References quoted in the ENSDF dataset: 96CD ADOPTED LEVELS

23 references found.

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

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1969PE18

Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 1710 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 1566 (1970)

L.K.Peker

On the Spins of the Lower Levels of Four-Particle [(jp)²I(p max);(jn)₂I(n max)] Configurations and Possible Isomeric States in ⁸⁰Zr, ⁸⁸Zr, and Similar Nuclei

NUCLEAR STRUCTURE ^80,82,88Zr, ^82,84,90,92Mo, ⁹⁶Cd, ²¹⁰Po; deduced isomeric states, J, π.

1971PE16

Phys.Lett. 36B, 547 (1971)

L.K.Peker, E.I.Volmyansky, V.E.Bunakov, S.G.Ogloblin

Many-Particle Isomeric States as Sources of Proton and Neutron Radio-Activity

RADIOACTIVITY ⁸⁰Zr, ⁸²Zr, ^82,84Mo, ⁹⁶Cd, ⁵³Co, ⁷⁷Rb, ⁷⁹Rb, ⁸¹Y, ⁸¹Zr, ⁸¹Nb, ^97,99Cd, ⁶¹Sc, ⁶³Sc, ^63,70Ti, ^67,75Fe, ¹²¹Zr, ¹²³Mo; calculated nucleon decay T_1/2; analyzed configurations for isomeric states.

doi: 10.1016/0370-2693(71)90085-2

1983OG01

Phys.Rev. C28, 958 (1983)

K.Ogawa

Shell-Model Calculations of High-Spin Isomers in Neutron-Deficient lg_9/2-Shell Nuclei

NUCLEAR STRUCTURE ⁹⁵Pd, ⁹⁵Ag, ^96,97Cd; calculated levels, T_1/2; deduced high-spin isomer stability characteristics. ⁹⁵Pd deduced isomer, J, π. Shell model.

doi: 10.1103/PhysRevC.28.958

1985BU27

Yad.Fiz. 42, 57 (1985); Sov.J.Nucl.Phys. 42, 34 (1985)

V.P.Bugrov, V.E.Bunakov, S.G.Kadmensky, V.I.Furman

Single-Nucleon Decay of Isomeric Nuclear States

NUCLEAR STRUCTURE ^77,79Rb, ⁸¹Y, ⁹⁵Ag, ¹⁵¹Lu, ^121,80,82Zr, ^123,82,84Mo, ⁹⁶Cd, ^63,70Ti, ^67,75Fe, ⁵³Co; calculated isomeric state single nucleon decay T_1/2; deduced residual interaction finite range importance.

1988RE08

Phys.Rev. C38, 550 (1988)

N.Redon, J.Meyer, M.Meyer, P.Quentin, P.Bonche, H.Flocard, P.-H.Heenen

Proton-Rich Exotic Heavy Nuclei: Self-consistent calculations

NUCLEAR STRUCTURE ^{92,96,98,100,102,104,106,108,110}Cd; ^{142,140,138,136,134,132}Sm; calculated potential energy surfaces; deduced deformation features.

doi: 10.1103/PhysRevC.38.550

1992BI07

Phys.Rev. C46, 1555 (1992)

G.T.Biehle, P.Vogel

Calculation of Beta-Decay Half-Lives of Proton-Rich Nuclei of Intermediate Mass

NUCLEAR STRUCTURE ^74,76Sr, ^78,80Zr, ^84,86Mo, ^88,90Ru, ⁹²Pd, ⁹⁶Cd(β⁺); calculated T_1/2. Random phase approximation, quasiparticle formalism.

doi: 10.1103/PhysRevC.46.1555

1995DO05

Phys.Rev. C51, R1070 (1995)

J.Dobaczewski, W.Nazarewicz

Limits of Proton Stability Near ¹⁰⁰Sn

NUCLEAR STRUCTURE ^94,96,98,100Cd, ^{96,98,100,102}Sn, ^{98,100,102,104}Te; calculated total energy. ^106,108,110Te, ^{94,96,98,100,102}Sn; calculated two proton separation energies; deduced proton stability features. ^{92,94,96,98,100,102}Sn; calculated single particle proton energies. Skyrme HFB theory.

