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This is one little studied route towards a [[TOE]], not taking the relativistic option in the $cGh$ cube of [[physics]]. This might be worthwhile because relativity might bring distracting complications, not at the heart of everything that matters (e.g., dualities, nonlocal entanglement, etc.) | This is one little studied route towards a [[TOE]], not taking the relativistic option in the $cGh$ cube of [[physics]]. This might be worthwhile because relativity might bring distracting complications, not at the heart of everything that matters (e.g., dualities, nonlocal entanglement, etc.) | ||
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+ | A particular and concrete approach is that of the Newton-Schrödinger equation [https://en.wikipedia.org/wiki/Schr%C3%B6dinger%E2%80%93Newton_equation][https://iopscience.iop.org/article/10.1088/1367-2630/16/11/115007], which {{I}} actually use to label the $cGh$ cube although it is one aspect only of this corner. | ||
== Links == | == Links == |
This is one little studied route towards a TOE, not taking the relativistic option in the $cGh$ cube of physics. This might be worthwhile because relativity might bring distracting complications, not at the heart of everything that matters (e.g., dualities, nonlocal entanglement, etc.)
A particular and concrete approach is that of the Newton-Schrödinger equation [1][2], which I actually use to label the $cGh$ cube although it is one aspect only of this corner.
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