01 January 1970 19 6K Report

First of all, we must concede the "variability" of space-time, and it's a physical reality. First, this is the common ground of both the Special and General Theory of Relativity; the main body of relativity can be trusted to be correct and has been more than adequately verified by experiments. These experiments typically include the earliest light-bending experiments [Eddington 1919], the round-the-world flight experiments [1], the GPS clock-correction experiments [2], and later the LIGO gravitational-wave-detection experiments [3], the observation of gravitational lensing phenomena [4] [5], and so on. The meaning of "variable" is not necessarily the relative spacetime of SR or the curved spacetime of GR. Second, philosophically we should also recognize that spacetime will not be just a variable background for matter, since all interactions cannot be separated from spacetime. Spacetime is not just a distance scale but should take on the function of transmitting interactions.

What our teachers emphasized when they talked about the difference between the applicability of SR and GR is that SR is an event in flat spacetime and GR is an event in curved spacetime. But there is only one spacetime, and for a moving electron, its SR spacetime and GR spacetime would have to be the same** if we had to consider both its SR and GR effects*.

Einstein's fondness for the concept of curved spacetime may have arisen from the intuitive nature of the geodesic concept, or perhaps from the affirmation of the maximal nature of spacetime dynamics. In any case, GR's expression of gravity in terms of a curved spacetime concept was already orthodox, though beyond the empirical perception of all. Feynman constantly questioned the notion of "spacetime curvature" and used the concept of a " measure " of spacetime in general relativity instead of "curvature" [6]. Weinberg thought that geometry might be more appropriately viewed as an analog of GR, politely expressing his skepticism, and L. Susskind, when teaching GR, said that no one knows what four-dimensional spacetime bending looks like†. We believe that Einstein was also not a great believer in the notion of four-dimensional spacetime bending, and his subsequent repeated turn to the study of five-dimensional spacetime[7][8] does not appear to have been solely for the sake of gravitational unification with Maxwell's electromagnetic theory, but perhaps also as a passing attempt to find a dimension for the three-dimensional sphere into which it could be embedded‡.

All of our current measurements and verifications of SR and GR spacetime do not involve true spacetime "curvature", although there are many proposed methods [9]. The LIGO gravitational wave measurements, the gravitational redshift and violetshift, can only be considered as a response to changes in the spacetime metric. This is similar to Feynman's view.

Let us assume a scenario: an electron of mass m in four-dimensional spacetime, and a stationary observer in a fifth-dimensional abstract space, who keeps changing the direction and velocity of the motion of the electron in four-dimensional spacetime through the fifth dimension. Ask, in the opinion of this observer:

1) Do SR spacetime and GR spacetime have to be identical?

2) Is it possible to fully express spacetime "curvature" with a spacetime metric? Excluding " twisting ".

3) Is there a notion of "curvature" for the "curvature" of one-dimensional time? Usually in GR it is also said to be the gravitational time dilation [10]. The curvature of one-dimensional space can have the concept of curvature, but in which direction? How can it not interfere with the other two dimensions?

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Notes:

* Usually physics recognizes that GR effects are ignored because the electron mass is so small. This realization masks great problems. We are extrapolating from macroscopic manifestations to microscopic manifestations, and from manifestations abstracted as point particles at a distance to manifestations when structure exists at close range. As long as structure exists, when distance is sufficiently small, everything behaves as a distributed field. At this point, the abstract notion of force (magnitude, direction, point of action) has disappeared. For electrons, even the concept of charge disappears. Yet the concept of gravity does not necessarily disappear at this point, thus causing a reversal of the order of magnitude difference in action at very close distances.

** There is a difference between this and the state of affairs during GPS clock calibration. When doing GPS calibration, we are using the ground as the reference frame. A flying satellite in the sky has an SR effect, but we approximate it to be flat in space-time. The GR effect, on the other hand, is relative to the ground, not of itself. Thus, the composite calibration is the difference between the two. If one were to change the scenario and the relatively immobile space station if it needed to be calibrated with the clock of some sort of vehicle on the ground moving at high speed around it, then the composite calibration would be the sum of the two. Please correct me if there are problems with this scenario.

† He also said, when teaching QM, that no one knows what the top and bottom spins of the electron are.

‡ Einstein says that the universe is a finite three-dimensional sphere.

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References:

[1] Hafele, J. C. and R. E. Keating (1972). "Around-the-World Atomic Clocks: Observed Relativistic Time Gains." Science 177(4044): 168-170.

[2] "Relativity in GNSS"; Ashtekar, A. and V. Petkov (2014). Springer Handbook of Spacetime. Berlin, Heidelberg, Springer Berlin Heidelberg.

[3] Cahillane, C. and G. Mansell (2022). "Review of the Advanced LIGO gravitational wave observatories leading to observing run four." Galaxies 10(1): 36.

[4] https://hubblesite.org/contents/articles/gravitational-lensing;

[5] Tran, K.-V. H., A. Harshan, K. Glazebrook, G. K. Vasan, T. Jones, C. Jacobs, G. G. Kacprzak, T. M. Barone, T. E. Collett and A. Gupta (2022). "The AGEL Survey: Spectroscopic Confirmation of Strong Gravitational Lenses in the DES and DECaLS Fields Selected Using Convolutional Neural Networks." The Astronomical Journal 164(4): 148.

[6] Feynman, R. P. (2005). The Feynman Lectures on Physics(II).

[7] Pais, A. (1983). The science and the life of Albert Einstein II Oxford university press.

[8] Weinberg, S. (2005). "Einstein’s Mistakes." Physics Today 58(11).

[9] Ciufolini, I. and M. Demianski (1986). "How to measure the curvature of space-time." Physical Review D 34(4): 1018.

[10] Roura, A. (2022). "Quantum probe of space-time curvature." Science 375(6577): 142-143.

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