Presentation is loading. Please wait.

Presentation is loading. Please wait.

218 Po ‘ 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 Aside: information.

Similar presentations


Presentation on theme: "218 Po ‘ 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 Aside: information."— Presentation transcript:

1

2 218 Po

3 ‘ 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 Aside: information here is used extensively in environmental monitoring; + radioactive dating – age of the earth ~10 9 yrs…evidence for evolution....

4

5 ‘Nuclei = combinations of protons (Z) and neutrons (N). Chart of the Nuclides = a ‘2-D’ periodic table…… <300 of the (Z,N) combinations are stable and make up’everyday’ atoms. ~7,000 other combinations are unstable nuclei. Most energetically stable nuclei in the middle, More exotic, unstable nuclei at the edges ….

6

7

8 For a ‘typical’ nucleus, Nuclear Volume  A (= number of protons and neutrons) Since for a sphere, V = 4  R 3 /3 Thus nuclear radius, R  A 1/3  R = (1.2 x m) A 1/3 Rutherford Scattering experiments showed this relation to hold for all nuclei studied….so what’s new to learn…. Then… 1985 – the strange case of ‘Lithium -11’ (note stable lithium isotopes are Lithium-6 and Lithium-7)

9 The probability of a beam of ‘neutron-rich’ lithium-11 isotopes colliding on carbon target was much larger than expected…(remind you of anything?)… Lithium beam target detector

10 Nuclear ‘halos’ and Borromean Nuclei…. Nuclear ‘halos’ and Borromean Nuclei…. J.S. Al-Khalili & J.A. Tostevin, Phys. Rev. Lett. 76 (1996) 3903 Halo nuclei are examples of ‘Borromean’ systems, only bound with three Interactions…remove any one and the other two fall apart….

11 4n4n 4n4n Borromean Halo states tetraneutron Proton dripline

12 What about ‘inside’ the nucleus (i.e. nuclear ‘structure’) ? Can we see ‘inside’ the nucleus ? What does it tell us?

13

14 Euroball IV at Strasbourg

15 The 12 valence particles move in equatorial orbits, driving the nucleus to an oblate shape! 158 Er at ‘High Spins’ from Daresbury Lab

16 Rotations in the Universe Revolutions/sec Typical size (cm)

17 How Far Can We Go ? What is the heaviest element ? What are the ‘nuclear limits’ ? How are the heavier elements formed ?

18 Super Heavy Elements? Rutherford worked with decays from Thorium and Uranium the heaviest element (Z=90 & 92) known at the time. He inferred their presence and other elements in their decay chains by characteristic alpha decay sequences….

19

20 Elements Z=116 and 118 discovered from fusion of Calcium ions on radioactive targets of Californium and Curium (Oganessian et al., Phys. Rev. C74 (2006) ). Periodic table has increased by 26 elements since Rutherford’s work on Uranium and Thorium decays.

21 K-electrons L-electrons T1/2 = 10.4 s 205 Au Pt How are the heavy elements made ? Is it via the Rapid Neutron Capture (R-) Process ? Many of the nuclei which lie on the r-process predicted path have yet to be studied. Do these radioactive nuclei act as we expect ?

22 Evidence for nuclear shell structure….. energy of 1 st excited state in even-even nuclei….E(2 + ). What do we expect ?

23 large gaps in single-particle structure of nuclei…MAGIC NUMBERS = ENERGY GAPS

24 A (big!) problem, can’t reproduce the observed elemental abundances. We can ‘fix’ the result by changing the shell structure (i.e. changing the magic numbers)….but is this scientifically valid ? N=126 N=82 Need to look at N=82 and 126 ‘exotic’ nuclei in detail….

25 Turning Lead into Gold and Platinum….

26 Facility for Anti-Proton and Ion Research (FAIR) To be constructed at the current GSI site, near Darmstadt, Germany Will bring currently ‘theoretical nuclear species’ into experimental reach for the first time.

27 (some) Nuclear Physics Research c Nuclei comprise 99.9% of all matter we can see in the Universe and are the fuel that burns in stars. A comprehensive description of nuclei requires theoretical and experimental investigations of rare isotopes with unusual neutron-to-proton ratios. These nuclei are labeled exotic, or rare, because they are not typically found on Earth. They are difficult to produce because they usually have extremely short lifetimes. The goal of a comprehensive description and reliable modeling of all nuclei represents one of the great intellectual opportunities for physics in the twenty-first century.

28 (‘Big’) Physics Questions from the STFC Nuclear Physics Advisory Panel What is the Nature of Nuclear Matter? What are the limits of nuclear existence? How do simple patterns emerge in complex nuclei? Can nuclei be described in terms of our understanding of the underlying fundamental interactions? What is the equation-of-state of nuclear matter? How does the ordering of quantum states change in extremely unstable nuclei? Are there new forms of structure and symmetry at the limits of nuclear existence? What are the Origins of the Elements? How, and where, were the heavy elements synthesised? What are the key reaction processes that drive explosive astrophysical events such as supernovae, and X-ray bursts? What is the equation-of-state of compact matter in neutron stars? What are the nuclear processes, and main astrophysical sites, that produce the γ-ray emitting radionuclides observed in our galaxy? How do nuclear reactions influence the evolution of massive stars, and how do they contribute to observed elemental abundances?


Download ppt "218 Po ‘ 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 Aside: information."

Similar presentations


Ads by Google