<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">465809308</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180323112111.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">170327e19900101xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1007/BF02902623</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)springer-10.1007/BF02902623</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">On the interactions between nucleons in the valence shells of trans-208Pb nuclei</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[G. Mouze, C. Ythier]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">Summary: A lot of information concerning the interaction laws between nucleons in the valence shells of trans-208Pb nuclei can be obtained from experimental mass tables. The proton-neutron interaction energy can be expressed by $$E_{np} = N_p N_n \varepsilon '_{np} $$ , whereN p N n is the number of n-p couples in the valence shells, and $$\varepsilon '_{np} $$ a weak, nearly constant interaction energy per n-p couple. Two methods are proposed for the calculation ofE np. In even-even nuclei, the integral 2p-2p interaction energy is given by $$E_{2p - 2p} = - \mathcal{N}_p (\mathcal{N}_p - 1)\varepsilon _{2p - 2p} /2$$ , where $$\mathcal{N}_p $$ is the number of proton pairs, and $$\varepsilon _{2p - 2p} $$ a weak, nearly constant interaction energy per 2p-2p couple. A similar relation holds for valence neutron pairs. The energy binding all the valence proton pairs to the208Pb core is $$\mathcal{N}_p \bar \sigma _{2p} $$ , where $$\bar \sigma _{2p} $$ is calculable in a simple way fromZ=84 toZ=92; its value is independent of the number of pairs of nucleons of the other kind in the valence shells. A similar relation holds for valence neutron pairs. Similar laws hold in odd nuclei. The weakness of all these valence shell interaction energies, and the fact that the energy binding an unpaired proton to the208Pb core of odd-Z nuclei decreases rapidly as $$\mathcal{N}_p $$ increases, explain several properties, which are briefly discussed, of trans-208Pb nuclei: repulsion between valence neutrons, feasibility of Oganessian reactions, shell internal energy, and reactivity of the valence nucleons.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">Società Italiana di Fisica, 1990</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">21.10 - General and average properties of nuclei</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">25.40 - Nucleon-induced reactions</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Mouze</subfield>
   <subfield code="D">G.</subfield>
   <subfield code="u">Laboratoire de Chimie Atomique, Faculté des Sciences, 06 034, Nice, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Ythier</subfield>
   <subfield code="D">C.</subfield>
   <subfield code="u">Laboratoire de Chimie Atomique, Faculté des Sciences, 06 034, Nice, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Il Nuovo Cimento A (1965-1970)</subfield>
   <subfield code="d">Società Italiana di Fisica</subfield>
   <subfield code="g">103/1(1990-01-01), 105-128</subfield>
   <subfield code="q">103:1&lt;105</subfield>
   <subfield code="1">1990</subfield>
   <subfield code="2">103</subfield>
   <subfield code="o">40763</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1007/BF02902623</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="908" ind1=" " ind2=" ">
   <subfield code="D">1</subfield>
   <subfield code="a">research-article</subfield>
   <subfield code="2">jats</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">856</subfield>
   <subfield code="E">40</subfield>
   <subfield code="u">https://doi.org/10.1007/BF02902623</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Mouze</subfield>
   <subfield code="D">G.</subfield>
   <subfield code="u">Laboratoire de Chimie Atomique, Faculté des Sciences, 06 034, Nice, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Ythier</subfield>
   <subfield code="D">C.</subfield>
   <subfield code="u">Laboratoire de Chimie Atomique, Faculté des Sciences, 06 034, Nice, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">773</subfield>
   <subfield code="E">0-</subfield>
   <subfield code="t">Il Nuovo Cimento A (1965-1970)</subfield>
   <subfield code="d">Società Italiana di Fisica</subfield>
   <subfield code="g">103/1(1990-01-01), 105-128</subfield>
   <subfield code="q">103:1&lt;105</subfield>
   <subfield code="1">1990</subfield>
   <subfield code="2">103</subfield>
   <subfield code="o">40763</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="898" ind1=" " ind2=" ">
   <subfield code="a">BK010053</subfield>
   <subfield code="b">XK010053</subfield>
   <subfield code="c">XK010000</subfield>
  </datafield>
  <datafield tag="949" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="F">NATIONALLICENCE</subfield>
   <subfield code="b">NL-springer</subfield>
  </datafield>
 </record>
</collection>