doi: 10.1103/PhysRevC.51.R1070

1995FR10

Nucl.Phys. A587, 36 (1995)

M.Freer, R.R.Betts, A.H.Wuosmaa

Relationship between the Deformed Harmonic Oscillator and Clustering in Light Nuclei

NUCLEAR STRUCTURE ⁸Be, ¹²C, ²⁰Ne, ²⁴Mg, ³²S, ³⁶Ar, ⁵⁶Ni, ⁴⁸Cr, ⁷²Kr, ⁸⁰Zr, ⁹⁶Cd; calculated harmonic oscillator configuration contour density plots at 2:1, 3:1 axial deformations; deduced deformed harmonic oscillator, clustering relationship.

doi: 10.1016/0375-9474(94)00820-D

1996DE63

Phys.Lett. 367B, 17 (1996)

D.J.Dean, S.E.Koonin, T.T.S.Kuo, K.Langanke, P.B.Radha

Complete 0(h-bar x Omega) Shell Model Carlo Calculations of ⁹⁴Ru, ⁹⁶Pd, ^96,98Cd and ¹⁰⁰Sn

NUCLEAR STRUCTURE ⁹⁴Ru, ⁹⁶Pd, ^96,98Cd, ¹⁰⁰Sn; calculated Gamow-Teller transition, masses, strengths. Shell model Monte Carlo technique.

doi: 10.1016/0370-2693(95)01446-2

1997HE24

Nucl.Phys. A627, 35 (1997)

H.Herndl, B.A.Brown

Shell-Model Calculations for the Properties of Nuclei with A = 86-100 Near the Proton Drip Line

NUCLEAR STRUCTURE ^92,94Pd, ^90,91,92Rh, ⁸⁹Tc; calculated levels, J, π. ^86,87,88Sr, ^86,87,88,89Y, ^{86,87,88,89,90}Zr, ^{86,87,88,89,90,91}Nb, ^{86,87,88,89,90,91,92}Mo, ^{86,87,88,89,90,91,92,93}Tc, ^{86,87,88,89,90,91,92,93,94}Ru, ^{86,87,88,89,90,91,92,93,94,95}Rh, ^{86,87,88,89,90,91,92,93,94,95,96}Pd, ^{87,88,89,90,91,92,93,94,95,96,97}Ag, ^{88,89,90,91,92,93,94,95,96,97,98}Cd, ^{89,90,91,92,93,94,95,96,97,98,99}In, ^{90,91,92,93,94,95,96,97,98,99,100}Sn; calculated binding energies; deduced proton drip line. ^86,87,88Sr, ^86,87,88,89Y, ^{86,87,88,89,90}Zr, ^{86,87,88,89,90,91}Nb, ^{86,87,88,89,90,91,92}Mo, ^{86,87,88,89,90,91,92,93}Tc, ^{86,87,88,89,90,91,92,93,94}Ru, ^{90,91,92,93,94,95}Rh, ^{88,89,90,91,92,93,94,95,96}Pd, ^94,95,96,97Ag, ^{92,93,94,95,96,97,98}Cd, ^98,99In, ^98,99,100Sn; calculated ground-state spin, T_1/2. Shell model.

doi: 10.1016/S0375-9474(97)00407-7

1998GO26

Phys.Rev. C58, R3051 (1998)

A.L.Goodman

T = 0 and T = 1 Pair Correlations in N = Z Medium-Mass Nuclei

NUCLEAR STRUCTURE ⁷⁶Sr, ⁸⁰Zr, ⁸⁴Mo, ⁸⁸Ru, ⁹²Pd, ⁹⁶Cd; calculated ground state pairing strengths; deduced T=0, 1 pairing contributions. HFB equation, isospin generalized BCS equations.

doi: 10.1103/PhysRevC.58.R3051

1999GO12

Phys.Rev. C60, 014311 (1999)

A.L.Goodman

Proton-Neutron Pairing in Z = N Nuclei with A = 76-96

NUCLEAR STRUCTURE ⁷⁶Sr, ⁸⁰Zr, ⁸⁴Mo, ⁸⁸Ru, ⁹²Pd, ⁹⁶Cd; calculated deformation, pair correlation features, proton-neutron pairing contributions. Hartree-Fock - Bogoliubov theory.

