tools for analyzing measurement processes in quantum optics and the dynamics of open quantum systems in fields like condensed matter physics.

Category:Interpretations of quantum mechanics Category:Quantum measurement Category:Quantum foundations