First Study of EC/β+ Decay Schemes for Neutron-Deficient Isotopes 153Er and 157Yb

  • 153Er and 157Yb were produced via xu fusion-evaporation reaction by irradiation of 142Nd and 147Sm with 16O, respectively. A He-jet recoil tape transport system, X-γ and γ-γ coincidence measurements were employed to separate and identify the reaction products and to study the EC/β+ decay of 153Er and 157Yb. The EC/β+ decay schemes of 153Er and 157Yb have been proposed for the first time, from which a new three qussi-particle state and two new single proton states have been assigned to 153Ho, and a new isomer and a new rotational band have been assigned to 157Tm. According to systematic behaviour of the low-laying energy levels for odd holmium and odd thulium isotopes with N=82-102, it can be seen that the change from spherical to deformed shapes of nuclear ground states in the two isotope chains appears between N=86 and 88.
  • [1] J.D.Bowman,R.E.EPPley,E.K.Hyde,Phys.Rev.,C25(1982)941.[2]E.Hagberg,P.G.Hansen,J.C.Hardy et al.,Nucl.Phys.,A293(1977)1.[3]M.A.Lee,Nucl.Data.Sheets,60(1990)513.[4]R.Neugart et al.,5thInt.Conf.on Nuclei far from Stability,Rosseau Lake,Canada,p.126(1988).[5]M.A.Lee,Nucl.Data Sheets,60(1990)509.[6]M.H.Rafailovich,O.C.Kistner,A.W.Sunyar et al.,Phys.Rev.,C30(1984)169.[7]C.Ekstrom,L.Robertsson et al.,Z.Phys.,A316(1984)239.[8]G.Andi,A.H.Wapstra,Nucl.Phys.,A565(1993)1.[9]R.Kossakowski,J.Jastzebski,P.Rymuza et al.,Phys.Rev.,C32(1985)1612.[10]M.A.RILEY,C.Baktash,Y.A.Ellis-Akovali et al.,Argonne National Laboratory Report,ANL-PHY-88-2,1988.[11]K.S.Toth,C.R.Bingham,W.D.Schmidt-ott,Phys.Rev.,C10(1974)1550.[12]L.Kh.Batist et al.,Izv.Akad.Nauk SSSR Ser.Fiz.,46(1982)2200.[13]袁双贵、徐树威、张学谦等,核技术,16(8)(1993)475.[14]徐树威、王以好、罗亦孝等,He-jet带传输及X-γ(t)符合测量装置和153Er(EC+β+)衰变新γ的测定,核技术,(1995)待发表。[15]XuShuwei,XieYuanxiang,PanQiangyan et al.,The(EC+β+)decay of 153Er,Z.Phys.,A350(1994)187.[16]XuShuwei,XieYuanxiang,PanQiangyan et al.,(EC+β+)decay of 157Yb,Phys.Rev.,C50,No6(1994).[17]N.B.Gove,M.J.Martin,Nucl.Data Tables,10(1971)206.[18]R.B.Firestone,J.M.Nitchke,P.A.Wilmarth et al.,Phys.Rev.,C39(1989)219.[19]K.S.Tothetal.,Phys.Rev.,C44(1991)1868.[20]R.Barden,A.Plochocki,D.Schardt et al.,Z.Phys.,A329(1988)11.[21]W.Meczynski,K.Zuber,R.Broda et al.,Programme and Abstracts of 6th Int.Conf.on Nucl.far from Stability,PE34(1992)[22]P.C.Sood and R.K.Sheline,Atomic Data and Nucl ear Data Tables,43(1989)259.[23]K.S.Toth et al.,Phys.Rev.,C32(1985)342.[24]G.D.Alkhazov,A.E.Barzakh,I.Ya.Chubukov et al.,Nucl.Phys.,A477(1988)37.[25]A.K.Jain,R.K.Sheline,P.C.Sood et al.,Rev.Mod.Phys,62(1990)393.[26]P.Kleibeinz,B.Rubio,M.Oyawa et al.,Z.Phys.,A322(1985)705.[27]M.O.Kortelahtic,K.S.Toth,K.S.Vierinen et al.,Phys.Rev.,C39(1989)636.[28]A.V.Potempa et al.,Izv.Akad.Nauk.SSSR Ser.Fiz.,54(1990)852.
  • [1] J.D.Bowman,R.E.EPPley,E.K.Hyde,Phys.Rev.,C25(1982)941.[2]E.Hagberg,P.G.Hansen,J.C.Hardy et al.,Nucl.Phys.,A293(1977)1.[3]M.A.Lee,Nucl.Data.Sheets,60(1990)513.[4]R.Neugart et al.,5thInt.Conf.on Nuclei far from Stability,Rosseau Lake,Canada,p.126(1988).[5]M.A.Lee,Nucl.Data Sheets,60(1990)509.[6]M.H.Rafailovich,O.C.Kistner,A.W.Sunyar et al.,Phys.Rev.,C30(1984)169.[7]C.Ekstrom,L.Robertsson et al.,Z.Phys.,A316(1984)239.[8]G.Andi,A.H.Wapstra,Nucl.Phys.,A565(1993)1.