Why Does Helium-3 Fission into H-3 and H Upon Neutron Absorption?

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SUMMARY

Helium-3 (He-3) fissions into Tritium (H-3) and Hydrogen (H-1) upon neutron absorption due to the energy dynamics involved in nuclear reactions. The reaction is less likely to proceed via the strong interaction alone, making the formation of a short-lived He-4 intermediate a crucial factor. The cross-section for this reaction is significantly lower at 55 microbarns compared to proton emission at 5500 barns, indicating a lower probability of occurrence. The emission of a single nucleon is favored over the split into two similar bound parts, which explains the observed reaction pathway.

PREREQUISITES
  • Understanding of nuclear reactions and conservation laws
  • Familiarity with nuclear cross-sections and their significance
  • Knowledge of isotopes, particularly Helium-3 and Helium-4
  • Basic principles of strong and electromagnetic interactions in nuclear physics
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  • Research the concept of nuclear cross-sections and their measurement techniques
  • Study the mechanisms of neutron absorption in light isotopes
  • Explore the role of intermediate states in nuclear reactions
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Students and professionals in nuclear physics, researchers studying nuclear reactions, and anyone interested in the behavior of isotopes under neutron bombardment.

murdakah
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I'm curious, why does Helium-3 fission into H-3 and H upon neutron absorption? Surely the He-4 nucleus configuration is more stable?
I get that the energy release may be what splits the nucleus, because it releases quite a lot of energy if it were to simply absorb the neutron.
 
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How does the energy get released if it does not split up?
That reaction is possible, but I would expect it to be unlikely as it cannot proceed via the strong interaction alone.
 
mfb said:
How does the energy get released if it does not split up?
That reaction is possible, but I would expect it to be unlikely as it cannot proceed via the strong interaction alone.
I find the cross-section quoted as 55 microbarns - compared to the cross-section of proton emission, at 5500 barns.
Looking around the light isotopes, those which can release the energy by strong interaction - He-3, Li-6, B-10 and N-14 - have cross-section in barns to kilobarns. Those which cannot and only are capable of electromagnetic interaction and gamma ray emission - all H isotopes, Li-7, Be, B-11, C, N-15, O - have cross-section in microbarn to millibarn range.
 
Ok, so you're saying that its just much more likely to split up. Actually, now that you mention it, it makes sense now. So if I'm understanding correctly, the He-4 does form, but is only a short lived intermediate product, proceeding to decay into other smaller sub-components.
n + He-3 --> (He-4) --> H-3 + H-1 (or H-2 + H-2?)
What promotes the one fission reaction to be more probable than the other? ( Assuming of course D+D is a valid product)
 
I'm not sure if the intermediate state lives long enough to call it He-4.
The emission of a single nucleon (or alpha particle for heavier nuclei) is more likely than a split into two similar and bounds parts.
 
mfb said:
I'm not sure if the intermediate state lives long enough to call it He-4.
The emission of a single nucleon (or alpha particle for heavier nuclei) is more likely than a split into two similar and bounds parts.
I see. So just proton emission then. Thanks a lot. :)
 
murdakah said:
I'm curious, why does Helium-3 fission into H-3 and H upon neutron absorption? Surely the He-4 nucleus configuration is more stable?
I get that the energy release may be what splits the nucleus, because it releases quite a lot of energy if it were to simply absorb the neutron.

Nuclear reactions have to conserve both energy and momentum. When you only have one product it's not possible to conserve both except when the reactants have the right kinetic energies. Thus nuclear reactions with only 1 product tend to be rare. For instance why the d+d = He-4 reaction is also rare.
 

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