Quasielastic scattering of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">He</mml:mi><mml:mprescripts /><mml:none /><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>on<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Be</mml:mi><mml:mprescripts /><mml:none /><mml:mrow><mml:mn>9</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>at 25 MeV/nucle

Ye, Y. L.; Pang, Dan; Jiang, D. X.; Tao, Zheng; Wang, Q. J.; Li, Z. H.; Li, X. Q.; Ge, Yufeng; Wu, Changqi; Zhang, G. L.; Wang, Jiashu; Chen, Z. Q.; Ozawa, A.; Yamaguchi, Yoshitaka; Kanungo, R.; Tanihata, I.

doi:10.1103/physrevc.71.014604

Cited by 29 publications

(11 citation statements)

References 26 publications

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“…As a result, our knowledge of nuclear physics has also been extended from stable nuclei to unstable ones. Experiments with RI beams [4][5][6][7][8][9][10][11][12][13][14][15][16] have already shown that the properties of unstable nuclei are quite different from those of stable ones [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32]. Therefore it is very interesting to investigate the properties of unstable nuclei theoretically with reliable theories or models.…”

Section: Introductionmentioning

confidence: 99%

Charge density distributions and charge form factors of theN=82andN=126isotonic nuclei

2006

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Charge form factors for N = 82 and N = 126 isotonic nuclei are calculated with the relativistic eikonal approximation, in which the charge density distributions are from the relativistic mean-field theory. The variations of charge form factors with proton number are discussed in detail. It is found that the most sensitive parts of the charge form factors are those around the minimums and maximums. For an increasing proton number, the charge form factors near the extrema have an upward shift. As the protons increase and occupy a new shell, the minimums and maximums of the charge form factors could also have a significant inward shift. The results can be useful for the study of behaviors of valence-proton wave functions for such nuclei as can be considered as a core plus proton(s), and thus the proton-halo phenomenon. In addition, the results can also be useful for future electron-unstable nucleus scattering experiments and provide tests of the reliability of the relativistic mean-field theory for the unstable nuclei.

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Section: Introductionmentioning

confidence: 99%

Charge density distributions and charge form factors of theN=82andN=126isotonic nuclei

2006

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“…One is that the behavior of the charge density distributions for the nuclei with N = 20 and 28 is very similar. The main reason for this similarity lies in that the two nuclides, for instance 42 Ti and 50 Ti, which belong to the same element have the same number of protons and the configurations of state of the protons also do not differ much. Another feature of the charge density distributions shown in Fig.…”

Section: Numerical Results and Discussionmentioning

confidence: 99%

“…In this section, we present the numerical results of the charge density distributions and charge radii from the RMF model, and the charge form factors from the REA method for the nuclei 16 O, 18 Ne, 20 Mg, 22 Si with neutron number N = 8, the nuclei 18 O, 20 Ne, 22 Mg, 24 Si, 26 S with N = 10, 40 Ca, 42 Ti, 44 Cr, 46 Fe, 48 Ni with N = 20 and 48 Ca, 50 Ti, 52 Cr, 56 Ni with N = 28. And, along with these results, we also give our detailed discussions.…”

Section: Numerical Results and Discussionmentioning

confidence: 99%

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Study of the isotonic shifts of charge form factor for the light proton-rich nuclei

Wang

Ren

2007

Nuclear Physics A

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“…Recently, the DEM has attracted much attention not only because it is completely different from the classical physics, but also, it is playing a central role in quantum information theory, quantum computation and communication, [31][32][33] quantum cryptography, [34][35][36] quantum teleportation, [37] and dense coding. [38,39] Entanglement is produced by different interactions. With the aid of the simplest model i.e., JCM; generating and observing of the DEM have been realized.…”

Section: Introductionmentioning

confidence: 99%

Single‐Atom Entanglement for a System of Directly Linked Two Cavities in the Presence of an External Classical Field: Effect of Atomic Coherence

Hanoura

Ahmed

Khalil

et al. 2019

Fortschritte der Physik

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The Hamiltonian of a system composed of two standard Jaynes‐Cummings cells connected by the overlap of evanescent cavity fields, which allows photons to hop from the first cavity to the second and vice versa, and interacting with an external classical field, is simplified in the framework of unitary canonical transformations. James's method of the effective Hamiltonian is used in the derivation of two effective Hamiltonians with two completely dispersive regimes. Analytical expressions for the time dependent wavefunction and the elements of the reduced atomic operators for the different Hamiltonians are derived. The temporal evolution of atomic quantum entropy is calculated when the fields are initially in their vacuum states with various forms of the atomic initial states. Effects of the photon hopping strength, detuning and the various forms of the atomic initial states on the evolution of the von Neumann entropies are analyzed. The impact of the time‐average technique on the features resulting due to involving the controlling parameters and their influences on the considered functions is discussed. Damping is taken into account through a non‐Hermitian Hamiltonian and results are discussed. General conclusions reached are illustrated by numerical results.

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Quasielastic scattering ofHe6onBe9at 25 MeV/nucle

Cited by 29 publications

References 26 publications

Charge density distributions and charge form factors of theN=82andN=126isotonic nuclei

Charge density distributions and charge form factors of theN=82andN=126isotonic nuclei

Study of the isotonic shifts of charge form factor for the light proton-rich nuclei

Single‐Atom Entanglement for a System of Directly Linked Two Cavities in the Presence of an External Classical Field: Effect of Atomic Coherence

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