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  2. 16. Fission and Fusion - Particle and Nuclear Physics

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_16_FissionFusion.pdf
    10 Feb 2024: SEMF B(A, Z) = aV A aSA2/3 acZ. 2. A1/3 aA. ... Z2. A1/3(1 ϵ. 2. 5). Change in Binding Energy: B = B(ϵ)B(0) = aCA2/3(Z2.
  3. Not examinable Not examinable H1 H2 H3 H4 H5 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H8-appendices.pdf
    6 Dec 2023: e.g. : two possible exchanged gluons. bb. b b. e.g. : only one possible exchanged gluon. ... b b. gr. g r. 346 / 604. Not examinable. Not examinable.
  4. 9. The Weak Force - Particle and Nuclear Physics

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_09_Weak.pdf
    11 Dec 2023: Bc J/ψeν̄e. W. b. Bc c̄. e. ν̄e. c. c̄ J/ψ. ... t̄. b. gW Vtb. between quarks differing by one family are “Cabibbo Suppressed”.
  5. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H8.pdf
    6 Dec 2023: r r. b b. Other configurations where quarks don’t change colour •Only matrices with non-zero entries in 11 and 33 position are involved. ... e.g. : two possible exchanged gluons. bb. b b. e.g. : only one possible exchanged gluon.
  6. 2. Kinematics, Decays and Reactions - Particle and Nuclear Physics

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_02_KinematicsDecaysReactions.pdf
    30 Jan 2024: AµBµ = A.B = A0B0 A.B. or pµpµ = pµgµvp. v =µ=0,3. ... σ[60Ni(α,n)63Zn] σ[63Cu(p,n)63Zn]. n.b. common notation for nuclearreactions:aA bB A(a,b)B. Energy of p selected to give samec.m.
  7. 8. Quark Model of Hadrons - Particle and Nuclear Physics

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_08_QuarkModel.pdf
    26 Feb 2024: Examples:. Mesons(JP = 0. ): B(bū); B0(b̄d); B0s (b̄s); B. c (bc̄). ... m(s) = 510 MeV. )(m(t) = 175 GeV. m(b) = 4.5 GeV.
  8. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H8-without-appendices.pdf
    6 Dec 2023: r $ b; r $ g; b! g. SU(3)-colour symmetry is exact. ... r r. b b. Other configurations where quarks don’t change colour •Only matrices with non-zero entries in 11 and 33 position are involved.
  9. Particle Physics Dr Lester Handout 14 : Precision Tests ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H14_Frankenstein.pdf
    23 Nov 2023: b bb. q qb. b. b. « Each jet will contain one b-hadron which will decay weakly« Because is small hadrons containing. ... fb. be–. e+. Z. Z f. fb. b. e. « The only way to distinguish.
  10. Not examinable Not examinable H1 H2 H3 H4 H5 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H2-appendices.pdf
    4 Nov 2023: i if Ai Bi = 11 otherwise. 9>=. >;(by (49)). = s(A, B)d1Y. ... X. X2A. (AX )1 Y (AX ). =X. X2AA. (X )1 Y (X ). =X. X2A. (X )1 Y (X ) (since A A {A B, B 2 A} = A). =
  11. Particle and Nuclear Physics Handout #3 Nuclear Physics Lent/Easter…

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/PNP_Handout3.pdf
    19 Feb 2024: m(A,Z) = Zmp (A Z)mn B. B = aV A aSA2/3 acZ. ... Prof. Tina Potter 13. Basic Nuclear Properties 20. Nuclear Size Mirror Nuclei115 B.
  12. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H2-without-appendices.pdf
    4 Nov 2023: 34) () [(E m)A = ( p)B]. ()h(E m)( p)A = ( p)2B. ... pEm B. B. 8B. or, equivalently, we could say u+ = u 2 span{u1, u2} and u = v 2 span{v1, v2} where:.
  13. Particle and Nuclear Physics Handout #1 Problem…

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/PNP_Handout1.pdf
    19 Feb 2024: of magnitude.[ B+ (b̄u) and B0(b̄d) have masses of about 5280 MeV. ... b) Calculate the minimum energy of the ν which would permit e production.
  14. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H2.pdf
    4 Nov 2023: pEm B. B. 8B. or, equivalently, we could say u+ = u 2 span{u1, u2} and u = v 2 span{v1, v2} where:. ... X. X2A. (AX )1 Y (AX ). =X. X2AA. (X )1 Y (X ). =X. X2A. (X )1 Y (X ) (since A A {A B, B 2 A} = A). =

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