Solving Decay & Parity Problem with J=1 & Spin 1/2 Particles

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SUMMARY

The discussion centers on the decay of a particle with spin J=1 into two identical particles with spin 1/2. The key conclusion is that the total spin of the final state must be S=1 and the orbital angular momentum L=1, which satisfies the conservation of angular momentum. The assumption that J is conserved is confirmed, and the requirement for an antisymmetric wave function leads to the conclusion that S=1 and L=1 is the only viable solution. Misunderstandings regarding the relationships between spin and orbital angular momentum are clarified.

PREREQUISITES
  • Understanding of angular momentum conservation in quantum mechanics
  • Fermi-Dirac statistics and antisymmetric wave functions
  • Concept of total angular momentum J as a vector sum of spin S and orbital angular momentum L
  • Knowledge of particle spin states, specifically spin 1/2 and spin 1 particles
NEXT STEPS
  • Study the principles of angular momentum coupling in quantum mechanics
  • Learn about Fermi-Dirac statistics and its implications for identical particles
  • Explore the mathematical formulation of total angular momentum J = L + S
  • Investigate examples of particle decay processes involving spin and parity
USEFUL FOR

Physicists, particularly those specializing in quantum mechanics and particle physics, as well as students seeking to deepen their understanding of angular momentum and particle decay processes.

erwinscat
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Hello all ! I was trying to solve the following problem : you have a particle with spin J=1 and unknown parity that decays into 2 indentical particles of spin = 1/2

We want to know how much the angular momentum of the final state is and also the final total spin.

Now, my reasonment was the following.

Stot_final = either 0 or 1 since it is the vector sum of the spin of both identical final particles.

Knowing that |L-S|<=J<= L+S we have to cases but I assumed that J=1 is conserved in the decay but it wasn't told so ...

we would have

for S=0 => L= 1
for S=1 => L= (0,1,2)

knowing that the final particles are indentical they must have a antisymmetric wave function due to Fermi Dirac...and so L must be odd . => L=1

but we still have to cases (S,L)= (0,1) or (1,1) if J=1 was to be conserved I'd say th only possible is (0,1) but the solutions say the only possibile solution knowing that J=1 is (1,1) ..

Conclusion, I don't know where I'm mistaking !

Any help would be appreciated ! Maybe I shouldn't assume that J was conserved...

Thanks in advance !
Erwin
 
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J is conserved and equals 1.
But,
"knowing that the final particles are indentical they must have a antisymmetric wave function due to Fermi Dirac...and so L must be odd . => L=1"
is wrong.
The spinXorbital wave function must be antisymmetric.
This means that S=0 goes with L=0 or 2, neither of which can give J=1.
Therefor S=1, and L=1, with 1+1=1.
 
Hi and thanks a lot for the answer !

There is still something I don't get .. how do you get L=0 or L=2 with S=0 and more how do you get J=1 = L+S = 1+1 ?? if L=1 and S= 1 shouldn't you get in this case 0 or 2 . (L-S or L+S)?

Isn't this correct :

|L-S|<= 1<= L+S

if S= 0 then you have L=1
if S=1 then you have L= 0,1,2 ?

I guess not since you just said so ...but why isn't that so , where is my mistake ?

Thanks in advance !
Erwin
 

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