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I examine some problems standing in the way of a successful `field interpretation' of quantum field theory. The most popular extant proposal depends on the Hilbert space of `wavefunctionals.' But since wavefunctional space is unitarily equivalent to many-particle Fock space, two of the most powerful arguments against particle interpretations also undermine this form of field interpretation. 1. Introduction 2. Field Interpretations and Field Operators 3. The Wavefunctional Interpretation 4. Fields and Inequivalent Representations 4.1. The Rindler representation 4.2. Spontaneous symmetry breaking 4.3. Coherent representations 5. The Fate of Fields in Interacting QFT 6. Conclusions
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David J. Baker (2009) studied this question.
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