Contracting Riemann tensor with itself

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In Padmanabhan's "Gravitation: Foundations and Frontiers," the author attempts to demonstrate that the horizon singularity of the Schwarzschild metric is merely a coordinate singularity by constructing a scalar from the Riemann tensor. The equation presented, R_{abcd} R^{abcd} = 48M^2/r^6, is questioned for its validity. Contrary to the claim that the anti-symmetries of the Riemann tensor imply this quantity is zero, it is clarified that this scalar is known as the Kretschmann scalar. The discussion highlights the importance of correctly interpreting the properties of the Riemann tensor in the context of general relativity. Understanding these concepts is crucial for analyzing singularities in black hole physics.
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In chapter 8 of Padmanabhan's "Gravitation: Foundations and Frontiers" titiled Black Holes, where he wants to explain that the horizon singularity of the Schwarzschild metric is only a coordinate singularity, he does this by trying to find a scalar built from Riemann tensor and show that its well-behaved at the horizon. He writes (eq. 8.3) ##R_{abcd} R^{abcd}=\frac{48 M^2}{r^6}##. But this can't be correct. The (anti-)symmetries of the Riemann dictate that ##R_{abcd} R^{abcd}## is equal to zero. What is he doing here?
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The anti-symmetries do not dictate that this is zero.
 
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Also, this quantitiy is called the Kretschmann scalar. You may have seen posts about it recently.
 
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In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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