References quoted in the ENSDF dataset: 55ZN ADOPTED LEVELS

19 references found.

Clicking on a keynumber will list datasets that reference the given article.

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1991DE26

Z.Phys. A340, 227 (1991)

C.Detraz

The Branching Ratio of β-Delayed Two-Proton Emission

RADIOACTIVITY ²²Al, ^22,23Si, ²⁶P, ²⁷S, ³¹Ar, ³⁵Ca, ³⁹Ti, ⁴³Cr, ⁴⁶Mn, ^46,47Fe, ^49,50,51Ni, ⁵⁵Zn; calculated β-delayed one-, two-proton emission probability ratios. Compound nucleus decay.

1997OR04

Phys.Rev. C55, 2407 (1997)

W.E.Ormand

Mapping the Proton Drip Line up to A = 70

NUCLEAR STRUCTURE ^46,47,48Mn, ^46,47,48,49Fe, ^{47,48,49,50,51,52}Co, ^{49,50,51,52,53}Ni, ^{49,50,51,52,53,54,55,56}Cu, ^{50,52,53,54,55,56,57}Zn, ^{54,55,56,57,58,59,60,61}Ga, ^{56,57,58,59,60,61,62,63}Ge, ^{58,59,60,61,62,63,64,65}As, ^{62,63,64,65,66,67}Se, ^{65,66,67,68,69}Br, ^66,67,68,69Kr, ^68,70Rb; calculated binding energy, one-, two-proton separation energy, β-decay endpoint energy, Q(EC). ³⁸Ti, ⁴⁵Fe, ^48,49Ni, ⁵⁵Zn, ⁵⁹Ge, ^63,64Se, ^66,67,68,69Kr; calculated di-proton emission T_1/2, one-, two-proton separation energies. Coulomb energy difference from shell model.

doi: 10.1103/PhysRevC.55.2407

2001FI23

At.Data Nucl.Data Tables 79, 241 (2001)

J.L.Fisker, V.Barnard, J.Gorres, K.Langanke, G.Martinez-Pinedo, M.C.Wiescher

Shell Model Based Reaction Rates for rp-Process Nuclei in the Mass Range A = 44-63

NUCLEAR REACTIONS ^44,45,46Ti, ^45,46,47V, ^{45,46,47,48,49,50}Cr, ^{45,46,47,48,49,50,51,52,53}Mn, ^{50,51,52,53,54,55,56}Fe, ^{50,51,52,53,54,55,56,57}Co, ^{55,56,57,58,59}Ni, ^{54,55,56,57,58,59,60,61}Cu, ^{59,60,61,62,63}Zn, ^{59,60,61,62,63}Ga(p, γ), E not given; calculated astrophysical reaction rates vs temperature.

NUCLEAR STRUCTURE ^45,46,47V, ^46,47,48Cr, ^{46,47,48,49,50,51}Mn, ^{46,47,48,49,50,51,52,53,54}Fe, ^{51,52,53,54,55,56,57}Co, ^{51,52,53,54,55,56,57,58}Ni, ^{56,57,58,59,60}Cu, ^{55,56,57,58,59,60,61,62}Zn, ^{60,61,62,63,64}Ga, ^{60,61,62,63,64}Ge; calculated levels, J, π, decay widths. Shell model.

doi: 10.1006/adnd.2001.0867

2001GI10

Eur.Phys.J. A 11, 247 (2001)

J.Giovinazzo, B.Blank, C.Borcea, M.Chartier, S.Czajkowski, G.de France, R.Grzywacz, Z.Janas, M.Lewitowicz, F.de Oliveira Santos, M.Pfutzner, M.S.Pravikoff, J.C.Thomas

First Observation of ^{55, 56}Zn

NUCLEAR REACTIONS Ni(⁵⁸Ni, X)⁵⁵Zn/⁵⁶Zn, E=74.5 MeV/nucleon; measured σ. Discussed possible decay modes.

doi: 10.1007/s100500170060

2005JI06

Eur.Phys.J. A 25, 29 (2005)

W.Z.Jiang, Z.Z.Ren, T.T.Wang, Y.L.Zhao, Z.Y.Zhu

Relativistic mean-field study for Zn isotopes

NUCLEAR STRUCTURE ^{52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75}Zn; calculated binding energies, radii, deformation. Relativistic mean-field approach.

