A Relativistically invariant 2-body phase space integral

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The discussion centers on the relativistically invariant 2-body phase space integral and the function ##\lambda^{\frac{1}{2}}##, which is identified as the Källén function. Participants seek references for equations involving this function, particularly in the context of total energy in the center-of-mass frame. A suggestion is made to consult a specific lecture note and the Review of Particle Physics for comprehensive kinematic insights. The Källén function is defined as the square root of the Källén function notation, clarifying its mathematical representation. Overall, the conversation emphasizes the need for authoritative resources on relativistic particle kinematics.
George Wu
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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:
1684333571500.png

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:
P$3{FTJ%2Z0E4A%)9[BD%[C.png

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.
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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