'Theta function' setting conditions similar to delta function?

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The discussion centers on the confusion surrounding the 'theta function' mentioned in a paper, which is clarified to be the Heaviside step function. This function is defined as the area under a delta function, indicating values of s that satisfy a specific inequality. The integral presented in the paper can be expressed as an integral involving the delta function, confirming its relationship to the Heaviside function. The participant expresses relief at understanding this connection, despite initial uncertainty. Overall, the conversation highlights the importance of recognizing the Heaviside function in the context of integrals involving delta functions.
Mithra
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Hi, I'm reading through a paper and have come across what my tutor described as a 'theta function', however it seems to bear no resemblance to the actual 'theta function' I can find online. In the paper it reads:

\int^1_0 dz~\theta (s-\frac{4m^2}{z}-\frac{m^2}{1-z})

And apparently this ensures that s > \frac{4m^2}{z}+\frac{m^2}{1-z} when that expression is included in a longer integration over s and z, however I've never come across something like this before. That expression above is obtained integrating

\delta (q-p-p')

over p and p' (4-momenta). Does anyone have any advice about what this is and how to include it in the integral? Thanks!
 
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Hi Mithra! :smile:

this θ is the usual theta function

θ(f(x)) (the Heaviside step function) is the area under a delta function (0 before f(x), 1 after f(x)) …

so it is the integral of a delta function from minus-infinity to f(x): \int^{f(x)}_{-\infty} \delta(y) dy​

\int^1_0 dz~\theta (s-\frac{4m^2}{z}-\frac{m^2}{1-z})

=\int^1_0 dz\int^{s-\frac{4m^2}{z}-\frac{m^2}{1-z}}_{-\infty} dw~\delta (w)
 
tiny-tim said:
Hi Mithra! :smile:

this θ is the usual theta function

θ(f(x)) (the Heaviside step function) is the area under a delta function (0 before f(x), 1 after f(x)) …

so it is the integral of a delta function from minus-infinity to f(x): \int^{f(x)}_{-\infty} \delta(y) dy​

\int^1_0 dz~\theta (s-\frac{4m^2}{z}-\frac{m^2}{1-z})

=\int^1_0 dz\int^{s-\frac{4m^2}{z}-\frac{m^2}{1-z}}_{-\infty} dw~\delta (w)

Ah brilliant, thanks very much! I thought it must be related to the Heaviside function, but could only seem to find Theta function. A little embarrassing having not heard of these as a fourth year physicist but hey ho :P. Cheers.
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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