doi: 10.1140/epja/i2004-10235-1

2006AG14

Phys.Scr. T125, 178 (2006)

M.Aggarwal

Two-proton radioactivity in proton-rich fp shell nuclei at high spin

NUCLEAR STRUCTURE ^45,46Fe, ^48,49,50Ni, ^54,55,56Zn; calculated one- and two-proton separation energies vs spin.

doi: 10.1088/0031-8949/2006/T125/039

2007DO17

Nucl.Phys. A792, 18 (2007)

C.Dossat, N.Adimi, F.Aksouh, F.Becker, A.Bey, B.Blank, C.Borcea, R.Borcea, A.Boston, M.Caamano, G.Canchel, M.Chartier, D.Cortina, S.Czajkowski, G.de France, F.de Oliveira Santos, A.Fleury, G.Georgiev, J.Giovinazzo, S.Grevy, R.Grzywacz, M.Hellstrom, M.Honma, Z.Janas, D.Karamanis, J.Kurcewicz, M.Lewitowicz, M.J.Lopez Jimenez, C.Mazzocchi, I.Matea, V.Maslov, P.Mayet, C.Moore, M.Pfutzner, M.S.Pravikoff, M.Stanoiu, I.Stefan, J.C.Thomas

The decay of proton-rich nuclei in the mass A = 36-56 region

NUCLEAR REACTIONS Ni(⁵⁸Ni, X), E=74.5 MeV/nucleon; measured fragments isotopic yields.

RADIOACTIVITY ^36,37Ca, ^39,40,41Ti, ⁴³V, ^42,43,44,45Cr, ^46,47Mn, ^46,47,48,49Fe, ^50,51Co, ^{49,50,51,52,53}Ni, ⁵⁵Cu, ^55,56Zn(β⁺), (EC), (β⁺p) [from Ni(⁵⁸Ni, X)]; measured T_1/2, β-delayed proton and γ spectra, branching ratios. ^43,45Cr, ⁴⁶Mn, ^46,47,48Fe, ⁵⁰Co, ^50,51,52,53Ni deduced levels. Two-proton decay observed. Comparison with model predictions.

doi: 10.1016/j.nuclphysa.2007.05.004

2012SI16

Int.J.Mod.Phys. E21, 1250076 (2012); Erratum Int.J.Mod.Phys. E22, 1392001 (2013)

D.Singh, G.Saxena

Study of two-proton radioactivity within the relativistic mean-field plus BCS approach

RADIOACTIVITY ³⁸Ti, ⁴²Cr, ⁴⁵Fe, ⁴⁸Ni, ⁵⁵Zn, ⁶⁰Ge, ^63,64Se, ⁶⁸Kr, ⁷²Sr, ⁷⁶Zr(2p); calculated one- and two-proton separation energies, quadrupole deformation parameters, pairing gap, radial wave functions and density distributions. Comparison with available data.

doi: 10.1142/S0218301312500760

2013TI01

Phys.Rev. C 87, 014313 (2013)

J.Tian, N.Wang, C.Li, J.Li

Improved Kelson-Garvey mass relations for proton-rich nuclei

ATOMIC MASSES ⁵Be, ⁶B, ¹³F, ¹⁵Ne, ¹⁸Mg, ^16,17Na, ^19,20,21,22Al, ^21,22,23Si, ^{22,23,24,25,26}P, ^24,25,26,27S, ^{25,26,27,28,29,30}Cl, ^{28,29,30,31,32,33,34}K, ^{27,28,29,30,31}Ar, ^{30,31,32,33,34,35}Ca, ^{31,32,33,34,35,36,37,38}Sc, ^{33,34,35,36,37,38,39}Ti, ^{35,36,37,38,39,40,41,42,43}V, ^{37,38,39,40,41,42,43,44,45}Cr, ^{39,40,41,42,43,44,45,46,47}Mn, ^{41,42,43,44,45,46,47,48,49}Fe, ^{43,44,45,46,47,48,49,50,51,52}Co, ^{45,46,47,48,49,50,51,52,53}Ni, ^{47,48,49,50,51,52,53,54,55,56}Cu, ^{49,50,51,52,53,54,55,56,57}Zn, ⁶⁰Ga, ⁶²Ge, ⁶⁴As, ⁶⁶Se, ⁶⁸Br, ⁷⁰Kr, ⁷²Rb, ⁷⁴Sr; calculated binding energies, mass excess, S_p, S_2p using improved Kelson-Garvey (ImKG) mass relations. Comparison with experimental data for mirror analogs. Predictions of masses for proton-rich nuclides. Discussed diproton emission.

