S- and P-Wave Cross Section Explained

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SUMMARY

The discussion clarifies the concepts of s-wave and p-wave cross sections in quantum mechanics, specifically relating to the l-quantum number of incoming waves. The l-quantum number is defined as 0 for s-waves and 1 for p-waves, paralleling atomic physics notation. The cross section is directly proportional to the modulus square of the scattering amplitude, with contributions from partial waves truncated at a maximum l value determined by the potential range and incoming particle momentum. This understanding is essential for interpreting scattering phenomena in quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with partial wave expansion techniques
  • Knowledge of angular momentum in quantum systems
  • Basic grasp of scattering theory and cross section calculations
NEXT STEPS
  • Study the mathematical formulation of partial wave expansion in quantum mechanics
  • Explore the implications of angular momentum quantization in scattering processes
  • Learn about the relationship between scattering amplitude and cross sections
  • Investigate the role of excited states in particle scattering and cross-section variations
USEFUL FOR

Students and professionals in physics, particularly those focusing on quantum mechanics, scattering theory, and particle physics. This discussion is beneficial for anyone seeking to deepen their understanding of wave interactions and cross-section analysis.

touqra
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What does it mean when they say s wave cross section, p wave cross section .. ?
 
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touqra said:
What does it mean when they say s wave cross section, p wave cross section .. ?

the [itex]l[/itex]-quantum number of the incoming wave. You often have a plane wave coming into the target. The plane wave you write as a linear combination of spherical waves, and you call this "Partial Wave expansion".

http://farside.ph.utexas.edu/teaching/qm/lectures/node70.html

The [itex]l[/itex] that you see in eq 957 is then the "[itex]l[/itex] - QM number".
And [itex]l[/itex] is denoted by, 0 = s, 1 = p, 2 = d, etc, same as in atomic physics notation.

Semiclassicaly, you can see the [itex]l[/itex] as the classical angular momenta of the incoming particle with respect to the centre of the scattering potential. And also the [itex]l[/itex] is quantisized, so only some values of [itex]l[/itex] are allowed.

Now since the sum goes to infinity in eq 957, we cut of where we expect no partial waves to contribute. And that is often assigned by [tex]l_{max} \approx R\cdot k[/tex]
Where R is the range of the potential and k is the momenta of the incoming particle (wave number).

Now the cross section is proportional to the scattering amplitude modulus square, i.e the modulus square of eq. 965 times a constant with a lot of pi's hbar's etc.

So the s-cross section, you only have [itex]l[/itex] = 0 in you sum, and p-cross section only [itex]l[/itex] = 1. etc.

I hope you got the idea =)
 
Hello,
To munch the QM into an analogy:
Another way to look at is - how does one particle look to another. If you assume the target particle to be ball-like, then in its basic form (ground state), you'll get the classic 3D cross-section - this is how it will appear to the incoming particle and such it will be scattered from the target particle. But if the particle is excited to a higher state, then it will no longer appear as a ball but something else entirely. And vice versa.
Smoochie
 

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