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Cosmic Alchemy: How Are We Made ? Prof. Paddy Regan FInstP Department of Physics University of Surrey Guildford, GU2 7XH p.regan@surrey.ac.uk
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Medieval alchemist…trying to turn base metals into gold… Mistake…to try and use ‘chemistry’…needed nuclear physics
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3 Z = number of protons N= number of neutrons A = N+Z = mass number neutral atom has Z electrons m(nucleon) 2000 m(electron) AXNAXN Z For element X write Atoms comprise nuclei and electrons - known since 1910 Nuclei comprise protons and neutrons - known since 1932 the neutron Ernest Rutherford Nobel Chemistry 1909 Founder of Nuclear Physics the nucleus Marie Curie (see later) Nobel Physics 1903 Nobel Chemistry 1911 radioactivity J J Thomson Nobel Physics 1906 the electron
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Atoms (‘indivisible’) …… ~10 -10 m, electrons (and their orbital structure) determine chemistry of the elements, e.g., NaCl Nuclei…..~10 -14 m across, protons determine the chemical element (Z); neutron number (N) determines the mass, (A = N+Z). > 99.9 % of the mass of the atom is in the nucleus. Nucleons (protons and neutrons ~10 -15 m) have a substructure, three quarks in each nucleon (‘ups’ and ‘downs’)…but they don’t exists on their own.
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Mendeleyev
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Moseley’s Law….evidence for Atomic numbers…. ‘Characteristic’ X-rays…with a chemical (Z) dependence
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Z=43 Tc Z=61 Pm Z=84 Po Elemental composition of the Solar Nebula
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Figure Wiescher, Regan & Aprahamian, Physics World Feb. 2002, page 33-38 Slow-neutron capture process allows formation of elements from A~56 to A=209 (Bi)... terminates at 209 Bi...why?
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X-rays come from atomic ‘vacancies’ i.e. holes in the electron shells around the atom. Quantum mechanics means that the electron orbits are fixed in energy…. X-rays come from an electron ‘dropping’ from one energy level to a lower one
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X-rays come from atomic ‘vacancies’ i.e. holes in the electron shells around the atom. Quantum mechanics means that the electron orbits are fixed in energy…. X-rays come from an electron ‘dropping’ from one energy level to a lower one
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X-rays come from atomic ‘vacancies’ i.e. holes in the electron shells around the atom. Quantum mechanics means that the electron orbits are fixed in energy…. X-rays come from an electron ‘dropping’ from one energy level to a lower one X-ray emitted
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Spectral Maps of the Galaxy Ref http://adc.gsfc.nasa.gov/mw/mmw_images.html
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Full-sky Comptel map of 1.8 MeV gamma rays in 26 Mg following 26 Al -decay. Nuclear reactions are taking place continually around the galaxy. Radioactive 26 Al around the Galaxy…. Diehl et al., Astron. Astrophys 97, 181 (1993)
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Chart of the Nuclei 1H1H 2D2D 3 He 4 He 6 Li 7 Li n 9 Be 3T3T 6 He 5 Li 6 Be 7 Be 8 Li 9 Li 10 Be 10 Li 11 Li 8 He 11 Be 12 Be 10 B 11 B 9B9B 14 Be 12 B 13 B 14 B 15 B 8B8B 7B7B 12 C 13 C 14 C 15 C 16 C 17 C 11 C 10 C 9C9C Z = No. of Protons 0 1 2 3 4 5 6 N = No. of Neutrons 012345 6789
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Chart of the Nuclei The Landscape ~300 stable ~ 7000 unstable … radioactive.
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What makes a nucleus ‘stable’? There is an ongoing interplay and competition between coulomb repulsion and strong nuclear force interactions The result is that only certain combinations of Z and N give rise to stable configurations (about 300 in total). Other non-stable types can ‘radioactively decay’ (about 7,000 predicted).
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23 Radiation in our Environment We are all constantly subject to irradiation mainly from natural sources. There are three main sources of such radiation. a) Primordial -around since the creation of the Earth ( 4.5 x 10 9 years) 235,8 U ( and daughters including 210 Po), 232 Th or 40 K (+ 87 Rb, 138 La and others....) b) Cosmogenic – from interaction of Cosmic rays with Earth and atmosphere. 14 C, 7 Be formed from cosmic ray interactions. Cosmic rays are mostly protons. c) Produced or enhanced by human activity. Medical or dental X-rays; 137 Cs (product from nuclear fission, 239 Pu, 241 Am, 239 Pu from weapons fallout
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24 From NRPB-Average Radiation Dose in UK NRPB is now HPA-RPD
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25 Radioactive species in the body Isotope Average amount by weightActivity U-Uranium 90μg 1.1Bq Th-Thorium 30 μg 0.11Bq 40 K 17mg 4.4 kBq Ra 31pg 1.1Bq 14 C 22ng 3.7kBq 3 H-tritium 0.06pg 23Bq Po-Polonium 0.2pg 37Bq Some variation- for example smokers have 4-5 times more Po.
