02691nam 2200685 a 450 991078088610332120220117132744.01-283-14351-89786613143518981-279-066-7(CKB)2490000000001925(EBL)731327(OCoLC)738438002(SSID)ssj0000544424(PQKBManifestationID)12232502(PQKBTitleCode)TC0000544424(PQKBWorkID)10536288(PQKB)10356110(SSID)ssj0000639194(PQKBManifestationID)11403982(PQKBTitleCode)TC0000639194(PQKBWorkID)10604542(PQKB)11039480(MiAaPQ)EBC731327(WSP)00006721(Au-PeEL)EBL731327(CaPaEBR)ebr10480235(CaONFJC)MIL314351(PPN)182038688(EXLCZ)99249000000000192520110228e20101970 uy 0engur|n|---|||||txtccrNuclear collective motion[electronic resource] models and theory /David J. RoweSingapore ;Hackensack, N.J. World Scientific Pub. Co.c20101 online resource (250 p.)"The first edition was published by Methuen in 1970."--t.p. verso.981-279-065-9 981-279-064-0 Includes bibliographical references and index.pt. 1. Phenomenological models -- pt. 2. Microscopic theories.The two most important developments in nuclear physics were the shell model and the collective model. The former gives the formal framework for a description of nuclei in terms of interacting neutrons and protons. The latter provides a very physical but phenomenological framework for interpreting the observed properties of nuclei. A third approach, based on variational and mean-field methods, brings these two perspectives together in terms of the so-called unified models. Together, these three approaches provide the foundations on which nuclear physics is based. They need to be understood by eMany-body problemNuclear collective modelsNuclear spectroscopyMany-body problem.Nuclear collective models.Nuclear spectroscopy.539.74Rowe D. J(David J.)1573771MiAaPQMiAaPQMiAaPQBOOK9910780886103321Nuclear collective motion3849659UNINA