Nuclear Physics PHY 361 2008-04-21 Outline history structure of the nucleus • • • nuclear binding force liquid drop model shell model – magic numbers binding energy • • chart of nuclides line of stability, drip line, island of stability radioactivity • • ,, decay fission, fusion History Becquerel – discovered radioactivity (1896) Rutherford – nuclear model • • • classified ,, radiation, particle = 4He nucleus used scattering to discover the nuclear model postulated ‘neutrons’ A=Z+N (1920); bound p+ e- state? Mosley – studied nucleus via X-ray spectra • • correlated (Z = charge of nucleus) with periodic table extra particles in nucleus: A = Z + ? Chadwick – discovered neutron (1932) Pauli – postulated neutral particle from -decay (1930) Fermi – theory or weak decay (1933) ‘neutrino’ Fission – Hahn, Strassmann, (&Meitner!) (1938) • first reactor (chain reaction), Fermi (1942) Bohr, Wheeler – liquid drop model Mayer, Jensen – shell model (1949) Hofstadter – electron scattering (1953-) • • measured the charge density of various nuclei discovered structure in the proton (not point-like particle) Nuclear potential strong force + Coulomb repulsion (p-p) ~ finite square potential hard core – const. density Hofstadter, electron scattering Liquid drop model of the nucleus constant density like a liquid R = R0 A1/3 where R0 ~ 1.2 fm = A / (4/3 R3) = 1014 g/cm3 ! finite square potential • • p,n act as free particles inside of drop states filled to Fermi energy ‘surface tension’ • • normally prevents breakup excitation can induce split into smaller drops with lower overall energy Shell model of the nucleus 1949 – M. Mayer, J.H.D. Jensen similar to atomic orbitals difference: • • • • • • • • • quantized angular momentum energy levels multi-particle wave function nucleus no ‘central’ potential (nucleus) effective finite square potential complicated nuclear force strong dependence on spin two particles: p, n more types of decays atom Chart of Nuclides – binding energy A X q Z N A = Z + N = # protons + # neutrons B = Z MHc2 + N mnc2 - MAc2 nuclides – Z,N • • • • ex. 1H, 2H, 3He, 4He isotope isotone isobar isomer – constant Z (‘same place’) – constant N (isoto‘n’e) – constant A (‘same weight’) – excited state or nuclide Chart of Nuclides – lifetime magic numbers http://www.nndc.bnl.gov/chart Chart of Nuclides – decay mode magic numbers stable nuclide - decay , electron capture decay p decay n decay spontaneous fission http://www.nndc.bnl.gov/chart Chart of Nuclides – island of stability magic numbers http://en.wikipedia.org/wiki/Island_of_stability Nuclear decay modes: ++ decay - decay (isobar) + decay (isobar) electron capture (isobar) p decay (isotone) n decay (isotope) decay (isomers) electron conversion (EC) spontaneous fission (SF) double beta decay (2) neutrino-less double beta decay (0) beta-delayed n,p, decay ISOTONES ISOMERS ISOTOPES Z N Alpha-decay Beta-decay