Half-life and magnetic moment of the first excited state in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">I</mml:mi><mml:mprescripts /><mml:none /><mml:mrow><mml:mn>132</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>

Tanigaki, M.; Izumi, Satoru; Ouchi, Hiroki; Sasaki, Akihiko; Miyashita, Yuji; Sato, Nobuyuki; Hoshino, Shotaro; Shimada, K.; Wakui, Takashi; Shinozuka, T.; Ohkubo, Y.

doi:10.1103/physrevc.80.034304

Cited by 8 publications

(8 citation statements)

References 20 publications

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“…In this β-decay study, only the low spin states were popu- lated. The lifetime and magnetic moment measurements of low spin states have been reported in various investigations [40][41][42]. The presence of an isomeric state (8 − , T 1/2 = 83.6 ± 1.7 min) at 120 keV excitation was also reported in Ref.…”

Section: B 131 Isupporting

confidence: 53%

High-spin states above the isomers in neutron-rich iodine nuclei near N=82

Banik¹,

Bhattacharyya²,

Rejmund³

et al. 2020

Phys. Rev. C

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Excited states of neutron rich Iodine isotopes 130−134 I above the high spin isomers have been identified using prompt-delayed γ-ray spectroscopy. The Iodine isotopes have been produced as fission fragments of fusion-fission and transfer induced fission of 9 Be(238 U, f) at a beam energy of 6.2 MeV/u. The complete (A, Z) identification was obtained using the large acceptance magnetic spectrometer VAMOS++. The AGATA γ-ray tracking array was used to detect the prompt γ rays while the delayed γ rays (in the time range of 100 ns to 200 µs) from the isomeric states were identified by the EXOGAM segmented Clover detectors, placed behind the focal plane of VAMOS++ spectrometer. The high spin states above the (8 −) isomers in 130,132 I have been populated for the first time and a new isomer in 132 I has been identified. New γ-ray transition has also been assigned to the level structure of 134 I. Prompt transitions above the 19/2 − isomer have been identified in 131,133 I, for the first time. The level structures are interpreted in terms of the systematics of odd-Z nuclei above Z = 50 shell closure and large scale shell model calculations.

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Section: B 131 Isupporting

confidence: 53%

High-spin states above the isomers in neutron-rich iodine nuclei near N=82

Banik¹,

Bhattacharyya²,

Rejmund³

et al. 2020

Phys. Rev. C

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“…The lifetime of the first excited state of 132 I, reported in the literature using either plastic or inorganic scintillators, is found to have wide variations, ranging from 7.14ns [6] to 2.94ns [7]. Recently, measurements have been carried out with BaF 2 scintillators from the decay of 132 Te radioactive beam [8]. However, BaF 2 detectors, though have a very good time resolution, are not suitable for precise energy selection because of their poor energy resolution.…”

Section: Introductionmentioning

confidence: 99%

Lifetime measurements and decay spectroscopy of¹³²I

Bhattacharyya

Banerjee

Das

et al. 2014

EPJ Web of Conferences

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“…( 1). 1 Using three detectors with an external magnetic field from a cage-type magnet of 0.3 T [12] applied perpendicularly to the detector plane, the directional anisotropy R(t) was obtained according to…”

Section: B Time-differential Perturbed Angular Correlation Measurementsmentioning

confidence: 99%

Magnetic moment of the 2083 keV level of140Ce

Ohkubo

Taniguchi

et al. 2013

Phys. Rev. C

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For the magnetic moment of the 2083 keV level of 140 Ce, there are four published data, all obtained by applying an external magnetic field of less than 5 T to a liquid sample containing 140 La using the time-differential perturbed angular correlation (TDPAC) technique. Although these four values are consistent within two times their uncertainties (2σ ), the range of values in 2σ extends from μ = +3.0 to + 5.2 (in units of nuclear magneton, μ N ). This time, the TDPAC technique was successfully applied to the 2083 keV level of 140 Ce implanted in an Fe foil. The magnetic moment of this level was determined to be μ = +4.00(20)μ N , employing the known hyperfine field at 141 Ce in Fe, − 41(2) T, which agrees very well with one of the values, μ = +4.06(15)μ N . The present value is compared with two shell-model calculations.

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Half-life and magnetic moment of the first excited state inI132

Cited by 8 publications

References 20 publications

High-spin states above the isomers in neutron-rich iodine nuclei near N=82

High-spin states above the isomers in neutron-rich iodine nuclei near N=82

Lifetime measurements and decay spectroscopy of¹³²I

Magnetic moment of the 2083 keV level of140Ce

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Half-life and magnetic moment of the first excited state inI132

Cited by 8 publications

References 20 publications

High-spin states above the isomers in neutron-rich iodine nuclei near N=82

High-spin states above the isomers in neutron-rich iodine nuclei near N=82

Lifetime measurements and decay spectroscopy of132I

Magnetic moment of the 2083 keV level of140Ce

Contact Info

Product

Resources

About

Lifetime measurements and decay spectroscopy of¹³²I