doi: 10.1103/PhysRevC.87.014313

2016ME17

Phys.Rev. C 94, 064313 (2016)

T.J.Mertzimekis

Prediction and evaluation of magnetic moments in T = 1/2, 3/2, and 5/2 mirror nuclei

NUCLEAR MOMENTS A=3-63; ¹³N, ²³Mg, ²⁵Al, ²⁷Si, ²⁹P, ³¹S, ³⁹Ca, ⁴³Ti, ⁴⁵V, ⁴⁹Mn, ⁵¹Fe, ⁵³Co, ⁵⁵Ni, ⁵⁹Zn, ⁶³Ge; ⁹C, ⁹Li, ¹³O, ¹⁷N, ²¹F, ²⁵Si, ^27,33P, ³⁵S, ³⁵K, ³⁷Ca, ³⁹Sc, ⁴¹Ti, ⁴³V, ⁴⁵Cr, ⁴⁷Mn, ⁴⁹Fe, ⁵¹Co, ⁵³Ni, ⁵⁷Zn, ⁶¹Ge, ⁶³As; ²⁷S, ³¹Ar, ⁴³Cr, ⁴⁷Fe, ⁵¹Ni, ⁵⁵Zn, ⁵⁹Ge; compiled, analyzed, and predicted magnetic dipole moments for isospin 1/2, 3/2 and 5/2 mirror nuclei. ⁵⁷Cu; evaluated magnetic dipole moment of the ground state.

doi: 10.1103/PhysRevC.94.064313

2019MO01

At.Data Nucl.Data Tables 125, 1 (2019)

P.Moller, M.R.Mumpower, T.Kawano, W.D.Myers

Nuclear properties for astrophysical and radioactive-ion-beam applications (II)

NUCLEAR STRUCTURE Z=8-136; calculated the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one- and two-neutron separation energies, quantities related to β-delayed one- and two-neutron emission probabilities, average energy and average number of emitted neutrons, β-decay energy release and T_1/2 with respect to Gamow-Teller decay with a phenomenological treatment of first-forbidden decays, one- and two-proton separation energies, and α-decay energy release and half-life.

doi: 10.1016/j.adt.2018.03.003

2020CU01

Phys.Rev. C 101, 014301 (2020), Erratum Phys.Rev. C 104, 029902 (2021)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Two-proton radioactivity within a generalized liquid drop model

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated half-lives for 2p decay mode using generalized liquid drop model (GLDM) and compared with experimental half-lives, and other theoretical calculations. ²²Si, ²⁶S, ³⁴Ca, ^38,39Ti, ⁴²Cr, ⁴⁹Ni, ⁵⁵Zn, ^58,59,60Ge, ⁶⁴Se(2p); predicted half-lives using GLDM for 2p radioactivity.

doi: 10.1103/PhysRevC.101.014301

2020NE02

Phys.Rev. C 101, 014319 (2020)

