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- Jill North (2009). The “Structure” of Physics. The Journal of Philosophy 106 (2):57-88.We are used to talking about the “structure” posited by a given theory of physics. We say that relativity is a theory about spacetime structure. Special relativity posits one spacetime structure; different models of general relativity posit different spacetime structures. We also talk of the “existence” of these structures. Special relativity says the world’s spacetime structure is Minkowskian: it posits that this spacetime structure exists. Understanding structure in this sense seems important for understanding what physics is telling us about the world. But it is not immediately obvious just what this structure is, or what we mean by the existence of one structure, rather than another. The idea of mathematical structure is relatively straightforward. There is geometric structure, topological structure, algebraic structure, and so forth. Mathematical structure tells us how abstract mathematical objects t together to form different types of mathematical spaces. Insofar as we understand mathematical objects, we can understand mathematical structure. Of course, what to say about the nature of mathematical objects isn’t easy. But there seems to be no further problem for understanding mathematical structure. Modern theories of physics are formulated in terms of these mathematical structures. In order to understand “structure” as used in physics, then, it seems we must simply look at the structure of the mathematics that is used to state the physics. But it is not that simple. Physics is supposed to be telling us about the nature of the world. If our physical theories are formulated in mathematical language, using mathematical objects, then this mathematics is somehow telling us about the physical make-up of the world. What is..
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I suggest that we use this rule for more than just spacetime structure. We should also posit the least statespace structure required by the fundamental dynamical laws. This rule yields surprising conclusions. Applied to classical mechanics, it suggests that a world governed by the theory has less fundamental structure than we ordinarily think. For the theory’s statespace imparts less structure to a world’s physical space than we ordinarily think.
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How do we learn about the nature of the world from the mathematical formulation of a physical theory? One rule we follow, familiar from spacetime theorizing: posit the least amount of spacetime structure required by the fundamental dynamical laws. I think that we should extend this rule beyond spacetime structure. We should extend the rule to statespace structure. Using this rule, I argue that a classical mechanical world has a surprisingly spare amount of structure.
How do we learn about the fundamental nature of the world from a mathematically formulated physical theory? To learn about spacetime, we follow this rule: posit the least spacetime structure to the world required by a theory’s dynamical laws. Applied to special relativity, for example, this rule tells us to not posit an absolute simultaneity structure. I suggest that we should use this rule for more than just spacetime structure. We should use the rule for statespace, positing the least statespace structure required by a theory’s dynamical laws. Using this rule, I argue that a classical mechanical world has surprisingly little fundamental structure. Fundamentally, such a world does not have a Euclidean distance structure. This bears on more general questions: what physics tells us about the world; what possibilities are distinguished by a theory; what is in a theory’s fundamental ontology (which I suggest includes the statespace structure); and when two formulations of a theory are mere notational variants.
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