doi: 10.1103/PhysRevC.60.014311

2000GO31

Phys.Scr. T88, 170 (2000)

A.L.Goodman

T = 0 and T = 1 Pair Correlations in N = Z Nuclei with A = 76-96

NUCLEAR STRUCTURE ⁷⁶Sr, ⁸⁰Zr, ⁸⁴Mo, ⁸⁸Ru, ⁹²Pd, ⁹⁶Cd; calculated average pair gap, pairing energy; deduced relative T=0, T=1 pairing contributions.

doi: 10.1238/Physica.Topical.088a00170

2002BA58

Phys.Rev. C65, 064303 (2002)

E.Baldini-Neto, C.L.Lima, P.Van Isacker

Binding Energies of T = 0 and T = 1 Ground States of N = Z Nuclei in the Interacting Boson Model

NUCLEAR STRUCTURE ¹⁸F, ²⁰Ne, ²²Na, ²⁴Mg, ²⁶Al, ²⁸Si, ³⁰P, ³²S, ³⁴Cl, ³⁶Ar, ³⁸K, ⁵⁸Cu, ⁶⁰Zn, ⁶²Ga, ⁶⁴Ge, ⁶⁶As, ⁶⁸Se, ⁷⁰Br, ⁷²Kr, ⁷⁴Rb, ⁷⁶Sr, ⁷⁸Y, ⁸⁰Zr, ⁸²Nb, ⁸⁴Mo, ⁸⁶Tc, ⁸⁸Ru, ⁹⁰Rh, ⁹²Pd, ⁹⁴Ag, ⁹⁶Cd, ⁹⁸In; calculated binding energies, energy differences between T=0 and T=1 states. Interacting boson model.

doi: 10.1103/PhysRevC.65.064303

2002IS08

Yad.Fiz. 65, 1466 (2002); Phys.Atomic Nuclei 65, 1431 (2002)

V.I.Isakov, K.I.Erokhina

Nuclear Masses and Properties of Nuclei in the Vicinity of the Remote Magic Nucleus ¹⁰⁰Sn

NUCLEAR STRUCTURE ^{96,97,98,99,100}Cd, ^{97,98,99,100,101}In, ^{98,99,100,101,102}Sn, ^{99,100,101,102,103}Sb, ^{100,101,102,103,104}Te; calculated mass differences. ^100,132Sn; calculated nucleon density distributions. ⁹²Mo, ⁹⁴Ru, ⁹⁶Pd, ⁹⁸Cd, ¹⁰⁰Sn; calculated levels, J, π, B(E2).

doi: 10.1134/1.1501655

2003AU03

Nucl.Phys. A729, 337 (2003)

G.Audi, A.H.Wapstra, C.Thibault

The AME2003 atomic mass Evaluation (II). Tables, graphs, and references

COMPILATION A=1-293; compiled, evaluated atomic mass data.

doi: 10.1016/j.nuclphysa.2003.11.003

2004ME13

Pramana 62, 841 (2004)

M.S.Mehta, T.K.Jha, S.K.Patra, R.K.Gupta

Potential energy surfaces for N = Z, ²⁰Ne-¹¹²Ba nuclei

NUCLEAR STRUCTURE ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca, ⁴⁴Ti, ⁴⁸Cr, ⁵²Fe, ⁵⁶Ni, ⁶⁰Zn, ⁶⁴Ge, ⁶⁸Se, ⁷²Kr, ⁷⁶Sr, ⁸⁰Zr, ⁸⁴Mo, ⁸⁸Ru, ⁹²Pd, ⁹⁶Cd, ¹⁰⁰Sn, ¹⁰⁴Te, ¹⁰⁸Xe, ¹¹²Ba; calculated energy vs deformation. Deformed relativistic mean field approach.

