Undergrad Is the Kroneker Delta Identity Used Correctly in this Paper?

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The discussion centers on the correct application of the Kronecker delta identity in a paper, specifically questioning the identity $$ \delta^3 (k) \delta^3 (k) = \frac{2\pi^2}{k^3} ~ \delta (k_1- k_2) $$ and its implications for wave numbers k, k1, and k2. It highlights the importance of distinguishing between the Kronecker delta, which applies to discrete variables, and the Dirac delta function, which is used for continuous variables. The left-hand side of the equation is dimensionally inconsistent with the right-hand side, raising concerns about the validity of the identity. Furthermore, it is noted that squaring the Dirac delta function is nonsensical, indicating a potential error in the paper. The conclusion emphasizes that the paper does not contain the erroneous formula in question.
Safinaz
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A question about a Kroneker Delta identity
Is there a Kroneker Delta identity:

$$ \delta^3 (k) \delta^3 (k) = \frac{2\pi^2}{k^3} ~ \delta (k_1- k_2) $$?

Where k is a wave number. In this Paper: Equations 26 and 27, I think this identity is used to make ##k_1=k_2## and there is an extra negative sign.
 
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Could you tell us what is the relation among k, k_1 and k_2 ?
Assuming they have same dimension k, dimension of LHS is k^-6 that of RHS is k^-4. They do not coincide.
 
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First of all you must clearly distinguish between a Kronecker (sic!) ##\delta## and Dirac ##\delta## distributions, which refers to discrete variables, i.e.,
$$\delta_{k_1 k_2}=\begin{cases} 1 &\text{for} \quad k_1=k_2, \\
0 &\text{for} k_1 \neq k_2. \end{cases}
$$
Then you have ##\delta_{k_1k_2}^2=\delta_{k_1 k_2}##.

For Dirac-##\delta## distributions the square doesn't make any sense. Whenever it occurs somewhere, the authors make a mistake. In the paper you linked, nowhere is such a non-sensical formula though!
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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