<i>Introductory Nuclear Physics</i>

Wong, S.S.M.; Kalelkar, M.

doi:10.1063/1.2810763

Cited by 50 publications

(47 citation statements)

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“…The relation between ϑ and gamma energy E is given by [26]: (12) and the relation between E and is given by [27]:…”

Section: Methods and Calculationsmentioning

confidence: 99%

Microscopic description of energy-levels for even-even 124-134Xe isotopes

Ahmed

2017

AIP Conference Proceedings

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Abstract.The first measured excited states 1 2 E and the ratio of the second to the first measured excited states, the back-bending, the E-GOS and the ratio among the energies of the (I+2) and (I) states as a function of the spin (I) have been drawn to determine the properties of the ground-states band. The odd-even staggering has been drawn to determine the difference between the energies of ground states band (GSB) and negative parity band (NPB). Bohr-Mottelson Model ( BM ), Interacting Boson Model ( IBM-1 ), Interacting Vector Boson Model ( IVBM ) and Doma-El-Gendy (D-G) relation have been used to calculate the energy levels of (GSB), IBM-1 has been used to calculate the energy of the gamma band (GB), while IVBM and BM have been used to calculate the energy levels of (NPB). The calculated energy levels in comparison with the measured data indicated the quality of the fitness presented in this work.

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“…The relation between ϑ and gamma energy E is given by [26]: (12) and the relation between E and is given by [27]:…”

Section: Methods and Calculationsmentioning

confidence: 99%

Microscopic description of energy-levels for even-even 124-134Xe isotopes

Ahmed

2017

AIP Conference Proceedings

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“…The g-factors are constants with values (Wong, 1998) g ℓ = 1 for proton 0f o rn e u t r o n : g s = 5.585695 for proton −3.826085 for neutron (35) The integrals in equations (32), (33) and (34) can be analytically evaluated (Rampho, 2010). As an illustration the evaluation of the variational energy is summarized.…”

Section: Will-be-set-by-in-techmentioning

confidence: 99%

Antisymmetrized Molecular Dynamics and Nuclear Structure

Rampho¹,

Sofianos²

2012

Molecular Dynamics - Theoretical Developments and Applications in Nanotechnology and Energy

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“…and are constants: = 2.87 fm and = 67.4 fm 2 [34,37]. We know that the deuteron consists of two nucleons.…”

Section: The Hyperfine Interactionmentioning

confidence: 99%

“…We know that = 1/ = 0.714 (fm −1 ) [34], by using of (24), we can get amount of parameters , , , and :…”

Section: Isrn High Energy Physicsmentioning

confidence: 99%

Exact Solution of the Dirac Equation for the Yukawa Potential with Scalar and Vector Potentials and Tensor Interaction

Azizi

Salehi

Rajabi

2013

ISRN High Energy Physics

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We present exact solutions of the Dirac equation with Yukawa potential in the presence of a Coulomb-like tensor potential. For this goal we expand the Yukawa form of the nuclear potential in its mesonic clouds by using Taylor extension to the power of seventh and bring out its simple form. In order to obtain the energy eigenvalue and the corresponding wave functions in closed forms for this potential (with great powers and inverse exponent), we use ansatz method. We also regard the effects of spin-spin, spin-isospin, and isospin-isospin interactions on the relativistic energy spectra of nucleon. By using the obtained results, we have calculated the deuteron mass. The results of our model show that the deuteron spectrum is very close to the ones obtained in experiments.

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Introductory Nuclear Physics

Cited by 50 publications

References 0 publications

Microscopic description of energy-levels for even-even 124-134Xe isotopes

Microscopic description of energy-levels for even-even 124-134Xe isotopes

Antisymmetrized Molecular Dynamics and Nuclear Structure

Exact Solution of the Dirac Equation for the Yukawa Potential with Scalar and Vector Potentials and Tensor Interaction

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