Nuclear Data Sheets for A=105

Lalkovski, S.; Tímár, J.; Elekes, Z.

doi:10.1016/j.nds.2019.11.001

Cited by 12 publications

(5 citation statements)

References 203 publications

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“…Figure 5. Reduced electromagnetic transitions strength B(E2) in105 Cd, from the present work, compared to the B(E2) in 104,106,107 Cd nuclei[22,[25][26][27]. Transitions arrow widths are proportional to the reduced electromagnetic rates.…”

mentioning

confidence: 74%

“…105 Cd partial level scheme confirmed in the present study. Level and γ-ray energies, as well as spin and parity assignments are taken from [22]. 11/2 + , 15/2 − , 19/2 − levels half-lives are from the present experiment.…”

Section: Discussionmentioning

confidence: 99%

“…Experimental data for 105 Cd: rounded of level energies (E level ) and spin/parities (J π ), half-lives (T 1/2 ); γ-ray energies of the de-exciting transitions (E γ ); γ-ray multipolarities (λM), reduced transition probabilities (B(E2)) and electron conversion coefficients (α). Except for T 1/2 data, which is from the present experiment, the data comes from Adopted levels and gammas in [22]; α values are calculated with BrIcc [23]. Everywhere, the statistical uncertainties are on the last significant digit.…”

Section: Discussionmentioning

confidence: 99%

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Core-excited states in ¹⁰⁵Cd

Ivanova,

Lalkovski,

Atanasova

et al. 2024

Phys. Scr.

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105Cd was produced in the 96Mo+12C fusion/evaporation reaction, performed at NIPNE, Bucharest-Magurele, Romania. Various excited states of positive- and negative-parities were populated. Picosecond half-lives were measured by using the Differential Decay Curve Method (DDCM) method, allowing to control the side feeding of the states of interest. New data were obtained for the half-lives of the 11/2+, 15/2− and 19/2− 105Cd states. Reduced electric quadrupole transition strengths were calculated and compared to the neighboring odd-A and even-A cadmium nuclei. The particle-core weak coupling approach was used to interpret excited states of 105Cd in the light of the new data.

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mentioning

confidence: 74%

Section: Discussionmentioning

confidence: 99%

Section: Discussionmentioning

confidence: 99%

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Core-excited states in ¹⁰⁵Cd

Ivanova,

Lalkovski,

Atanasova

et al. 2024

Phys. Scr.

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“…[22,23], for example). Several 105 Mo γ rays [24] were identified in the coincidence data by setting gates at energies corresponding to transitions in this nucleus. For example, the strongest transition that depopulates the first excited state at 95 keV is of mixed M 1+E2 character, with mixing ratio δ = -0.24(4) and total internal conversion coefficient α = 0.355 (22) [24].…”

Section: B β-Decay Half-lifementioning

confidence: 99%

Ground-state and decay properties of neutron-rich 106Nb

Mitchell,

Orford,

Lane

et al. 2021

Preprint

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The ground-state properties of neutron-rich 106 Nb and its β decay into 106 Mo have been studied using the CARIBU radioactive-ion-beam facility at Argonne National Laboratory. Niobium-106 ions were extracted from a 252 Cf fission source and mass separated before being delivered as low-energy beams to the Canadian Penning Trap, as well as the X-Array and SATURN β-decay-spectroscopy station. The measured 106 Nb ground-state mass excess of -66202.0(13) keV is consistent with a recent measurement but has three times better precision; this work also rules out the existence of a second long-lived, β-decaying state in 106 Nb above 5 keV in excitation energy. The decay half-life of 106 Nb was measured to be 1.097(21) s, which is 8% longer than the adopted value. The level scheme of the decay progeny, 106 Mo, has been expanded up to ≈4 MeV. The distribution of decay strength and considerable population of excited states in 106 Mo of J ≥ 3 emphasises the need to revise the adopted J π = 1 − ground-state spin-parity assignment of 106 Nb; it is more likely to be J ≥ 3.

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“…[22,23], for example). Several 105 Mo γ rays [24] were identified in the coincidence data by setting gates at energies corresponding to transitions in this nucleus. For example, the strongest transition that depopulates the first-excited state at 95 keV is of mixed M1 + E 2 character, with mixing ratio δ = −0.24(4) and total internal-conversion coefficient α = 0.355 (22) [24].…”

Section: B β-Decay Half-lifementioning

confidence: 99%

Ground-state and decay properties of neutron-rich Nb106

et al. 2021

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The ground-state properties of neutron-rich 106 Nb and its β decay into 106 Mo have been studied using the CARIBU radioactive-ion-beam facility at Argonne National Laboratory. Niobium-106 ions were extracted from a 252 Cf fission source and mass separated before being delivered as low-energy beams to the Canadian Penning Trap, as well as the X-Array and SATURN β-decay-spectroscopy station. The measured 106 Nb ground-state mass excess of −66202.0(13) keV is consistent with a recent measurement but has three times better precision; this work also rules out the existence of a second long-lived, β-decaying state in 106 Nb above 5 keV in excitation energy. The decay half-life of 106 Nb was measured to be 1.097(21) s, which is 8% longer than the adopted value. The level scheme of the decay progeny, 106 Mo, has been expanded up to ≈4 MeV. The distribution of decay strength and considerable population of excited states in 106 Mo of J 3 emphasizes the need to revise the adopted J π = 1 − ground-state spin-parity assignment of 106 Nb; it is more likely to be J 3.

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Nuclear Data Sheets for A=105

Cited by 12 publications

References 203 publications

Core-excited states in ¹⁰⁵Cd

Core-excited states in ¹⁰⁵Cd

Ground-state and decay properties of neutron-rich 106Nb

Ground-state and decay properties of neutron-rich Nb106

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Nuclear Data Sheets for A=105

Cited by 12 publications

References 203 publications

Core-excited states in 105Cd

Core-excited states in 105Cd

Ground-state and decay properties of neutron-rich 106Nb

Ground-state and decay properties of neutron-rich Nb106

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Product

Resources

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Core-excited states in ¹⁰⁵Cd

Core-excited states in ¹⁰⁵Cd