01 January 1970 13 3K Report

Gravitational waves are ripples of spacetime propagating at the speed of light [1]. A gravitational wave can be described as a small perturbation hμν on a flat spacetime metric ημν [2]:

gμν = ημν + hμν ....... (Eq.1)

1) Cosmological observations prove that the speed of gravitational waves and the speed of light are identical [3]. In the absence of any third party or any law constraints, if the speeds of gravitational waves and light are exactly the same, they cannot be independently unrelated to each other, so what should be the relationship between them?

2) "The energy associated with gravitational waves is a second-order effect, and so its justification goes beyond the linearised approximation considered so far. ...... Aside from energy, GWs may also carry angular momentum and linear momentum" [1]. Gravitational waves undoubtedly contain energy, and when it travels at the speed of light, it means that the energy spreads at the speed of light and that there is momentum, not that there may be momentum. It does not make sense that energy travelling at the speed of light is not light and is not directly related to light. Light itself contains defined energy and momentum, why wouldn't a gravitational wave contain both defined energy and momentum? How is it best defined if its energy and momentum are defined with only the spacetime parameter?

3) We usually interpret gravity as a geometrical effect of spacetime, and also as an exchange of "gravitons", what is the relationship between these two interpretations, and are gravitons embodied by spacetime parameters? Is there local gravity inside a gravitational wave? What is its relation to the "graviton"?

4) One can think of hμν as the coefficients of the spacetime metrics , which, if combined, can express this ripple wave packet in terms of the variable metrics (there is a Locked Relationship between the space and time metrics). Then, in such a spacetime, let us assume that there is a light that is fully accompanied by gravitational wave propagation, i.e. they have a common source:

4.1) How do we define the speed of propagation of light when light itself is in ? Defined as c=Δs' /Δt', Δs' = √(Δx'2 + Δy'2 + Δz'2), it means that light is a synchronised ripple like gravitational waves.

4.2) How do we define the speed of gravitational waves themselves? Gravitational waves are the propagation speed of their own spacetime fluctuations . That is, how do we define the speed of propagation of this ? How much distance Δs it travelled in what time Δt?

4.3) LIGO directly measures the length contraction of space, not "bending". "Gravitational waves change the metric describing the spacetime between two freely falling test masses" [1]. "strain-to-length relation used in GW detection based on Michelson interferometers is h+=ΔL/L" [2]; if we consider the geometrical nature of Space-Time Curvature. Can we design a direct measurement of Space-Time Curvature?

4.4)“If light waves are stretched by gravitational waves, how can we use light as a ruler to detect gravitational waves?” This is explained in the literature [4]; is it sufficiently rational?

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Refererncs

[1] Bambi, C., Katsanevas, S., & Kokkotas, K. D. (2022). Handbook of Gravitational Wave Astronomy. Springer Nature.

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

[3] Abbott, B. P., Abbott, R., Abbott, T., Acernese, F., & etal. (2017). Gravitational waves and gamma-rays from a binary neutron star merger: GW170817 and GRB 170817A. The Astrophysical Journal Letters, 848(2), L13.

[4] Saulson, P. R. (1997). If light waves are stretched by gravitational waves, how can we use light as a ruler to detect gravitational waves? American Journal of Physics, 65(6), 501-505.

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