Main difference between P, S & D Partial Waves in Decays?

Click For Summary

Discussion Overview

The discussion revolves around identifying the contributions of S, P, and D partial waves in the decay of hadrons and mesons, specifically focusing on decay channels such as ##a_1 \to \rho \pi## and ##a_2 \to \rho \pi##. Participants explore the quantum numbers involved, conservation laws, and the implications for decay width.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about identifying S, P, or D wave contributions in hadron decays, using the example of the decay channel ##a_1 \to \rho \pi##.
  • Another participant explains the importance of quantum numbers and conservation laws, noting that the decay involves ##J^{P}=1^+## for ##a_1##, ##J^P=1^-## for ##\rho##, and ##J^P=0^-## for ##\pi##, leading to possible partial waves.
  • A later reply clarifies that for the decay channel ##a_2 \to \rho \pi## with quantum numbers ##2^+ \to 1^- 0^-##, the allowed value for angular momentum L is only 2 (D wave) to conserve total angular momentum.
  • Another participant inquires about which total angular momentum to consider for conservation, asking whether it should be the ##J## of ##a_2##, ##\rho##, or their relative difference.
  • Further clarification is provided that the total angular momentum of the final system must equal that of the initial system, specifically referencing the total angular momentum of ##a_2##.
  • A participant requests literature recommendations for understanding hadron decays, indicating their newness to the field.
  • Another participant suggests several references, noting that advanced topics can be challenging to find in understandable literature.

Areas of Agreement / Disagreement

Participants generally agree on the importance of quantum numbers and conservation laws in determining partial wave contributions, but specific interpretations and applications of these principles remain contested, particularly regarding the total angular momentum considerations.

Contextual Notes

The discussion highlights the complexity of hadron decay processes and the need for careful consideration of quantum mechanical principles, with some assumptions about the applicability of conservation laws and the interpretation of angular momentum that may not be universally agreed upon.

Naeem Anwar
Messages
14
Reaction score
0
I am a little confused about; how to identify that Hadron/Meson may have S, P or D wave contribution to its decay to other hadrons. e.g in case of light meson decay

a1→ ρπ

this decay channel have two partial waves S & D, so my question is that from where I can guess that this channel have two or more partial wave contributions to total decay width?
 
Physics news on Phys.org
You need to consider the quantum numbers of the particles involved. In this case the ##a_1## has ##J^{P}=1^+##, the ##\rho## has ##J^P=1^-## and the ##\pi## has ##J^P=0^-##. Your decay is therefore of the kind ##1^+\to1^-0^-##.
Since this is a strong decay you need to conserve both total angular momentum and parity. The total parity of the final system is given by ##P_{\rho\pi}=P_\rho P_\pi (-1)^L##, where L is the relative angular momentum. The possible candidates to conserve you parity are therefore L=0,2,4,6,... Now with L=0 and L=2 you are fine and you can conserve both parity and total angular momentum. With L>2 though, even if parity is conserved, you can't conserve momentum anymore since ##J=1\otimes 0\otimes L## for L>2 always gives total angular momentum greater that 1 (the J of the ##a_1## meson).

Is this what you were looking for?
 
  • Like
Likes   Reactions: vanhees71 and Naeem Anwar
Got it! Yes I was exactly looking this. Thanks for this brief & exact answer, I am on the track now. Let me please correct here once more, for the channel ##a_2\to\rho\pi## with quantum numbers ##2^+\to1^-0^-##, by using relation ##P_{\rho\pi}=P_\rho P_\pi (-1)^L##, now possible value of L=0,2,4,6... but allowed value is only 2 (D wave). To conserve parity allowed values are 0 & 2 but to conserve ##J## only 2, so my question is that which total angular momentum I will keep in mind to conserve here? The ##J## of ##a_2## the ##J## of ##\rho## or their relative difference?
 
The total angular momentum of the final system, which in your case is ##J_\rho\otimes J_\pi\otimes L## must be equal to the total angular momentum of the initial one, which in your case is ##J_{a_2}=2##.
 
Dear Sir Einj..!
Thanks for the valuable comments. Could you kindly recommend some basic literature on the fundamentals of hadron decays. I am quite new in this field, just started the graduation course work with little research related the strong decays of hadrons (mesons).

Thanks! Looking forward to listen from you.
 
For this advanced topics is usually quite hard to find decent understandable literature. I have few suggestions but you might need to spend some time on them since they are not really straightforward:

1) Wise - "Heavy Quark Physics"
2) Donoghue - "Dynamics of the Standard Model"

These two are real books. However I always found the best reference to be a review from Casalbuoni et al.: http://arxiv.org/abs/hep-ph/9605342 . I think so far is the most complete review we have and it's quite understandable.

I hope this is useful!
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
Replies
7
Views
2K
  • · Replies 31 ·
2
Replies
31
Views
3K
  • · Replies 0 ·
Replies
0
Views
4K
Replies
2
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 0 ·
Replies
0
Views
3K
  • · Replies 49 ·
2
Replies
49
Views
13K