scholarly journals Ground-state configuration of neutron-rich Al35 via Coulomb breakup

2017 ◽  
Vol 96 (3) ◽  
Author(s):  
S. Chakraborty ◽  
Ushasi Datta ◽  
T. Aumann ◽  
S. Beceiro-Novo ◽  
K. Boretzky ◽  
...  
Keyword(s):  
Ground State ◽  
Coulomb Breakup ◽  
Ground State Configuration ◽  
State Configuration

scholarly journals Ground-state configuration of neutron-rich Aluminum isotopes through Coulomb Breakup

2014 ◽  
Vol 66 ◽  
pp. 02019 ◽  
Author(s):  
S. Chakraborty ◽  
U. Datta Pramanik ◽  
T. Aumann ◽  
S. Beceiro ◽  
K. Boretzky ◽  
...  
Keyword(s):  
Ground State ◽  
Coulomb Breakup ◽  
Ground State Configuration ◽  
State Configuration

GROUND-STATE CONFIGURATION OF THE NEUTRON-RICH 11BE AND 17,19,21,23O NUCLEI STUDIED BY COULOMB BREAKUP

2003 ◽  
Author(s):  
R. PALIT ◽  
T. AUMANN ◽  
K. BORETZKY ◽  
B.V. CARLSON ◽  
D. CORTINA ◽  
...  
Keyword(s):  
Ground State ◽  
Coulomb Breakup ◽  
Ground State Configuration ◽  
State Configuration

scholarly journals Observables in inhomogeneous ground states at large global charge

2021 ◽  
Vol 2021 (8) ◽  
Author(s):  
Simeon Hellerman ◽  
Nozomu Kobayashi ◽  
Shunsuke Maeda ◽  
Masataka Watanabe
Keyword(s):  
Ground State Energy ◽  
Ground State ◽  
State Energy ◽  
Point Function ◽  
Ground State Configuration ◽  
Charge Densities ◽  
Direct Extension ◽  
Fixed Set ◽  
State Configuration ◽  
Large Charge

Abstract As a sequel to previous work, we extend the study of the ground state configuration of the D = 3, Wilson-Fisher conformal O(4) model. In this work, we prove that for generic ratios of two charge densities, ρ1/ρ2, the ground-state configuration is inhomogeneous and that the inhomogeneity expresses itself towards longer spatial periods. This is the direct extension of the similar statements we previously made for ρ1/ρ2 ≪ 1. We also compute, at fixed set of charges, ρ1, ρ2, the ground state energy and the two-point function(s) associated with this inhomogeneous configuration on the torus. The ground state energy was found to scale (ρ1 + ρ2)3/2, as dictated by dimensional analysis and similarly to the case of the O(2) model. Unlike the case of the O(2) model, the ground also strongly violates cluster decomposition in the large-volume, fixed-density limit, with a two-point function that is negative definite at antipodal points of the torus at leading order at large charge.

The ground-state configuration of Zr90

1964 ◽  
Vol 11 (2) ◽  
pp. 140-141 ◽  
Author(s):  
J.L. Yntema
Keyword(s):  
Ground State ◽  
Ground State Configuration ◽  
State Configuration

scholarly journals Investigation of M1 transitions of the ground-state configuration of In-like tungsten

2016 ◽  
Vol 49 (10) ◽  
pp. 105002 ◽  
Author(s):  
W Li ◽  
J Xiao ◽  
Z Shi ◽  
Z Fei ◽  
R Zhao ◽  
...  
Keyword(s):  
Ground State ◽  
Ground State Configuration ◽  
State Configuration

An Investigation on the Fine Structure Levels in the Ground State Configuration for the Antimony Anion

2014 ◽  
Vol 69 (8-9) ◽  
pp. 397-402
Author(s):  
Leyla Özdemir ◽  
Sadiye Tuna
Keyword(s):  
Fine Structure ◽  
Ground State ◽  
Transition Probabilities ◽  
Relativistic Effects ◽  
Electric Quadrupole ◽  
Radiative Transition ◽  
Ground State Configuration ◽  
Hartree Fock ◽  
First Time ◽  
State Configuration

We have investigated the correlation, relativistic, and isotope shift effects on the fine structure levels in the ground state configuration for the antimony anion ( Sb-). Energies and radiative transition probabilities (for magnetic dipole, M1, and electric quadrupole, E2) have been obtained using the multiconfiguration Hartree-Fock method within the framework of the Breit-Pauli Hamiltonian. Therefore, the most important configuration interaction and relativistic effects have been included. Comparisons with other available works are presented. For some M1 and E2 lines the considered transition probabilities are reported for the first time

Ground-state configuration of double acceptors in silicon and germanium

1990 ◽  
Vol 42 (14) ◽  
pp. 8975-8981 ◽  
Author(s):  
Andreas Giesekus ◽  
L. M. Falicov
Keyword(s):  
Ground State ◽  
Ground State Configuration ◽  
Silicon And Germanium ◽  
State Configuration

Magnetic Moments of Five Levels in the Ground-State Configuration of Ni and Oii

1970 ◽  
Vol 2 (5) ◽  
pp. 1651-1655 ◽  
Author(s):  
V. Beltrán-López ◽  
Teodoro González E.
Keyword(s):  
Ground State ◽  
Magnetic Moments ◽  
Ground State Configuration ◽  
State Configuration

Ground-state configuration of 173Ta

1983 ◽  
Vol 133 (1-2) ◽  
pp. 44-46 ◽  
Author(s):  
R. Eder ◽  
E. Hagn ◽  
E. Zech
Keyword(s):  
Ground State ◽  
Ground State Configuration ◽  
State Configuration

SIC-LSD study of δ-Pu and PuO2±x

2003 ◽  
Vol 802 ◽  
Author(s):  
L. Petit ◽  
A. Svane ◽  
Z. Szotek ◽  
W. M. Temmerman
Keyword(s):  
Spin Density ◽  
Ground State ◽  
Electronic Structures ◽  
The Self ◽  
Local Spin Density Approximation ◽  
Density Approximation ◽  
Ground State Configuration ◽  
Local Spin ◽  
Δ Phase ◽  
State Configuration

ABSTRACTThe electronic structures of actinide solid systems are calculated using the self-interaction corrected local spin density approximation. Within this scheme the 5f electron manifold is considered to consist of both localized and delo-calized states, and by varying their relative proportions the energetically most favourable (ground state) configuration can be established. Specifically, we discuss elemental Pu in its δ-phase, and the effects of adding O to PuO2.

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