Why Does Alpha & Beta Particle Emission Occur in Radioactive Nuclei?

In summary: Thanks Bob S for catching that ... I got my decay modes mixed up :uhh:In summary, radioactive nuclei can also decay through spontaneous fission and electron capture, but alpha decay is the most common type of decay due to the high binding energy of the alpha particle and the preformation probability of nucleons forming into an alpha particle. Neutron emission, however, is less common due to the absence of a Coulomb barrier in a cold nucleus and the possibility of it being a result of photo-neutron emission or photodisintegration.
  • #1
ksac
9
0
Do we know why radioactive nuclei only decay through emission of alpha and beta particles? There is spontaneous fission in some cases, of course, but what I mean to ask is, why should just a proton or just a neutron or a particle X with 2 protons and 3 neutrons, or whatever else not be emitted? Why does this particular combination of 2 and 2 in alpha particle work as against any other?
 
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  • #2
cluster decay

Hi ksac! :smile:

From http://en.wikipedia.org/wiki/Cluster_decay" …
Cluster decay is a type of nuclear decay in which a radioactive atom emits a cluster of neutrons and protons heavier than an alpha particle. This type of decay happens only in nuclides which decay predominatly by alpha decay, and occurs only a small percentage of the time in all cases. Cluster decay is limited to heavy atoms which have enough nuclear energy to expel a portion of its nucleus.

Cluster decay has an intermediate position between alpha decay (in which a nucleus spits out a 4He nucleus) and spontaneous fission …

… see the full article for more details. :wink:
 
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  • #3
ksac said:
Do we know why radioactive nuclei only decay through emission of alpha and beta particles? There is spontaneous fission in some cases, of course, but what I mean to ask is, why should just a proton or just a neutron or a particle X with 2 protons and 3 neutrons, or whatever else not be emitted? Why does this particular combination of 2 and 2 in alpha particle work as against any other?
The alpha particle is a pretty stable collection of nucleons.

Radionuclei also experience electron capture in which a K-electron (and possibly L-electron) will be capture by the nucleus and a proton will be transformed into a neutron. It has the same effect as positron emission, in which Z decreases by 1 with A (integer) remaining the same.

Also, some of the transuranics undergo spontaneous fission.
 
  • #4
ksac said:
Do we know why radioactive nuclei only decay through emission of alpha and beta particles? There is spontaneous fission in some cases, of course, but what I mean to ask is, why should just a proton or just a neutron or a particle X with 2 protons and 3 neutrons, or whatever else not be emitted? Why does this particular combination of 2 and 2 in alpha particle work as against any other?

Beta decay is qualitatively different from alpha decay. It's a weak-force process, and it doesn't involve emission of a particle or cluster of particles that were already present inside the parent nucleus.

Tiny-tim has pointed out that other types of particle emission do occur. Another thing to realize is that in a hot nucleus (e.g., a nucleus that's just been created via fusion reactions in an accelerator), you do get lots of proton and neutron emission.

The reason you'll never see spontaneous neutron emission in a cold nucleus is that there's no Coulomb barrier to tunnel through. Therefore any neutron that has enough energy to escape will do so immediately, not after a longer time delay as with charged particles.

The main reason that alpha decay tends to be favored is that the alpha is a doubly magic nucleus, so it has an extremely large binding energy. That means that by phase space arguments, alpha emission is strongly favored.

Another issue is the somewhat foggy notion of "preformation." A straightforward way of estimating alpha decay rates is as follows. You calculate the probability P of tunneling out through the coulomb barrier. You estimate the frequency f with which an alpha particle assaults the barrier, which is basically found by taking the velocity scale (1% of the speed of light) and dividing by the distance scale (a few fm). Then 1/(Pf) gives an estimate of the alpha decay half-life. This estimate has all the right behavior as a function of A and Z, but it's much too short by some large, constant factor. To account for this you assume that there's only some small probability that neutrons and protons will already have gotten together and formed themselves into an alpha particle. This preformation probability is difficult to calculate, but it makes sense that it's higher for alphas than for other clusters. This is because (a) an alpha is small (only 4 particles), (b) the nuclear residual interaction includes a strong pairing force, which sort of favors the formation of nn and pp correlations, and (c) the binding energy of an alpha is very favorable. This is really just a plausibility argument. Formally, you really can't have an alpha particle cruising around inside a nucleus, because of the Pauli exclusion principle. However, nucleon-nucleon correlations inside nuclei do exist.
 
  • #5
bcrowell said:
The reason you'll never see spontaneous neutron emission in a cold nucleus is that there's no Coulomb barrier to tunnel through. Therefore any neutron that has enough energy to escape will do so immediately, not after a longer time delay as with charged particles.
Sometimes a radioactive nucleus will emit a neutron along with an antineutrino. This the process called K-capture (where an orbital electron and a proton convert to a neutron) discussed by Astronuc above.
Bob S
 
  • #6
Bob S said:
Sometimes a radioactive nucleus will emit a neutron along with an antineutrino. This the process called K-capture (where an orbital electron and a proton convert to a neutron) discussed by Astronuc above.
Bob S
Careful - In electron capture, the neutron stays in the nucleus. Neutron emission may happen when a gamma ray of sufficient energy interacts with the nucleus - a process known a photo-neutron emission - or photodisintegration in the case of a deuteron (d (γ,n) p).

One can also look at the requirement for various decay schemes - looking at the masses of the nuclei before and after the reaction with E or ΔE = Δm c2 to see if E or ΔE is > 0 (exothermic, preferred) or < 0 (endothermic, not spontaneous, but requires energy input).
 
  • #7
Astronuc said:
Careful - In electron capture, the neutron stays in the nucleus. Neutron emission may happen when a gamma ray of sufficient energy interacts with the nucleus - a process known a photo-neutron emission - or photodisintegration in the case of a deuteron (d (γ,n) p)..
My bad Sorry Bob S
 
  • #8
I forgot to mention two neutron-emitting radioactive sources I used as a grad student: Plubyllium (symbol PuBe), and Pobyllium (symbol PoBe). I don't know what the plutonium polonium beryllium mixture ratios were. Lots of neutrons, but the alphas were fully contained.
Bob S
[added] Read the abstract of
http://adsabs.harvard.edu/abs/1955PhRv...98..740S
 
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1. Why do some nuclei emit alpha and beta particles?

Alpha and beta particle emission occur in radioactive nuclei because these particles are released when an unstable nucleus attempts to reach a more stable state. This process is known as radioactive decay.

2. What causes a nucleus to become unstable?

A nucleus becomes unstable when there is an imbalance between the number of protons and neutrons. This can occur when there are too many or too few neutrons compared to the number of protons, leading to an unstable ratio.

3. How do alpha and beta particles differ?

Alpha particles are composed of two protons and two neutrons bound together, making them essentially a helium nucleus. Beta particles, on the other hand, are high-energy electrons or positrons that are emitted from the nucleus during decay.

4. What is the significance of alpha and beta particle emission in nuclear reactions?

Alpha and beta particle emission play a crucial role in nuclear reactions as they help to stabilize the nucleus by releasing excess energy. Additionally, the emission of these particles can also result in the formation of new elements.

5. How can we detect alpha and beta particles?

Alpha particles can be detected using a Geiger-Muller tube, which measures the ionization caused by the particles. Beta particles can be detected using a scintillation counter, which detects the light produced when the particles interact with a scintillator material.

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