×
Well done. You've clicked the tower. This would actually achieve something if you had logged in first. Use the key for that. The name takes you home. This is where all the applicables sit. And you can't apply any changes to my site unless you are logged in.

Our policy is best summarized as "we don't care about _you_, we care about _them_", no emails, so no forgetting your password. You have no rights. It's like you don't even exist. If you publish material, I reserve the right to remove it, or use it myself.

Don't impersonate. Don't name someone involuntarily. You can lose everything if you cross the line, and no, I won't cancel your automatic payments first, so you'll have to do it the hard way. See how serious this sounds? That's how serious you're meant to take these.

×
Register


Required. 150 characters or fewer. Letters, digits and @/./+/-/_ only.
  • Your password can’t be too similar to your other personal information.
  • Your password must contain at least 8 characters.
  • Your password can’t be a commonly used password.
  • Your password can’t be entirely numeric.

Enter the same password as before, for verification.
Login

Grow A Dic
Define A Word
Make Space
Set Task
Mark Post
Apply Votestyle
Create Votes
(From: saved spaces)
Exclude Votes
Apply Dic
Exclude Dic

Click here to flash read.

arXiv:2404.17798v2 Announce Type: replace
Abstract: In Hermann Minkowski's pioneering formulation of special relativity, the space-time geometry in any inertial frame is described by the line-element $ds^2= \eta_{\mu \nu} dx^\mu dx^\nu$. It is interesting to note that not only the Minkowski metric $\eta_{\mu \nu} $ is invariant under proper Lorentz transformations, the totally antisymmetric Levi-Civita tensor $e_{\mu \nu \alpha \beta} $ too is. In general relativity (GR), $\eta_{\mu \nu} $ of the flat space-time gets generalized to a dynamical, space-time dependent metric tensor $ g_{\mu \nu} $ that characterizes a curved space-time geometry. In the present study, it is put forward that the flat space-time Levi-Civita tensor gets elevated to a dynamical four-form field $\tilde {w} $ in curved space-time manifolds, i.e. $e_{\mu \nu \alpha \beta} \rightarrow w_{\mu \nu \alpha \beta} (x) = \phi (x) \ e_{\mu \nu \alpha \beta} $ so that $\tilde {w} = {1\over {4!}} \ w_{\mu \nu \rho \sigma} \ \tilde{d} x^\mu \wedge \tilde{d} x^\nu \wedge \tilde{d} x^\rho \wedge \tilde{d} x^\sigma$. It is shown that this geometrodynamical four-form field, extends GR by leading naturally to a torsion in the theory as well as to a Chern-Simons gravity. In order to subject the hypothesized four-form field $\tilde {w}$ to observational evidence, we first argue that the associated scalar-density $\phi (x)$ corresponds to an axion-like pseudo-scalar field in the Minkowski space-time, and that it can also masquerade as dark matter. Thereafter, we provide a simple semi-classical analysis in which a self-gravitating Bose-Einstein condensate of such ultra-light pseudo-scalars leads to the formation of a supermassive black hole.

Click here to read this post out
ID: 844607; Unique Viewers: 0
Unique Voters: 0
Total Votes: 0
Votes:
Latest Change: May 9, 2024, 7:32 a.m. Changes:
Dictionaries:
Words:
Spaces:
Views: 8
CC:
No creative common's license
Comments: