It may be that in quantum reality radioactive decay may be perfectly regular and predictable (maybe all such events are even simultaneous.) In mathematics it is easy to create a function with a regular input but a seemingly random output. — EnPassant
In mathematics it is easy to create a function with a regular input but a seemingly random output. — EnPassant
I'm not sure what you mean by everything happening simultaneous. If such were the case there would be no cause and effect? — boethius
Well, that was a throwaway comment. What I mean is anything could be the case for all we know. — EnPassant
Space is two things. It is an ontological reality and a geometric reality. Ontologically space is there. It is not nothingness, it is a substance. But space as geometry seems to be more accessible to science. — EnPassant
We don't see particles, we only see trace effects. A spot on a photographic plate is a trace effect, not a particle! What is important here is to see the both the detection apparatus and the trace effect are macroscopic, classical objects; they both exist in classical spacetime. This means that the trace effect is necessarily a classical object, obviously located in classical spacetime. But where is the particle before/after detection? Nowhere. Nowhere in classical spacetime that is. This is why Bohr says it is meaningless to say where it is. It is 'elsewhere'. — EnPassant
If there is a light source at A and a photographic plate at B and a photon is detected it is natural to assume that the photon traveled in a straight line from A to B. But, strictly speaking, all we can say is that the photon left a trace effect at A and a trace effect at B. — EnPassant
If the photon is not really travelling in a straight line (because it is not even in classical spacetime) the straight line must be seen as an artefact of the experimental apparatus itself. This is because the whole experiment is taking place on 'this side' of the interface between these two spacetimes. Consequently any relationship between trace effects must be in terms of a classical 4-D geometry. That is, the positions of particles (in reality trace effects) is imposed on the situation because the experimental apparatus, being a classical object in classical spacetime, can do nothing else but force things into a classical geometry. — EnPassant
Our apparatus is definitely classical, but it's a fairly radical direction to claim our apparatus imposes anything on the quantum realm ... as this seems to imply the apparatus exists first. — boethius
The crux of my idea is that there are two distinct spacetimes (quantum and classical) made manifest by ontological space. These spacetimes exist 'here' in our ontological space but because they are different geometries they are, from a geometric perspective, two different spacetimes. — EnPassant
The position that there is not any randomness in a Newtonian sense, is called "hidden variables theories", but you can imagine that there's just small "springs and gear mechanisms" everywhere (that we can't observe) that fully determining how every event turns out; the internal states of these tiny mechanisms are the hidden variables. — boethius
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