Reverse Physics for GR Gabriele Carcassi and

Published  . 0 views
↓ Download
Reverse Physics for GR Gabriele Carcassi and
1 / 1
Reverse Physics for GR Gabriele Carcassi and - slide 1 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 2 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 3 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 4 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 5 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 6 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 7 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 8 of 9 Reverse Physics for GR Gabriele Carcassi and - slide 9 of 9
Description: Reverse Physics for GR Gabriele Carcassi and Christine A. Aidala Physics Department University of Michigan Reverse Physics: from laws to physical assumptions, Found Phys 52, 40 (2022) Area within each DOF Scalar product across DOFs

Related Topics

Download Presentation

"Reverse Physics for GR Gabriele Carcassi and" is the property of its rightful owner. Permission is granted to download and print the materials on this website for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.

Presentation Transcript

slide1. Reverse Physics for GR Gabriele Carcassi and Christine A. Aidala
Physics Department University of Michigan Reverse Physics: from laws to physical assumptions,
Found Phys 52, 40 (2022)<br>
slide2. Area within each DOF Scalar product across DOFs Hamiltonian is the continuous version of Recovers relativistic particle mechanics without additional assumptions Assumptions of Physics, Michigan Publishing (v2 2023)<br>
slide3. Geometry of principle of least action (SDOF) The action is the line integral of the vector potential (unphysical) No state is “lost” or “created” as time evolves (Minus sign to match convention) DR KE Sci Rep 13, 12138 (2023)<br>
slide4. Counting states and configurations Discrete case<br>
slide5. Flow of states Line integral of the vector potential of the flow of state density? #DOFs? Flow of configurations? Flow of DOFs? We are mapping values between Cauchy surfaces, #DOFs are the points on the Cauchy surface, #conf are the possible field values at each point<br>
slide6. The problem with counting on the continuum Pick two! We’d like: Incompatible! Non-orthogonal states: different states but in different contexts Orthogonal states: different states all else equal additive sub-additive<br>
slide7. #conf=#DOFs Lower bound on this… …requires a lower bound on this Same problem! Distant points: independent DOFs Close points: DOFs not independent additive sub-additive From QM: Lower bound on state count requires a severe revisitation of particle state space Does lower bound on DOF count require an equally severe revisitation of space-time?<br>
slide8. Wrapping up Classical mechanics is exactly det/rev mapping of configurations over finitely many DOFs
Conjecture: is general relativity exactly det/rev mapping of configurations over infinitely many (dense) DOFs (i.e. a field theory)?
Quantum mechanics sets a lower bound on state count
Entropy of pure state is zero, pure states count as one state
Conjecture: is quantum gravity setting a lower bound on the DOF count?
No region of space can contain less than one DOF

Can we generalize the physical/geometric interpretation of the action principle to field theory and to QM?<br>