L.Neufcourt, Y.Cao, S.Giuliani, W.Nazarewicz, E.Olsen, O.B.Tarasov

Beyond the proton drip line: Bayesian analysis of proton-emitting nuclei

RADIOACTIVITY ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated Q(2p) using eleven global mass models: Skyrme models SkM*, SkP, SLy4, SV-min, UNEDF0, UNEDF1, UNEDF2, BCPM and D1M, FRDM-2012 and HFB-24, and Bayesian model averaging (BMA) results: BMA-0, BMA-I, BMA-II, BMA-III, and comparing with experimental data from AME2016 and later literature. Z=17-82; calculated nuclear binding-energy, and probability of proton decay, relative to the neutron number of the lightest proton-bound isotope with known experimental S(p) or S(2p), in the proton-rich region using BMA-I and BMA-II model averaging methods. ^25,26,27S, ^29,30,31Ar, ^33,34,35Ca, ^37,38,39Ti, ^40,41,42,43Cr, ^44,45,46Fe, ^47,48,49,50Ni, ^52,53,54,55Zn, ^56,57,58,59Ge, ^61,62,63,64Se, ^{64,65,66,67,68}Kr, ^{68,69,70,71,72}Sr, ^{72,73,74,75,76}Zr, ^{76,77,78,79,80}Mo, ^{80,81,82,83,84}Ru, ^{83,84,85,86,87,88}Pd, ^{87,88,89,90,91}Cd, ^{91,92,93,94,95}Sn, ^{100,101,102,103}Te, ^{104,105,106,107}Xe, ^{108,109,110,111,112}Ba, ^{111,112,113,114,115,116}Ce, ^{115,116,117,118,119}Nd, ^{119,120,121,122,123,124}Sm, ^{123,124,125,126,127,128,129}Gd, ^{128,129,130,131,132,133,134}Dy, ^{131,132,133,134,135,136,137}Er, ^{135,136,137,138,139,140,141,142}Yb, ^{141,142,143,144,145,146,147}Hf, ^{145,146,147,148,149,150}W, ^{150,151,152,153,154,155}Os, ^{152,153,154,155,156,157,158}Pt, ^{156,157,158,159,160,161,162}Hg(2p); calculated Q(2p) and half-lives using BMA-1 method. ³⁰Ar, ³⁴Ca, ³⁹Ti, ⁴²Cr, ⁵⁸Ge, ⁶²Se, ⁶⁶Kr, ⁷⁰Sr, ⁷⁴Zr, ⁷⁸Mo, ⁸²Ru, ⁸⁶Pd, ⁹⁰Cd, ¹⁰³Te; predicted as most promising 2p emitters. ^131,132Dy, ^134,135Er, ^144,145Hf; predicted as excellent candidates for the sequential emission of two protons. Bayesian Gaussian processes for separation-energy residuals and combined via Bayesian model averaging for mass predictions, with uncertainty quantification of theoretical predictions.

doi: 10.1103/PhysRevC.101.014319

2021KL02

Phys.Rev. C 103, 024316 (2021)

O.Klochko, N.A.Smirnova

Isobaric-multiplet mass equation in a macroscopic-microscopic approach

NUCLEAR STRUCTURE A=20-100; analyzed Isobaric-multiplet mass equation (IMME) for T=1/2, 1, 3/2, 2, and 5/2 multiplets using P. Moller's macroscopic-microscopic approach with finite-range liquid-drop model (FRLDM); deduced coefficients of the IMME, and mass excesses of Z>N nuclei up to A=100. ^{43,44,45,46,47,48,49}Mn, ^{44,45,46,47,48,49,50,51}Fe, ^{46,47,48,49,50,51,52,53}Co, ^{48,49,50,51,52,53,54,55}Ni, ^{50,51,52,53,54,55,56,57}Cu, ^{52,53,54,55,56,57,58,59}Zn, ^{54,55,56,57,58,59,60,61}Ga, ^{56,57,58,59,60,61,62,63}Ge, ^{58,59,60,61,62,63,64,65}As, ^{60,61,62,63,64,65,66,67}Se, ^{62,63,64,65,66,67,68,69}Br, ^{64,65,66,67,68,69,70,71}Kr, ^{66,67,68,69,70,71,72,73}Rb, ^{68,69,70,71,72,73,74,75}Sr, ^{70,71,72,73,74,75,76,77}Y, ^{72,73,74,75,76,77,78,79}Zr, ^{74,75,76,77,78,79,80,81}Nb, ^{76,77,78,79,80,81,82,83}Mo, ^{78,79,80,81,82,83,84,85}Tc, ^{80,81,82,83,84,85,86,87}Ru, ^{82,83,84,85,86,87,88,89}Rh, ^{84,85,86,87,88,89,90,91}Pd, ^{86,87,88,89,90,91,92,93}Ag, ^{88,89,90,91,92,93,94,95}Cd, ^{90,91,92,93,94,95,96,97}In, ^{92,93,94,95,96,97,98,99}Sn, ^{94,95,96,97,98,99,100}Sb, ^{96,97,98,99,100,101}Te; deduced S(p), S(2p), positions of proton-drip lines. Comparison with available experimental data.

doi: 10.1103/PhysRevC.103.024316

2021KO07

Chin.Phys.C 45, 030001 (2021)

