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Lesson 7 Alpha Decay. Alpha decay (  ) Decay by the emission of doubly charged helium nuclei 4 He 2+. 238 U  234 Th + 4 He  Z = -2,  N=-2,  A=-4.

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Presentation on theme: "Lesson 7 Alpha Decay. Alpha decay (  ) Decay by the emission of doubly charged helium nuclei 4 He 2+. 238 U  234 Th + 4 He  Z = -2,  N=-2,  A=-4."— Presentation transcript:

1 Lesson 7 Alpha Decay

2 Alpha decay (  ) Decay by the emission of doubly charged helium nuclei 4 He 2+. 238 U  234 Th + 4 He  Z = -2,  N=-2,  A=-4 All nuclei with Z≥83 decay by  -decay as do some rare earth nuclei.Alpha decay is also known in the 100 Sn region.

3 Alpha Decay The emitted  -particles are monoenergetic,ranging in energy from 1.8-11.6 MeV (typically 4-9 MeV). They can be stopped by a piece of paper and are thus an internal radiation hazard rather than an external hazard. The naturally occurring  -emitters form long series of nuclei that decay to one another. Some of these naturally occurring decays series involve isotopes of Rn, a gas.

4 Important Features of Alpha Decay Generally energy of decay increases with increasing Z, but in any case the energy of the emitted  -particle is less than the Coulomb barrier for the  -nucleus interaction. For e-e nuclei, decay leads to gs of daughter. For odd A nuclei, decay is not to the gs but a low-lying excited state.

5 Energetics of Alpha Decay Q alpha

6 Energetics of Alpha Decay (cont.) Q alpha --Generally increases with increasing Z, but is subject to shell effects. N=152-154 Z=82, N=126

7 Q , T  Difference between detecting emitted alpha particle and detecting alpha from implanted atom.

8 Closed decay cycles Used to measure unknown masses or Q values for beta decay

9 Understanding natural alpha- decay chains In the U natural decay series, see pattern of mixed alpha and beta decays. Why?

10 Understanding Alpha Decay The problem:

11 Understanding Alpha Decay (cont.) The Geiger Nuttall Law

12 Theory of Alpha Decay One of the first successes of quantum mechanics

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14 After some algebra and simplifying for the nuclear case Then This is called the “one-body” theory of alpha decay

15 How well does one-body theory work? Role of “pre-formation factor”

16 Effect of angular momentum Selection Rules

17 Which states of daughter are populated in alpha decay? Dominant effect is Q  Angular momentum effect Angular momentum = Parity = (-1)

18 Hindrance Factors Hindrance Factor=t 1/2 (meas)/t 1/2 (one-body)

19 Proton Decay Same theory as alpha decay, except no pre- formation factor for protons Where do you expect to see proton decay? (S p =0) proton dripline

20 Proton Decay(cont.) Proton energies are low and transmission factors are small.

21 Proton Decay(cont.) Alpha decay complicates measurements

22 Heavy Particle Decay What about emitting particles other than alphas or protons? Q 12C


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