Relativistically invariant 2-body phase space integral

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George Wu
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TL;DR
I encounter a function that I don‘t know in the calculation of Relativistically invariant 2-body phase space integral
I encounter a function that I don‘t know in the calculation of Relativistically invariant 2-body phase space integral:
Three-line derivation of the two-body Lorentz-invariant phase space dPS2: a delta-function form, then (1/(4pi)^2)|p1 cm|/sqrt(s) dOmega1, then (1/(8pi)) lambda^(1/2)(1, m1^2/s, m2^2/s) dx1 dx2.

in this equation, ##s##is the square of total energy of the system in the center-of-mass frame(I think)
I don't know what the function ##\lambda^{\frac{1}{2}}## is.
There are more equations involving this function:
Three equations for two-body kinematics in the centre-of-mass frame: |p1cm| = |p2cm| = lambda^(1/2)(s, m1^2, m2^2) / (2 sqrt(s)), E1cm = (s + m1^2 - m2^2) / (2 sqrt(s)), and E2cm = (s + m2^2 - m1^2) / (2 sqrt(s)).

I just want to know if anyone knows which textbook these equations come from, or what the function ##\lambda^{\frac{1}{2}}## is.
 
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Do you have any reference for those 2 screenshots? A book, some lecture notes we could have access to. Otherwise, I can't recall any special function in mathematics with that notation.