Defiunition of kroneker delta as a tensor

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hi,

the delta symbol as a tensor (in the minkovski space, in case one has to be specific), what is it exactly?
is it
\delta^a_b = \frac{\partial{x^a}}{\partial{x^b}}

is it
\delta^a_b = g^{ac} g_{cb}or is there some other definition?thanks
 
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The Kroneker delta is the the indexed components of the Identity operator which looks the same in all bases.

\mathbf{1}\mathbf{x} = \mathbf{x}: x^\mu = \delta^\mu_\nu x^\nu
 
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tamiry said:
hi,

the delta symbol as a tensor (in the minkovski space, in case one has to be specific), what is it exactly?



is it
\delta^a_b = \frac{\partial{x^a}}{\partial{x^b}}

is it
\delta^a_b = g^{ac} g_{cb}


or is there some other definition?


thanks

It is both. The kroneker delta represents the mixed (covariant/contravariant) components of the metric tensor, and applies to both flat as well as curved spacetime.
 
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I believe the technical definition is:

\delta^a_b = 0 (a != b), \delta^a_a = 1

In other words, it's just the identity matrix. The two "definitions" you gave don't define δ, rather you can show those two expressions equal δ as I defined it.
 
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To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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