Graduate Second derivative of Heaviside step function

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The discussion focuses on the computation of the second derivative of the Heaviside step function, specifically in the context of quantum field theory as presented in Peskin and Schroeder. The action of the Klein-Gordon operator on the propagator is analyzed, leading to the equation (∂² + m²)D_R(x-y) = -iδ⁴(x-y). The first derivative of the Heaviside function results in a delta function, while the second derivative yields a distribution with specific properties. The retarded Green's function is identified as proportional to Θ(x⁰ - y⁰), confirming its role in the context of the Klein-Gordon operator. This highlights the mathematical relationships essential for understanding propagators in quantum field theory.
abhinavabhatt
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TL;DR
Identifying Klein Gordon propagator as Green's Function
In QFT by peskin scroeder page 30 the action of Klein Gordon Operator on propagator
(∂2+m2)DR(x-y)=∂2θ(x0-y0)...

how to compute this
2θ(x0-y0)?
 

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First derivative is delta function. The second derivative ##\delta'(x)## has property
\int \delta'(x) f(x) dx = -f'(0)
 
Thanks for the answer.
 
Note that Peskin and Schroeder write in fact the correct equation, i.e.,
$$(\Box+m^2) D_{R}(x-y)=-\mathrm{i} \delta^{(4)}(x-y).$$
Since by definition ##D_R(x-y) \propto \Theta(x^0-y^0)## this function is the retarded Green's function of the Klein-Gordon operator (modulo the usual conventional factor ##-\mathrm{i}## on the right-hand side).
 

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