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Its implications, however, reach algebraic geometry, representation theory, and even parts of theoretical physics. If you truly want to actually understand Tannaka duality, Isbell conjugation, or Grothendieck’s schemes, then you don’t get terribly far without Yoneda. But how can chasing idₐ be this impactful? The “Yoneda perspective,” that objects are their relations, is forced on you by the math. (2/22)
It's a hangover from misinterpreting wave functions in 3D space when they really live in something else called "configuration space." It confuses a calculational trick with physical ontology. Time for some rigor. \int D\phi, e^{iS[\phi]/\hbar People love to say that particles explore every possible path simultaneously—even going back in time or to the moon. Firstly, what is this word “possible”? Possible isn't a physics word. Do you mean to say every continuous path in R^4? Every once differentiable path in R^3? What is it? (2/20)
Most likely, your GR instructor glossed over energy, perhaps mumbled something about “pseudo-tensors” under their breath, then quickly changed the subject. Why the rush? Why the evasion on such a supposedly fundamental concept? The full, honest treatment is extremely messy, deeply controversial, and fundamentally unresolved even after a century. Einstein himself wrestled with it, and the compromises he made are still debated today. Let’s talk about that mess. (2/20)
Firstly, epistemology is just fancy technical jargon for "what and how we can know." So, knowledge. Questions in the field of epistemology are questions that deal with the nature, sources, and limits of knowledge. The "nature" of this knowledge even includes defining what knowledge is (see Gettier's problem), but this is beside the point. 2/
Firstly, note that entropy is NOT a measure of disorder… It's a way you count states. From this, we'll see that geometry *is* entropy, and entropy *is* geometry. Let's start with classical mechanics... (2/19)
Here's the core idea, stripped of the (intimidating) math. Imagine you're in a completely dark room. You can't *see* anything, but you still have expectations. You *predict* where the walls are, where the furniture might be. Now you see that your brain doesn't merely receive but *infers*. This is the difference between passivity and activity. 2/13
When a function maps elements from one set to another, Lawvere showed that if you have a "nice" function (technically, a "fixed point operator") that can map elements from a set of functions to another set, you'll *always* find a fixed point (an element that maps to itself). Importantly, we don't assume the existence of this operator. We *derive* it. That's the power of this theorem. 2/13
Most people think of quantum mechanics as being about wave functions. What if Ψ isn't' fundamental? What if it's just a mathematical convenience? What happens to the associated devices like Hilbert spaces and state vectors? To Jacob, sure, they're useful, but they're not "real."
First, what's a “model”? In a formal theory, it's a set of axioms and rules (actually it's what “satisfies” those). Examples would be set theory or arithmetic. A “model” for that theory is like a mathematical world (technically called by model-theorists a “Universe,” interestingly enough) where all those axioms and rules are true. Some say it's like an interpretation, but I'd say it's more like what's being “referred to.” So, if you have a theory that says, “There exists an infinite set,” a model for that theory would be a mathematical structure that contains an infinite set. Super simple so far. (2/10)
Usually people say phase space (incorrectly) when they actually mean “state space” so lets' define this phase space. It's an abstract space (not spacetime) where each point represents a particle's state is given by its position (q) and momentum (p). So, phase space is a space of (q, p) pairs. You can extend this to N particles, of course. (2/10)
It all starts w/ symplectic geometry. Think of a classical phase space, but forget coordinates for the moment. What you require is something called a symplectic form -- a closed, non-degenerate 2-form, ω... (2/7)