Environmental decoherence is widely held to be the key to understanding the emergence of classicality in a quantum universe. However, in conjunction with traditional principles of interpretation, decoherence leaves unanswered a fundamental question, a version of the quantum measurement problem: Why should macroscopic objects have definite properties at all? I critically evaluate a variety of interpretive strategies intended to parlay the formal results of decoherence into the definiteness, or apparent definiteness, of familiar macroscopic properties. I argue that the crucial role of environmental decoherence in accounting for definite properties is effecting the dynamical decoupling of components of the global quantum state for which these properties are definite.This role of decoherence is most evident in the context of the Everett interpretation, where considerations regarding branch dynamics lead naturally to the conclusion that dynamical autonomy (non-interference) of branches is a restriction on any division of the global quantum state into branches. Environmental decoherence results in the requisite dynamical autonomy for branches in which familiar macroscopic observables are definite, thus providing a natural and principled way to identify an interpretation basis.The modal interpretation, with its property ascription rule based on the spectral decomposition of the reduced state, secures the right definite properties only in those cases in which it picks out properties that correspond almost exactly with the non-interfering components of the global quantum state. I argue that the non-interference of these components should be accorded interpretational significance in its own right; then the right properties can be specified without recourse to the distinctive property ascription rules of the modal interpretation.Finally, I criticize attempts of decoherence theorists to account for definite properties by appeal to effects of decoherence such as approximate diagonality of the reduced state and preservation of correlations with respect to a set of privileged states. I argue that definiteness can be accounted for by looking not to these effects but to their cause, the dynamical autonomy of the environmentally-privileged components of the global quantum state. Precisely because they are dynamically autonomous, these states can be accorded physical significance in their own right.
Environmental decoherence is widely held to be the key to understanding the emergence of classicality in a quantum universe. However, in conjunction with traditional principles of interpretation, decoherence leaves unanswered a fundamental question, a version of the quantum measurement problem: Why should macroscopic objects have definite properties at all? I critically evaluate a variety of interpretive strategies intended to parlay the formal results of decoherence into the definiteness, or apparent definiteness, of familiar macroscopic properties. I argue that the crucial role of environmental decoherence in accounting for definite properties is effecting the dynamical decoupling of components of the global quantum state for which these properties are definite.This role of decoherence is most evident in the context of the Everett interpretation, where considerations regarding branch dynamics lead naturally to the conclusion that dynamical autonomy (non-interference) of branches is a restriction on any division of the global quantum state into branches. Environmental decoherence results in the requisite dynamical autonomy for branches in which familiar macroscopic observables are definite, thus providing a natural and principled way to identify an interpretation basis.The modal interpretation, with its property ascription rule based on the spectral decomposition of the reduced state, secures the right definite properties only in those cases in which it picks out properties that correspond almost exactly with the non-interfering components of the global quantum state. I argue that the non-interference of these components should be accorded interpretational significance in its own right; then the right properties can be specified without recourse to the distinctive property ascription rules of the modal interpretation.Finally, I criticize attempts of decoherence theorists to account for definite properties by appeal to effects of decoherence such as approximate diagonality of the reduced state and preservation of correlations with respect to a set of privileged states. I argue that definiteness can be accounted for by looking not to these effects but to their cause, the dynamical autonomy of the environmentally-privileged components of the global quantum state. Precisely because they are dynamically autonomous, these states can be accorded physical significance in their own right.
Environmental decoherence is central to contemporary accounts of quantum measurement, yet its relation to definite outcomes remains disputed. This review distinguishes four explanatory demands: interference suppression, preferred-basis selection, operational objectivity, and outcome actualization. It compares open-system formalism and experimental evidence with the principal philosophical accounts of definiteness. In nonrelativistic models, environmental entanglement disperses phase coherence into inaccessible correlations, rendering the reduced system–apparatus state approximately diagonal in an interaction-selected pointer basis. Experiments support this loss of locally observable interference, while einselection and redundant environmental records explain the stability and intersubjective accessibility of macroscopic properties. These achievements neither convert an improper mixture into ignorance about an actual result nor select one component of the global state. Everettian interpretations reject global uniqueness, Bohmian mechanics adds an actual configuration, objective-collapse theories modify the dynamics, and QBist or pragmatist approaches revise quantum-state semantics. Decoherence is therefore indispensable to the formation of classical records but insufficient, by itself, for an interpretation-neutral derivation of unique actualization. Its foundational significance lies in identifying where unitary dynamical explanation ends and an ontological, dynamical, or semantic account of definiteness must begin.
The consistent histories formalism can be used to describe histories comprised of events across many systems, times, and places, plausibly rich enough to describe our experiences of the classical world; however, many consistent history sets are nonclassical and thus not obviously relevant to our experiences. Meanwhile, the program of environmentally induced decoherence identifies dynamically privileged classical degrees of freedom, but provides no general account of when or how many such degrees of freedom consistently combine to form histories. This work shows that the strengths of these two approaches can be combined by adopting a dynamics-first perspective on decoherence. Inspired by quantum causal models and quantum Darwinism, we define the process of decoherence in terms of the causal influences through unitary dynamics required for the proliferation of information about observables. We characterise decoherence as a property of the unitary dynamics, without presupposing the existence of any quantum state. Instead, we show that the state emerges from dual decoherence, related to decoherence by time-reversal of the unitary dynamics. Indeed, for any set of systems in an arbitrary unitary circuit, decoherence and its dual single out a privileged consistent history set -- and we demonstrate through examples that states emerge from dual decoherence while outcomes emerge from decoherence. Hence the idea that quantum states emerge from the process of decoherence turns out to be the key missing ingredient for unifying environmentally induced decoherence and consistent histories. Taking this idea ontologically seriously leads to a recently proposed causal interpretation of quantum theory or a dynamics-first version of the Everett interpretation. The causal approach also sheds light on the suppression of off-diagonal terms, time asymmetry, and robustness of the pointer basis.
