I Einstein Hilbert action

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    Einstein Hilbert
Das apashanka
My question is why is the lagrangian density term in the action is equal to ricci scaler for gravitational field
 
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See e.g. Carroll's notes: it's the simplest scalar which contains up to second order derivatives of the metric. But maybe 'why' is the wrong question. We don't know 'why'. But it works.
 
It might be mentioned in this context that many theories of modified gravity instead put a general function ##f(R)##. Of course, to recover GR you need ##f(R) \simeq R## to leading approximation.
 
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So, to calculate a proper time of a worldline in SR using an inertial frame is quite easy. But I struggled a bit using a "rotating frame metric" and now I'm not sure whether I'll do it right. Couls someone point me in the right direction? "What have you tried?" Well, trying to help truly absolute layppl with some variation of a "Circular Twin Paradox" not using an inertial frame of reference for whatevere reason. I thought it would be a bit of a challenge so I made a derivation or...

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