Phase space in particle physics: what is it?

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Phase space in particle physics refers to the range of momentum and energy configurations available during particle decay, governed by energy-momentum conservation. It indicates how much momentum can be shared among decay products; limited phase space occurs when the sum of the rest masses of the products is close to that of the initial particle, resulting in minimal momentum. Conversely, ample phase space allows for greater momentum distribution, enhancing decay rates. The discussion highlights that while the term is used frequently, its definition can be elusive in some texts, such as "Quarks and Leptons" by Halzen and Martin. Understanding phase space is crucial for analyzing particle decay processes effectively.
tiger_striped_cat
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This should be an easy general question to someone out there. My "quarks and Leptons" book by Halzen and Martin introduces the term "phase space" 50 pages before the index reference, and never seems to define it.

The decay
\psi(s\overline{s}) \longrightarrow K(q\overline{s}) + \overline{K}(\overline{q}s)

with q= u,d is inhibited by lack of phase space while \phi \longrightarrow \pi\pi\pi has plenty of phase space but requires annihilation of the s\overline{s} pair.

What is phase space in this context?
Thanks
 
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Just a fancy term for energy-momentum conservation. In a nutshell, either the rest mass of the products is larger than the rest mass of the initial particle, or the difference is extremely small. Most likely the formerl.
 
tiger_striped_cat said:
This should be an easy general question to someone out there. My "quarks and Leptons" book by Halzen and Martin introduces the term "phase space" 50 pages before the index reference, and never seems to define it.



What is phase space in this context?
Thanks

Roughly speaking, it's a jargon term for the amount of momentum available to the decaying particle. If the sum of the rest mass of the product particles is very close to the rest mass of the initial particle, one says that there is little phase space available, meaning that that the produced particles are created with almost no three-momenta (in the rest frame of the decaying particle). However, if the mass of the produced particles is much smaller than the mass of the decaying particle, there's plenty of momentum to share among the produced particles and this enhanced the decay rate.

By the way, H&M *do* define the explicit expressions for phase space in the case of a decaying particle. Unfortunately, I don't have it with me but I'll give you the equation number later if you want.


Pat
 
Phase space for a system is the set of possible momentum/energy points for which momentum and energy are conserved. If, for example, A -> B + C, then in A's center of momentum frame, pB + pC = 0 (3D vector equation), and eB+eC = mA. In this case, the available phase space is a spherical surface whose radius depends on the masses.

Also, sometimes people will refer to integration over 3- or 4- momentum space as integration over phase space.

Regards,
Reilly Atkinson
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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