Matches in SemOpenAlex for { <https://semopenalex.org/work/W2021982171> ?p ?o ?g. }
- W2021982171 endingPage "014007" @default.
- W2021982171 startingPage "014007" @default.
- W2021982171 abstract "I overview new aspects of the structure of exotic nuclei as compared to stable nuclei, focusing on several characteristic effects of nuclear forces. The shell structure of nuclei has been proposed by Mayer and Jensen, and has been considered to be kept valid basically for all nuclei, with well-known magic numbers, 2, 8, 20, 28, 50, .... Nuclear forces were shown, very recently, to change this paradigm. It will be presented that the evolution of shell structure occurs in various ways as more neutrons and/or protons are added, and I will present basic points of this shell evolution in terms of the monopole interaction of nuclear forces. I will discuss three types of nuclear forces. The first one is the tensor force. The tensor force is one of the most fundamental nuclear forces, but its first-order effect on the shell structure has been clarified only recently in studies on exotic nuclei. The tensor force can change the spin–orbit splitting depending on the occupation of specific orbits. This results in changes of the shell structure in many nuclei, and consequently some of Mayer–Jensen's magic numbers are lost and new ones emerge, in certain nuclei. This mechanism can be understood in an intuitive way, meaning that the effect is general and robust. The second type of nuclear forces is central force. I will show a general but unknown property of the central force in the shell-model Hamiltonian that can describe nuclear properties in a good agreement with experiment. I will then demonstrate how it can be incorporated into a simple model of the central force, and will discuss how this force works in the shell evolution. Actually, by combining this central force with the tensor force, one can understand and foresee how the same proton–neutron interaction drives the shell evolution, for examples such as Sn/Sb isotopes, N = 20 nuclei and Ni/Cu isotopes. The distribution of single-particle strength is discussed also in comparison to (e,e'p) experiment on 48Ca. The shell evolution affects shapes of nuclei through Jahn–Teller-type mechanism, and a very interesting example with exotic Si isotopes is discussed. The third type of nuclear force is a three-body force, which originates in the Δ particle excitation as proposed by Fujita and Miyazawa many years ago. This force is shown to produce a repulsive interaction between valence neutrons after averaging effects from the third nucleon in the core. The same three-body force is responsible for neutron stars. By including such effects of the three-body force, one can predict the correct drip line of oxygen isotopes, for instance. Thus, the landscape of atomic nuclei varies in going from stable to exotic nuclei due to particular nuclear forces, leading to a paradigm shift. This paper overviews some basic ideas and selected examples." @default.
- W2021982171 created "2016-06-24" @default.
- W2021982171 creator A5036770921 @default.
- W2021982171 date "2013-01-01" @default.
- W2021982171 modified "2023-09-30" @default.
- W2021982171 title "Exotic nuclei and nuclear forces" @default.
- W2021982171 cites W1494985844 @default.
- W2021982171 cites W1508073480 @default.
- W2021982171 cites W1581078709 @default.
- W2021982171 cites W171395355 @default.
- W2021982171 cites W1966781496 @default.
- W2021982171 cites W1967184079 @default.
- W2021982171 cites W1968164765 @default.
- W2021982171 cites W1968203672 @default.
- W2021982171 cites W1968361397 @default.
- W2021982171 cites W1968986208 @default.
- W2021982171 cites W1973859166 @default.
- W2021982171 cites W1976905288 @default.
- W2021982171 cites W1980384226 @default.
- W2021982171 cites W1981267267 @default.
- W2021982171 cites W1982823307 @default.
- W2021982171 cites W1983767566 @default.
- W2021982171 cites W1985083812 @default.
- W2021982171 cites W1985289694 @default.
- W2021982171 cites W1985867665 @default.
- W2021982171 cites W1986616937 @default.
- W2021982171 cites W1987478715 @default.
- W2021982171 cites W1988500848 @default.
- W2021982171 cites W1995969332 @default.
- W2021982171 cites W1999050968 @default.
- W2021982171 cites W2001232237 @default.
- W2021982171 cites W2002541882 @default.
- W2021982171 cites W2005599087 @default.
- W2021982171 cites W2006489109 @default.
- W2021982171 cites W2008670282 @default.
- W2021982171 cites W2009300342 @default.
- W2021982171 cites W2011103011 @default.
- W2021982171 cites W2014179689 @default.
- W2021982171 cites W2016955605 @default.
- W2021982171 cites W2019030058 @default.
- W2021982171 cites W2019293116 @default.
- W2021982171 cites W2020062860 @default.
- W2021982171 cites W2021953538 @default.
- W2021982171 cites W2022789202 @default.
- W2021982171 cites W2023156807 @default.
- W2021982171 cites W2031219985 @default.
- W2021982171 cites W2035368781 @default.
- W2021982171 cites W2035770865 @default.
- W2021982171 cites W2038272968 @default.
- W2021982171 cites W2038785435 @default.
- W2021982171 cites W2038953989 @default.
- W2021982171 cites W2043179386 @default.
- W2021982171 cites W2045019917 @default.
- W2021982171 cites W2046721419 @default.
- W2021982171 cites W2048335927 @default.
- W2021982171 cites W2049983086 @default.
- W2021982171 cites W2051307589 @default.
- W2021982171 cites W2052520318 @default.
- W2021982171 cites W2054493526 @default.
- W2021982171 cites W2055588731 @default.
- W2021982171 cites W2059408344 @default.
- W2021982171 cites W2059823880 @default.
- W2021982171 cites W2067220891 @default.
- W2021982171 cites W2068195353 @default.
- W2021982171 cites W2072487485 @default.
- W2021982171 cites W2073462286 @default.
- W2021982171 cites W2076779267 @default.
- W2021982171 cites W2076908219 @default.
- W2021982171 cites W2077215465 @default.
- W2021982171 cites W2077522560 @default.
- W2021982171 cites W2078855286 @default.
- W2021982171 cites W2079449508 @default.
- W2021982171 cites W2080421281 @default.
- W2021982171 cites W2082663968 @default.
- W2021982171 cites W2085177067 @default.
- W2021982171 cites W2086456920 @default.
- W2021982171 cites W2086604678 @default.
- W2021982171 cites W2092786290 @default.
- W2021982171 cites W2093845677 @default.
- W2021982171 cites W2095270951 @default.
- W2021982171 cites W2096937309 @default.
- W2021982171 cites W2104667842 @default.
- W2021982171 cites W2111331220 @default.
- W2021982171 cites W2111746204 @default.
- W2021982171 cites W2119375674 @default.
- W2021982171 cites W2123521731 @default.
- W2021982171 cites W2125840978 @default.
- W2021982171 cites W2126261149 @default.
- W2021982171 cites W2135700676 @default.
- W2021982171 cites W2139326510 @default.
- W2021982171 cites W2146406469 @default.
- W2021982171 cites W2148936717 @default.
- W2021982171 cites W2154894801 @default.
- W2021982171 cites W2157581223 @default.
- W2021982171 cites W2167885013 @default.
- W2021982171 cites W2172167594 @default.
- W2021982171 cites W2226171111 @default.
- W2021982171 cites W2237990622 @default.