Submitted:
21 September 2023
Posted:
22 September 2023
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Abstract
Keywords:
1. Introduction
2. Physics Lingo: A Language for Cosmic Dialogue
- (i)
- Tangent vectors: rather than writing for the tangent vector at , which is an element of the tangent space , we write where the empty space within square brackets is a substitute for X, the dot downstairs is a substitute for the point p, and the arrow upstairs distinguishes a vector from its dual concept of 1-form or covector. We are therefore introducing a substitution map
- (ii)
- Vector fields: in this case, our substitution map acts according to
- (iii)
- 1-forms: we require thatwhere the arrow downstairs denotes the concept dual to the one in item (i).
- (iv)
- 1-form fields: we writewhere the dot has disappeared, as is the case in Equation (2), since we are dealing with a smooth assignment of 1-form as the point p is varying on the manifold M.
- (v)
- Tensor fields: a tensor field of type takes the formand, in particular, the Riemann curvature tensor, which is of type , can be denoted by
- (vi)
- The spacetime manifold , one of the great achievements of Einstein, can be expressed in the form
- (vii)
-
Vacuum Maxwell theory in curved spacetime can be described by the potential 1-form field A, its gauge curvature 2-form field , and the Hertz [1,2] 2-form P such thatThe simple but non-trivial tripletcan be represented in the formwhich, for the educated reader relevant for the CETI program, is enough for him/her to understand that this is a shorthand notation for the content of Equation (8).
- (viii)
- Tensor affinities are unfortunately denoted in the literature in the same way as tensor components, even though they do not transform in a homogeneous way under diffeomorphisms. Within our concise language, we propose instead to denote them in the formThe educated reader should understand that the resulting objects resemble tensor components, but do not transform tensorially under diffeomorphisms. Only arrows are appropriate for visual description of tensorial behaviour.
3. Some Peculiar Features of Interstellar Communication
4. Encoding and Transmitting Physics Words
4.1. Signal Modulation
4.2. Generality of the Approach
5. Concluding Remarks
- (i)
- We have first proposed a concise notation for describing some basic geometric concepts used in modern physical theories [18].
- (ii)
- We have then shown in detail how to obtain bit encoding for the images in Equations (1)–(7) and (9), which might be exploited for interstellar communication, since the resulting synthesis skills might attract the attention of advanced civilizations which receive signals sent from the Earth. On reflection, even the skeptical reader might appreciate that the unification of space and time as depicted in the sixth image of Figure 3, the electromagnetic theory depicted in the seventh image therein, and the Riemann curvature represented in the eighth image, deserve careful consideration.
Author Contributions
Funding
Conflicts of Interest
References
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