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  2. 10. Electroweak Unification - Particle and Nuclear Physics

    https://www.hep.phy.cam.ac.uk/~chpotter/particleandnuclearphysics/Lecture_10_Electroweak.pdf
    19 Feb 2024: the W , Z, and γ. W W3W.  ; B  W Z. ... m2γ = ⟨W3 sinθW B cosθW |M̂2|W3 sinθW B cosθW ⟩. = m2W sin2 θW m. 2B cos. 2 θW 2m2WB cosθW sinθW = 0.
  3. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H13.pdf
    6 Dec 2023: p3 = (E, E sin, 0, E cos). p4 = (E,E sin, 0,E cos). ... ML =gWp2 (0, 0, 0, 1) mW (0,cos,i, sin) =. 1p2gW mW sin.
  4. H1 H2 H3 H4 H5 H6 H7 H8 H9 ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/handouts2023/H5.pdf
    25 Oct 2023: 1. 642sh|Mfi|2i =. e4. 82s. 1 14 (1 cos). 2. (1 cos)2. ... c = cos(/2). In terms of = |p|Eme. (Non-relativistic limit:! 0Ultra-relativistic limit:!
  5. NATURAL SCIENCES TRIPOS: Part III PhysicsMASTER OF ADVANCED STUDY ...

    https://www.hep.phy.cam.ac.uk/~lester/teaching/partIIIparticles/exams/PartIIIParticles_202223_with_answers.pdf
    5 Oct 2023: Q2 = 2E1 E3(1 cos θ)Q2 > 0. (b) by considering the invariant mass of the final state hadronic system, orotherwise, determine the range of values which x can take. ... y =p2.qp2.p1. =p2.( p1 p3). 2E2. =p2.(0, 0, 0, E(1 cos θ)).
  6. 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.

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