This work is a critique of the program of "environment-induced decoherence" as advocated by Zurek, Zeh and Joos, among others. In particular, the alleged relevance of decoherence for a solution of the "measurement problem" is subjected to a detailed philosophical analysis. In the first chapter, an attempt is made to unravel what exactly this "measurement problem" amounts to for the decoherence theorists. The second chapter reviews the standard decoherence literature. The third chapter starts with a brief discussion of the philosophical implications of the decoherence program, followed by a non-standard reconstruction of the decoherence argument that aims to uncover some (mostly hidden) assumptions underlying the approach. It is argued that different subsets of these assumptions result in different versions of the decoherence argument. Next, these assumptions are investigated in more detail, and a number of open problems for the decoherence approach is formulated, in addition to the well-known "problem of outcomes". These problems concern the interpretational relevance of the preferred basis, the role and status of the ignorance interpretation of mixed states, imperfect decoherence and the role of the environment and the definition of subsystems. The fourth chapter addresses the question to what extent the embedding of decoherence in an Everett-like interpretational framework, such as Zurek's "existentional interpretation" and Wallace's structural-realistic version of the many-worlds interpretation, helps to resolve these problems. The main conclusions are formulated in the fifth chapter. Namely: 1) decoherence cannot address the "preferred-basis problem" without adding new interpretational axioms to the standard formalism, 2) the the locality principle (that says that the environment is the "irrelevant" part and should therefore be ignored) is not only problematic but also interpretationally superfluous, 3) the decoherence approach, when formulated in terms of the standard interpretation of quantum mechanics, is predicated on a solution of the "problem of outcomes" and thus cannot claim to account (even partially) for the latter, and 4) that the results of the decoherence program do not increase the plausibility of a realist interpretation of the quantum state.
The problem of measurement taken at face value shows clearly that there is an inconsistency inside the quantum formalism.The phenomenon of decoherence is often presented as a solution to it.A widely debated question is to decide between two different interpretations.The first one is to consider that the decoherence process has the effect to actually project a superposed state into one of its classically interpretable component, hence doing the same job as the reduction postulate.For the second one, decoherence is only a way to show why no macroscopic superposed state can be observed and so, to explain the classical appearance of the macroscopic world, while the quantum entanglement between the system, the apparatus and the environment never disappears.In this case, explaining why only one single definite outcome is observed remains to do.In this paper, we examine arguments for and against both interpretations and defend a position according to which the outcome that is observed is relative to the observer in close parallel to the Everett interpretation.
We investigate the conceptual relationship between decoherence and the origin of probabilistic outcomes in quantum mechanics. While decoherence theory successfully explains the suppression of interference and the emergence of classical behavior through interactions with environmental degrees of freedom, its role in providing a complete account of the probabilistic nature of quantum measurement remains limited. In this work, we argue that the suppression of interference and the origin of probabilistic outcomes constitute distinct problems that should be conceptually distinguished. By “probabilistic outcomes,” we refer to the appearance of statistical distributions in measurement results as described by the Born rule. To clarify this distinction, we analyze limiting scenarios, including isolated quantum systems and the universe treated as a closed system, where the standard decoherence mechanism becomes ineffective or inapplicable, yet probabilistic outcomes persist. These considerations are not intended as a formal proof, but rather as a means to isolate conceptual dependencies. We then revisit the Intrinsic Observability Framework (IOF), in which the Hilbert space is intrinsically decomposed into observable and hidden degrees of freedom. Within this framework, probabilistic descriptions arise from restricted access to the full quantum state, rather than from environmental interactions or dynamical processes. By contrasting decoherence with the IOF perspective, we argue that decoherence provides an account of the emergence of classicality, but does not directly address the origin of quantum probabilities. The IOF, on the other hand, offers a structural perspective at the level of pure states. This suggests that a complete understanding of quantum measurement requires recognizing the distinct roles played by these two elements.
Abstract This chapter argues for the view that the Everett (‘many worlds’) interpretation is nothing more or less than a literal reading of the formalism of unitary quantum mechanics. The central component of this story is decoherence: the process by which the evolution of the quantum state acquires a branching structure. The chapter gives a conceptual introduction to decoherence and its conceptual role, emphasizing the significance of its effects on the dynamics of degrees of freedom which are undergoing decoherence. It then argues that, although the branching structure generated by decoherence is ‘for all practical purposes’ in the sense that it is not part of the microscopic formalism of quantum theory, nonetheless it is a perfectly real, observer-independent feature of reality — it is emergent from that microscopic formalism in a way very familiar from many other parts of science.