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Related papers: Decay out of a Superdeformed Band

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We derive analytic formulae for the energy average (including the energy average of the fluctuation contribution) and variance of the intraband decay intensity of a superdeformed band. Our results may be expressed in terms of three…

Nuclear Theory · Physics 2009-11-07 A. J. Sargeant , M. S. Hussein , M. P. Pato , M. Ueda

We investigate a random matrix model [Phys. Rev. C {\bf 65} 024302 (2002] for the decay-out of a superdeformed band as a function of the parameters: $\Gamma^\downarrow/\Gamma_S$, $\Gamma_N/D$, $\Gamma_S/D$ and $\Delta/D$. Here…

Nuclear Theory · Physics 2009-11-10 A. J. Sargeant , M. S. Hussein , M. P. Pato , N. Takigawa , M. Ueda

We describe the decay out of a superdeformed band using the methods of reaction theory. Assuming that decay-out occurs due to equal coupling (on average) to a sea of equivalent chaotic normally deformed (ND) states, we calculate the average…

Nuclear Theory · Physics 2009-11-10 M. S. Hussein , A. J. Sargeant , M. P. Pato , N. Takigawa , M. Ueda

The attenuation factor F responsible for the decay out of a superdeformed (SD) band is calculated with the help of a statistical model. This factor is given by 1/F = (1 + Gamma(down) / Gamma(S)). Here, Gamma(S) is the width for the…

Nuclear Theory · Physics 2009-01-23 H. A. Weidenmueller , P. von Brentano , B. R. Barrett

We present analytic formulae for the energy average and variance of the intraband decay intensity of a superdeformed band.

Nuclear Theory · Physics 2015-06-26 M. S. Hussein , A. J. Sargeant , M. P. Pato , M. Ueda

Recent models of the decay out of superdeformed bands can broadly be divided into two categories. One approach is based on the similarity between the tunneling process involved in the decay and that involved in the fusion of heavy ions, and…

Nuclear Theory · Physics 2009-11-11 A. N. Wilson , A. J. Sargeant , P. M. Davidson , M. S Hussein

The attenuation of the intraband intensity of a superdeformed band, which results from mixing with normally deformed configurations, is calculated using reaction theory. It is found that the sharp increase of the attenuation is mostly due…

Nuclear Theory · Physics 2009-11-07 A. J. Sargeant , M. S. Hussein , M. P. Pato , N. Takigawa , M. Ueda

A new expression for the branching ratio for the decay via the E1 process in the normal-deformed band of superdeformed nuclei is given within a simple two-level model. Using this expression, the spreading or tunneling width Gamma^downarrow…

Nuclear Theory · Physics 2009-11-10 D. M. Cardamone , C. A. Stafford , B. R. Barrett

The history and importance of superdeformation in nuclei is briefly discussed. A simple two-level model is then employed to obtain an elegant expression for the branching ratio for the decay via the E1 process in the normal-deformed band of…

Nuclear Theory · Physics 2009-11-11 B. R. Barrett , D. M. Cardamone , C. A. Stafford

We compare a multi-level statistical model with a two-level model for the decay out of superdeformed rotational bands in atomic nuclei. We conclude that while the models depend on different dimensionless combinations of the input parameters…

Nuclear Theory · Physics 2009-11-11 A. J. Sargeant , M. S. Hussein , A. N. Wilson

Recent theoretical investigations of the decay mechanism out of a superdeformed nuclear band have yielded qualitatively different results, depending on the relative values of the relevant decay widths. We present a simple two-level model…

Nuclear Theory · Physics 2009-10-31 C. A. Stafford , B. R. Barrett

Superdeformed nuclei in the 190 mass region exhibit a striking universality in their decay-out profiles. We show that this universality can be explained in the two-level model of superdeformed decay as related to a strong separation of…

Nuclear Theory · Physics 2008-11-26 D. M. Cardamone , B. R. Barrett , C. A. Stafford

We choose the Reduction Formula, PCAC and Low Energy Theory to reduce the $S$ matrix of a OZI allowed two-body strong decay involving a light pseudoscalar, the covariant transition amplitude formula with relativistic wave functions as input…

High Energy Physics - Phenomenology · Physics 2022-03-30 Guo-Li Wang , Wei Li , Tai-Fu Feng , Ying-Long Wang , Yu-Bin Liu

From a comparison of the total gamma-spectra calculated for different functional dependencies of level density and radiative strength functions, there were obtained both their square root relative differences and analogous data for the used…

Nuclear Experiment · Physics 2010-09-27 A. M. Sukhovoj , V. A. Khitrov

Superdeformed (SD) states in $^{40}$Ar have been studied using the deformed-basis antisymmetrized molecular dynamics. Low energy states were calculated by the parity and angular momentum projection (AMP) and the generator coordinate method…

We examine the interplay between disorder and fractionality in a one-dimensional tight-binding Anderson model. In the absence of disorder, we observe that the two lowest energy eigenvalues detach themselves from the bottom of the band, as…

Disordered Systems and Neural Networks · Physics 2022-05-25 Mario I. Molina

This paper presents a new method to obtain the deformation distribution on the main reflector of an antenna only by measuring the electric intensity on a spherical surface with the focal point as the center of the sphere, regardless of…

Instrumentation and Methods for Astrophysics · Physics 2021-12-08 Qian Ye , Boyang Wang , Qiang Yao , Jinqing Wang , Qinghui Liu , Zhiqiang Shen

We formulate a linear difference equation which yields averaged semi-inclusive decay rates for arbitrary, not necessarily large, values of the masses. We show that the rates for decays $M \to m+\M'$ of typical heavy open strings are…

High Energy Physics - Theory · Physics 2009-11-07 Juan L. Manes

The behavior of coupled disordered one-dimensional systems, as modelled by identical fermionic Hubbard chains with the on-site potential disorder and coupling emerging through the inter-chain hopping $t'$, is analysed. The study is…

Disordered Systems and Neural Networks · Physics 2016-10-12 Peter Prelovšek

We estimate the decay width difference $\Delta Gamma_d / \Gamma_d$ in the $B_d$ system including $1/m_b$ contributions and next-to-leading order QCD corrections, and find it to be around 0.3%. We explicitly show that the time measurements…

High Energy Physics - Phenomenology · Physics 2011-01-27 A. S. Dighe , T. Hurth , C. S. Kim , T. Yoshikawa
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