'Theta function' setting conditions similar to delta function?

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.
 
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