2008BA53

Phys.Rev.Lett. 101, 252501 (2008)

D.Bazin, F.Montes, A.Becerril, G.Lorusso, A.Amthor, T.Baumann, H.Crawford, A.Estrade, A.Gade, T.Ginter, C.J.Guess, M.Hausmann, G.W.Hitt, P.Mantica, M.Matos, R.Meharchand, K.Minamisono, G.Perdikakis, J.Pereira, J.Pinter, M.Portillo, H.Schatz, K.Smith, J.Stoker, A.Stolz, R.G.T.Zegers

Production and β Decay of rp-Process Nuclei ⁹⁶Cd, ⁹⁸In, and ¹⁰⁰Sn

NUCLEAR REACTIONS ⁹Be(¹¹²Sn, X)⁹⁶Cd/⁹⁸In/¹⁰⁰Sn, E=120 MeV/nucleon; measured cross sections.

RADIOACTIVITY ⁹⁶Cd, ⁹⁸In, ¹⁰⁰Sn; measured decay spectra, half-lives.

doi: 10.1103/PhysRevLett.101.252501

2008KA19

Phys.Rev. C 77, 064304 (2008); Erratum Phys.Rev. C 78, 049903 (2008)

K.Kaneko, Y.Sun, M.Hasegawa, T.Mizusaki

Structure of upper-g_9/2-shell nuclei and shape effect in the ⁹⁴Ag isomeric states

NUCLEAR STRUCTURE ⁹⁴Ag; calculated levels, J, π, spectroscopic quadrupole moments, expectation values of proton and neutron numbers, B(E2). ^{90,91,92,93,94}Ru, ^91,92,93Tc, ^{90,92,93,94,95}Rh, ^{92,93,94,95,96}Pd, ⁹⁵Ag, ^96,98Cd; calculated level energies, J, π. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.064304

2008KRZW

Proc.Nuclear Physics and Astrophysics: From Stable Beams to Exotic Nuclei, Cappadocia, Turkey, June 25-30, 2008, I.Boztosun, A.B.Balantekin, Eds., p.52 (2008); AIP Conf. Proc. 1072 (2008)

R.Krucken

Probing the shell structure near ⁵⁴Ca and ¹⁰⁰Sn

NUCLEAR REACTIONS ⁹Be(⁵⁰Ca, ⁴⁹Ca), (⁵⁶Ti, ⁵⁵Ti), E not given; measured fragment spectra, Eγ, Iγ, (particle)γ-coin, and longitudinal momentum distributions using MUSIC system for particles and Miniball array for γ rays at GSI facility. ⁴⁹Ca, ⁵⁵Ti; deduced levels, J, π, and angular momentum transfers for one-neutron knockout reactions. Comparison with OXBASH shell-model calculations using GXPF1A interaction.

NUCLEAR REACTIONS ⁹Be(⁸⁶Kr, X)⁵⁰Ca/⁵⁶Ti, E=500 MeV/nucleon; ⁹Be(¹²⁴Xe, X)⁹³Ag/⁹⁴Ag/⁹⁵Ag/⁹⁶Ag/⁹⁷Ag/⁹⁸Ag/⁹⁹Ag/⁹⁵Cd/⁹⁶Cd/⁹⁷Cd/⁹⁸Cd/⁹⁹Cd/¹⁰⁰Cd/¹⁰¹Cd/⁹⁷In/⁹⁸In/⁹⁹In/¹⁰⁰In/¹⁰¹In/¹⁰²In/¹⁰³In/¹⁰⁰Sn/¹⁰¹Sn/¹⁰²Sn/¹⁰³Sn/¹⁰⁴Sn/¹⁰⁵Sn/¹⁰⁴Sb/¹⁰⁵Sb/¹⁰⁶Sb/¹⁰⁷Sb/¹⁰⁸Te/¹⁰⁹Te, E=1 GeV/nucleon; measured yields using RISING array for γ rays at GSI facility.

doi: 10.1063/1.3039864

2009AB02

Phys.Rev. C 79, 024317 (2009)

H.Abusara, A.V.Afanasjev

Hyperdeformation in the Cd isotopes: A microscopic analysis

NUCLEAR STRUCTURE ^{96,98,100,102,104,106,107,108,109}Cd; calculated energies of hyperdeformed configurations as a function of angular momentum, dynamic moments of inertia, transition quadrupole moments and mass hexadecapole moments using cranked relativistic mean field theory.

doi: 10.1103/PhysRevC.79.024317

2009AUZZ

Priv.Comm. (2009)

G.Audi, W.Meng, D.Lunney, B.Pfeiffer

Atomic Mass Evaluation 2009

2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.