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Z=43 Tc Z=61 Pm Z=84 Po Elemental composition of the Solar Nebula
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How it all starts….Hydrogen (Z=1) to Helium (Z=2) The Proton-Proton Chain
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Nuclear Fusion creates energy up to A~56 (Z=26 = Iron) If the star is hot enough, nuclear fusion will fuel the star and create elements up to A~56
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Figure Wiescher, Regan & Aprahamian, Physics World Feb. 2002, page 33-38 Slow-neutron capture process allows formation of elements from A~56 to A=209 (Bi)... terminates at 209 Bi...why?
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Once you have 4 He what next? 4 He + H → 5 Li not energetically allowed…neither is 4 He+ 4 He → 8 Be…we’re stuck with A=1,2,3 and 4…. BUT!!! 4 He can fuse with 2 other 4 He ( 8 Be) stuck together for a short time (~10 -16 sec) to make 12 C…complicated but understood. Once we have made 12 C (Z=6) nuclei can fuse together and gain energy (if the star is hot and massive enough) to make all elements up to Z=26 (Iron=Fe).
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B ~1.5 MeV per A
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Once you have 56 Fe what next? Top of the binding energy per nucleon curve reached at A~56…fusion above this costs energy…bad news for the star - supernova BUT elements from 27-92 exist in nature – how are these made ? Neutron Capture – neutrons have no charge – no electrostatic repulsion.
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Figure Wiescher, Regan & Aprahamian, Physics World Feb. 2002, page 33-38 Slow-neutron capture process allows formation of elements from A~56 to A=209 (Bi)... terminates at 209 Bi...why?
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Figure Wiescher, Regan & Aprahamian, Physics World Feb. 2002, page 33-38 Slow-neutron capture process allows formation of elements from A~56 to A=209 (Bi)... terminates at 209 Bi...why? Neutron capture… no electrostatic barrier to nuclear fusion…. all you need are enough Neutrons…
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Beta –radioactive decay, (consequence of E=mc 2 ) 2 types: (i) Beta- plus proton changes to a neutron (Z ->Z-1) (ii) Beta – minus neutron changes to a proton (Z -> Z+1)
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Nuclear reactions in Red giant stars create ‘spare’ neutrons Stellar neutron sources in the middle of Red Giant stars (e.g., Betelguese) 13 C+ 4 He→ 17 O*→ 16 O + n 22 Ne+ 4 He → 26 Mg*→ 25 Mg + n
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So, how do you make Gold ? Gold has 79 protons (i.e. Z=79) Start with Z=78 protons (i.e. Platinum) Specifically 196 Pt ( Pt = Z=78, N=196-78=118) Reaction is 196 Pt + neutron to make 197 Pt 197 Pt is radioactive and ‘beta-decays’ to make 197 Au (i.e., normal ‘stable’ gold).
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S-process makes 209 Bi from 208 Pb+n → 209 Pb (T 1/2 =3.2hr) → 209 Bi Neutron capture on stable 209 Bi → 210 Bi (T 1/2 =5 days) → 210 Po. 210 Po → + 206 Pb (stable nucleus, as is 207 Pb and 208 Pb) Polonium-210 ‘terminates’ the period table at Bi (via the s-process)
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Q 210 Pb) = 5.41 MeV E = 5.30 MeV E( 206 Pb) = 0.11 MeV T1/2 = 138 days. ‘ 218 Po =Radium A’ ‘ 218 At =Radium B’ C D E 210 Po =Radium ‘F’ Radon =‘Emanation’ ‘Radium’ C’ C’’ The Natural Decay Chain for 238 U BUT: Evidently, heavier (radioactive) elements like Th (Z=90) ; U (Z=92) exist ? How are they made?
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= 214 Pb = 214 Bi
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SN1987a before and after !!
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A=N+Z = fixed
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48 For a give fixed A (isobar), we have different combinations of Z and N. e.g., A=Z+N=137 can be from Z=56, N=81 → 137 Ba 81 ; or Z=55, N=82 → 137 Cs 82 (see later)… Mass Parabolas and Radioactive Decays A = constant
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Example of a mass parabola Mass energy (mc 2 ) A=N+Z=125 p → n + + + 125 Xe : Z=54; N=71 125 Cs : Z=55; N=70 125 I : Z=53; N=72 125 Ba : Z=56; N=69 125 Te : Z=52; N=73 STABLE ISOBAR FOR A=125 125 In : Z=49 125 Sn : Z=50; 125 Sb : Z=51; n → p + - +
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Figure Wiescher, Regan & Aprahamian, Physics World Feb. 2002, page 33-38 Slow-neutron capture process allows formation of elements from A~56 to A=209 (Bi)... terminates at 209 Bi...why?
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Summary What’s made where and how. –Hydrogen to Helium (in the sun, p-p chain CNO cycles). –Helium to Carbon, triple-alpha process, special fusion. –Carbon to iron: nuclear fusion reactions, if hot enough. –Above 56 Fe, (a) up to Z=92, 238 U, supernova, rapid neutron captures...also spits out material for future neutron capture in 2 nd / 3 rd generation star (b) can get up to 209 Bi ( 210 Po end-point) by slow neutron capture
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