Transverse spin polarization in odd-mass deformed nuclei

Bochnacki, Z.; Ogaza, S.

doi:10.1016/0029-5582(66)90115-5

Cited by 22 publications

(5 citation statements)

References 4 publications

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“…but it has been pointed out by Bochnacki and Ogaza [22] that the renormalization of g s could be different between s + , arising from the so-called transverse polarization, Eq. 12, and s 3 , the longitudinal polarization, Eq.…”

Section: Discussion Of the Magnetic Properties Of The Principal Bandsmentioning

confidence: 99%

“…The result is compatible with a common renormalization of g s in Eqs. (10) and (12), and therefore there is no reason to invoke the theory of Bochnacki and Ogaza [22].…”

Section: Discussion Of the Magnetic Properties Of The Principal Bandsmentioning

confidence: 99%

“…For the γ -vibrational bands, K = 2 Coriolis mixing can be treated in lowest order by (22) where K f = K i + 2. (cf.…”

Section: Bandmentioning

confidence: 99%

“…The analysis of the γ -ray branching ratios between the vibrational bands and the ground-state band yields experimental values for the parameter ratio M 2 /M 1 , which we can then apply in Eq. (22) to derive realistic E2 matrix elements for the Coulomb excitation calculations. We will discuss the Coriolis mixing of the ground state and γ -vibrational bands more fully in Sec.…”

Section: Bandmentioning

confidence: 99%

“…All the E2 matrix elements connecting the ground state to the excited bands may be obtained by substituting the extracted Q t in Eq (21),. or in the cases of K = 2 mixing, in Eq (22)…”

mentioning

confidence: 99%

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Band structure of235U

et al. 2012

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Over a period of several years we have performed three separate experiments at Lawrence Berkeley National Laboratory's 88-Inch Cyclotron in which 235 U (thick target) was Coulomb-excited. The program involved standalone experiments with Gammmasphere and with the 8pi Spectrometer using 136 Xe beams at 720 MeV, and a CHICO-Gammasphere experiment with a 40 Ca beam at 184 MeV. In addition to extending the known negativeparity bands to high spin, we have assigned levels in some seven positive-parity bands which are in some cases (e.g., [631]1/2, [624]7/2, and [622]5/2) strongly populated by E3 excitation. The CHICO data have been analyzed to extract E2 and E3 matrix elements from the observed yields. Additionally, many M1 matrix elements could be extracted from the γ-ray branching ratios. A number of new features have emerged, including the unexpected attenuation of magnetic transitions between states of the same Nilsson multiplet, the breakdown of Coriolis staggering at high spin, and the effect of E3 collectivity on Coriolis interactions.

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Section: Discussion Of the Magnetic Properties Of The Principal Bandsmentioning

confidence: 99%

“…The result is compatible with a common renormalization of g s in Eqs. (10) and (12), and therefore there is no reason to invoke the theory of Bochnacki and Ogaza [22].…”

Section: Discussion Of the Magnetic Properties Of The Principal Bandsmentioning

confidence: 99%

“…For the γ -vibrational bands, K = 2 Coriolis mixing can be treated in lowest order by (22) where K f = K i + 2. (cf.…”

Section: Bandmentioning

confidence: 99%

Section: Bandmentioning

confidence: 99%

“…All the E2 matrix elements connecting the ground state to the excited bands may be obtained by substituting the extracted Q t in Eq (21),. or in the cases of K = 2 mixing, in Eq (22)…”

mentioning

confidence: 99%

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