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![Page 1: PHYS3002. Nuclei and Particles. Synoptic. · 2018. 7. 9. · Decay Rates . Alpha Decay Beta Decay . Gamma Decay Nuclear Fission Nuclear Fusion _+ + e- + V. (4+4) {P} _+ e {D} + -XN(t)](https://reader033.vdocument.in/reader033/viewer/2022060808/608cdd597a556c3c3f7202ac/html5/thumbnails/1.jpg)
PHYS3002. Nuclei and Particles.Synoptic.
![Page 2: PHYS3002. Nuclei and Particles. Synoptic. · 2018. 7. 9. · Decay Rates . Alpha Decay Beta Decay . Gamma Decay Nuclear Fission Nuclear Fusion _+ + e- + V. (4+4) {P} _+ e {D} + -XN(t)](https://reader033.vdocument.in/reader033/viewer/2022060808/608cdd597a556c3c3f7202ac/html5/thumbnails/2.jpg)
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Rutherford Scattering and cross section
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Cross section
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Alpha Decay
Beta Decay
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Gamma Decay
The total angular momentum change, L in a nuclear transition can take the values |Li − Lf | ≤L ≤ |Li + Lf |, L>0This is also subject to selection rules for the parity difference between initial and final states: P = (−1)L, for electric transitionsand P = (−1)L−1, for the (even further suppressed) magnetic transitions. Here are some examples: 2+ → 1−(E1)2+ → 1+(M1)3+ → 1−(M2)3+ → 1+(E2)
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The Mőssbauer Effect
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Accelerators and particle kinematics
CM frame:
Fixed target:
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CMS DETECTOR
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Weak interactions
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Electromagnetic Interactions
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QCD(uuu)
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Summary of Conservation laws