[9]R.Kossakowski,J.Jastzebski,P.Rymuza et al.,Phys.Rev.,C32(1985)1612.[10]M.A.RILEY,C.Baktash,Y.A.Ellis-Akovali et al.,Argonne National Laboratory Report,ANL-PHY-88-2,1988.[11]K.S.Toth,C.R.Bingham,W.D.Schmidt-ott,Phys.Rev.,C10(1974)1550.[12]L.Kh.Batist et al.,Izv.Akad.Nauk SSSR Ser.Fiz.,46(1982)2200.[13]袁双贵、徐树威、张学谦等,核技术,16(8)(1993)475.[14]徐树威、王以好、罗亦孝等,He-jet带传输及X-γ(t)符合测量装置和153Er(EC+β+)衰变新γ的测定,核技术,(1995)待发表。[15]XuShuwei,XieYuanxiang,PanQiangyan et al.,The(EC+β+)decay of 153Er,Z.Phys.,A350(1994)187.[16]XuShuwei,XieYuanxiang,PanQiangyan et al.,(EC+β+)decay of 157Yb,Phys.Rev.,C50,No6(1994).[17]N.B.Gove,M.J.Martin,Nucl.Data Tables,10(1971)206.[18]R.B.Firestone,J.M.Nitchke,P.A.Wilmarth et al.,Phys.Rev.,C39(1989)219.[19]K.S.Tothetal.,Phys.Rev.,C44(1991)1868.[20]R.Barden,A.Plochocki,D.Schardt et al.,Z.Phys.,A329(1988)11.[21]W.Meczynski,K.Zuber,R.Broda et al.,Programme and Abstracts of 6th Int.Conf.on Nucl.far from Stability,PE34(1992)[22]P.C.Sood and R.K.Sheline,Atomic Data and Nucl ear Data Tables,43(1989)259.[23]K.S.Toth et al.,Phys.Rev.,C32(1985)342.[24]G.D.Alkhazov,A.E.Barzakh,I.Ya.Chubukov et al.,Nucl.Phys.,A477(1988)37.[25]A.K.Jain,R.K.Sheline,P.C.Sood et al.,Rev.Mod.Phys,62(1990)393.[26]P.Kleibeinz,B.Rubio,M.Oyawa et al.,Z.Phys.,A322(1985)705.[27]M.O.Kortelahtic,K.S.Toth,K.S.Vierinen et al.,Phys.Rev.,C39(1989)636.[28]A.V.Potempa et al.,Izv.Akad.Nauk.SSSR Ser.Fiz.,54(1990)852.
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Xu Shuwei, Xie Yuanxiang, Pan Qiangyan, Zhang Juping, Zhang Xueqian, Wang Yihao, Ge Yuanxiu, Yin Xijin, Wang Chunfang, Zhang Tianmei, Liu Zhong, Guo Bing, Luo Yixiao, Xing Zheng and Chen Xingqu. First Study of EC/β+ Decay Schemes for Neutron-Deficient Isotopes 153Er and 157Yb[J]. Chinese Physics C, 1995, 19(3): 193-202.
Xu Shuwei, Xie Yuanxiang, Pan Qiangyan, Zhang Juping, Zhang Xueqian, Wang Yihao, Ge Yuanxiu, Yin Xijin, Wang Chunfang, Zhang Tianmei, Liu Zhong, Guo Bing, Luo Yixiao, Xing Zheng and Chen Xingqu. First Study of EC/β+ Decay Schemes for Neutron-Deficient Isotopes 153Er and 157Yb[J]. Chinese Physics C, 1995, 19(3): 193-202. shu
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First Study of EC/β+ Decay Schemes for Neutron-Deficient Isotopes 153Er and 157Yb

    Corresponding author: Xu Shuwei,
  • Institute of Modern Physics, The Chinese Academy of Sciences, Lanzhou, 7300001 Department of Modern Physics, Lanzhou University, Lanzhou 730000

Abstract: 153Er and 157Yb were produced via xu fusion-evaporation reaction by irradiation of 142Nd and 147Sm with 16O, respectively. A He-jet recoil tape transport system, X-γ and γ-γ coincidence measurements were employed to separate and identify the reaction products and to study the EC/β+ decay of 153Er and 157Yb. The EC/β+ decay schemes of 153Er and 157Yb have been proposed for the first time, from which a new three qussi-particle state and two new single proton states have been assigned to 153Ho, and a new isomer and a new rotational band have been assigned to 157Tm. According to systematic behaviour of the low-laying energy levels for odd holmium and odd thulium isotopes with N=82-102, it can be seen that the change from spherical to deformed shapes of nuclear ground states in the two isotope chains appears between N=86 and 88.

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