F.G.Kondev, M.Wang, W.J.Huang, S.Naimi, G.Audi

The NUBASE2020 evaluation of nuclear physics properties

COMPILATION A=1-295; compiled, evaluated nuclear structure and decay data.

doi: 10.1088/1674-1137/abddae

2021KU30

Phys.Rev. C 104, 064610 (2021)

A.Kubiela, H.Suzuki, O.B.Tarasov, M.Pfutzner, D.-S.Ahn, H.Baba, A.Bezbakh, A.A.Ciemny, W.Dominik, N.Fukuda, A.Giska, R.Grzywacz, Y.Ichikawa, Z.Janas, L.Janiak, G.Kaminski, K.Kawata, T.Kubo, M.Madurga, C.Mazzocchi, H.Nishibata, M.Pomorski, Y.Shimizu, N.Sokolowska, D.Suzuki, P.Szymkiewicz, A.Swiercz, M.Tajima, A.Takamine, H.Takeda, Y.Takeuchi, C.R.Thornsberry, H.Ueno, H.Yamazaki, R.Yokoyama, K.Yoshida

Production of the most neutron-deficient Zn isotopes by projectile fragmentation of ⁷⁸Kr

NUCLEAR REACTIONS ⁹Be(⁷⁸Kr, X)⁵⁴Zn/⁵⁵Zn/⁵⁶Zn, E=345 MeV/nucleon; measured reaction products, production σ using BigRIPS separator at the RIBF-RIKEN facility. Comparison of measured σ for Zn isotopes in this work, and for germanium, selenium, and krypton isotopes in other studies with predictions of the EPAX3 parametrization, LISE++ abrasion-ablation model using the HFB22 mass model and the AME2020 mass tables. Relevance to production of nuclei decaying by 2p radioactivity such as ⁵⁴Zn.

doi: 10.1103/PhysRevC.104.064610

2021SA53

Phys.Rev. C 104, 064613 (2021)

K.P.Santhosh

Theoretical studies on two-proton radioactivity

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated T_1/2 using Coulomb and proximity potential model for deformed nuclei (CPPMDN) with and without deformation effects, and compared with experimental values, and various other theoretical calculations: generalized liquid drop model (GLDM), effective liquid drop model (ELDM), Gamow-like model (GLM), screened electrostatic barrier (SEB), two-potential approach with Skyrme Hartree Fock (SHF), unified fission model (UFM), new Geiger-Nuttall law (GNL), and four-parameter empirical formula (EF). ¹⁶Ne, ¹⁹Mg, ²²Si, ²⁶S, ³⁰Ar, ³⁴Ca, ^38,39Ti, ⁴²Cr, ⁴⁹Ni, ⁵⁵Zn, ^58,59,60Ge, ⁶⁴Se(2p); calculated T_1/2 with and without deformation effects, and compared with various other theoretical calculations as stated above.

doi: 10.1103/PhysRevC.104.064613

2021WA16

Chin.Phys.C 45, 030003 (2021)

M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi

The AME 2020 atomic mass evaluation (II). Tables, graphs and references

ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.

doi: 10.1088/1674-1137/abddaf

2021XI06

Chin.Phys.C 45, 124105 (2021)

F.Xing, J.Cui, Y.Wang, J.Gu

Two-proton radioactivity of ground and excited states within a unified fission model

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); ⁵Be, ^6,7B, ⁸C, ¹⁰N, ¹¹O, ^13,14F, ¹⁵Ne, ¹⁷Na, ²²Si, ²⁴P, ²⁶S, ^28,29Cl, ^29,30Ar, ^31,32K, ^33,34Ca, ⁴⁵Sc, ^35,37Sc, ^37,38,39Ti, ^39,40V, ^41,42Cr, ^43,44Mn, ⁴⁷Co, ⁴⁹Ni, ⁵²Cu, ⁵⁵Zn, ^56,57,58Ga, ^58,59Ge, ^60,61,62As, ^63,64Se, ^65,66Br, ⁶⁸Kr, ⁸¹Mo, ⁸⁵Ru, ¹⁰⁸Xe(2p); analyzed available data; calculated T_1/2. Comparison with the AME2020 table, available data.

doi: 10.1088/1674-1137/ac2425