Possible coexistence of principal and tilted axis rotation in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow /><mml:mrow><mml:mn>103</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">Ag</mml:mi></mml:math>

Datta, Pradip; Chattopadhyay, S.; Banerjee, P.; Bhattacharya, S.; Chatterjee, Jayita; Dasmahapatra, B.; Dey, C.C.; Ghosh, T. K.; Goswami, A.; Pal, Subrata; Ray, Indrani; Sarkar, M. Saha; Sen, S.; Jain, H. C.; Joshi, P. K.; Amita,

doi:10.1103/physrevc.67.014325

Cited by 20 publications

(10 citation statements)

References 22 publications

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“…The evolution of magnetic rotation with the growing number of neutrons can also be observed for bands with the configuration πg 9/2 ⊗[h 11/2 (g 9/2 /d 5/2 ) 1 ] in 103,105,107 Ag, which was reproduced by the TAC model in Ref. [34].…”

Section: Discussionmentioning

confidence: 69%

Lifetime measurements and magnetic rotation in107Ag

Yao

Zhu

et al. 2014

Phys. Rev. C

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The excited states in 107 Ag were populated through the heavy-ion fusion evaporation reaction 100 Mo ( 11 B, 4n) 107 Ag at a beam energy of 46 MeV. Lifetimes of high-spin states in 107 Ag have been measured through the Doppler shift attenuation method. The deduced B(M1) values, gradually decreasing with increasing spin, clearly demonstrate that both the yrast positive-parity band and the yrast negative-parity band in 107 Ag are magnetic rotation bands. Furthermore, experimental deduced B(M1) values for the yrast positive-parity band are compared with the predictions of the particle rotor model. The approximate agreement between theoretical calculations and experimental results further confirms the mechanism of magnetic rotation for the yrast positive-parity band. In addition, a systematic investigation shows the evolution of the magnetic rotation mechanism in the A ≈ 110 mass region.

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Section: Discussionmentioning

confidence: 69%

Lifetime measurements and magnetic rotation in107Ag

Yao

Zhu

et al. 2014

Phys. Rev. C

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“…However, band 2 in Ref. [10] does not exhibit significant lineshapes for any but the uppermost (516 keV) transition; therefore, a lineshape analysis for this band was not possible. Examples of the lineshape fits for the representative transitions are shown in Fig.…”

Section: Resultsmentioning

confidence: 98%

“…Previous studies have established high spin level structures of 103 Ag [10], 105 Ag [11], and 106 Ag [12] using heavy-ion fusion evaporation reactions. The partial level schemes of 103 Ag, 105 Ag, and 106 Ag pertinent to the present work have been adopted from these studies Fig.…”

Section: Methodsmentioning

confidence: 99%

“…The branching ratios and the side-feeding intensities, which are two of the input parameters for the lineshape analysis, were estimated using available intensity data for 103 Ag [10] and 105 Ag [11]. Typically, these values are obtained from the same reaction by using thin-target experiments because two different reactions may feed the high-spin states with slightly different intensities.…”

Section: B Lineshape Analysismentioning

confidence: 99%

“…A previous study [10] has determined the high spin level structure in 103 Ag, part of which is illustrated in Fig. 1.…”

Section: A 103 Agmentioning

confidence: 99%

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Systematics of the shears mechanism in silver isotopes

et al. 2006

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A systematic investigation of the shears mechanism in silver isotopes has been carried out. Lifetimes have been measured by means of the Doppler-shift attenuation method for states in two magnetic dipole (M1) bands in 105 Ag and one each in 103 Ag and 106 Ag. Experimental total angular momenta and reduced transition strengths for these bands have been compared with the predictions of the tilted axis cranking (TAC) model with configurations involving one g 9/2 proton and quasineutrons from the h 11/2 and g 7/2 or d 5/2 orbitals. There is good overall agreement for both the total angular momenta and reduced transition strengths. The deduced B(M1) strengths, which are a sensitive probe of magnetic rotation, show a decrease consistent with TAC predictions for one M1 band in 105 Ag and in 106 Ag, confirming the shears mechanism as the means of excitation. Furthermore, the staggering in the transition energies in 103 Ag and absence of regular sequences of M1 transitions for N 56 suggest that N = 56 is the lower boundary for the appearance of the shears mechanism in this mass region.

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Energy levels and branching ratios for Ag-103 (Silver-103)

Sukhoruchkin¹,

Soroko²

2008

Tables of Excitations of Proton- And Neutron-Rich Unstable Nuclei

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Possible coexistence of principal and tilted axis rotation in103Ag

Cited by 20 publications

References 22 publications

Lifetime measurements and magnetic rotation in107Ag

Lifetime measurements and magnetic rotation in107Ag

Systematics of the shears mechanism in silver isotopes

Energy levels and branching ratios for Ag-103 (Silver-103)

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