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Bell's theorem
This chapter discusses the result which has come to be known as ‘Bell’s Theorem’ but which Bell himself instead referred to as the ‘locality inequality theorem’.
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Quantum equilibrium and the origin of absolute uncertainty
The quantum formalism is a “measurement” formalism-a phenomenological formalism describing certain macroscopic regularities. We argue that it can be regarded, and best be understood, as arising from…
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On the Common Structure of Bohmian Mechanics and the Ghirardi–Rimini–Weber Theory
Bohmian mechanics and the Ghirardi–Rimini–Weber theory provide opposite resolutions of the quantum measurement problem: the former postulates additional variables (the particle positions) besides the…
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What Is Bohmian Mechanics
TLDR
Bohmian mechanics is a quantum theory with a clear ontology and the status and the role of of the quantum formalism is clarified.
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Quantum physics without quantum philosophy
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Quantum Equilibrium and the Role of Operators as Observables in Quantum Theory
Bohmian mechanics is arguably the most naively obvious embedding imaginable of Schrödinger's equation into a completely coherent physical theory. It describes a world in which particles move in a…
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Canonical typicality.
TLDR
This work clarifies, expands, and justifies remarks made by Schrödinger in 1952, that a much stronger statement holds for quantum systems when the composite S + B is described by the microcanonical ensemble corresponding to a suitable energy shell.
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Hypersurface Bohm-Dirac models
Among the different approaches to resolving the conceptual problems of quantum theory, Bohm’s approach is perhaps the simplest.
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On the Role of Density Matrices in Bohmian Mechanics
It is well known that density matrices can be used in quantum mechanics to represent the information available to an observer about either a system with a random wave function (“statistical mixture”)…
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Can Bohmian mechanics be made relativistic?
TLDR
It is argued that the possibility that, instead of positing it as extra structure, the required foliation could be covariantly determined by the wave function allows for the formulation of Bohmian theories that seem to qualify as fundamentally Lorentz invariant.
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