Hund's rule in the (1s2s)1,3S states of the two-electron Debye atom

We present an investigation of the (1s2s)1,3S excited states of the two-electron atom immersed in a plasma modeled by the Debye or screened Coulomb potential. Three variants of the Debye atom are considered. The validity of Hund's multiplicity rule is confirmed, and the contribution of the interparticle repulsion energy to the singlet-triplet splitting is examined. The feature that this system shares with the unscreened two-electron atom as well as with the confined two-electron atom and the two-electron quantum dot is that the triplet wave function is contracted relative to that of the singlet. This feature affects both the behavior of the 2s-electron ionization energies and the relative magnitudes of the interparticle repulsion energies in the singlet vs. the triplet. Debye screening of the one-body attraction effectively reduces the nuclear charge, enhancing the reversal of the relative magnitudes of the triplet vs. singlet interparticle repulsion energies. Debye screening of the interparticle repulsion acts in an opposite way.We present an investigation of the (1s2s)1,3S excited states of the two-electron atom immersed in a plasma modeled by the Debye or screened Coulomb potential. Three variants of the Debye atom are considered. The validity of Hund's multiplicity rule is confirmed, and the contribution of the interparticle repulsion energy to the singlet-triplet splitting is examined. The feature that this system shares with the unscreened two-electron atom as well as with the confined two-electron atom and the two-electron quantum dot is that the triplet wave function is contracted relative to that of the singlet. This feature affects both the behavior of the 2s-electron ionization energies and the relative magnitudes of the interparticle repulsion energies in the singlet vs. the triplet. Debye screening of the one-body attraction effectively reduces the nuclear charge, enhancing the reversal of the relative magnitudes of the triplet vs. singlet interparticle repulsion energies. Debye screening of the interparticle repulsio...

[1]  Jesus M. Ugalde,et al.  BOUND EXCITED STATES OF H- AND HE- IN THE STATICALLY SCREENED COULOMB POTENTIAL , 1998 .

[2]  X. López,et al.  Atomic and molecular bound ground states of the Yukawa potential , 1997 .

[3]  Winkler Detachment energies for a negative hydrogen ion embedded in a variety of Debye plasmas. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[4]  E. Castro,et al.  Critical screening parameters for screened Coulomb potentials , 1991 .

[5]  H. Graboske,et al.  BOUND EIGENSTATES OF THE STATIC SCREENED COULOMB POTENTIAL. , 1970 .

[6]  Yang Wang,et al.  Tune-out wavelengths for helium atom in plasma environments , 2016 .

[7]  H. James,et al.  On the Convergence of the Hylleraas Variational Method , 1937 .

[8]  C. Pekeris,et al.  Ground State of Two-Electron Atoms , 1958 .

[9]  E. Buend́ıa,et al.  Singlet vs. triplet interelectronic repulsion in confined atoms , 2018, Chemical Physics Letters.

[10]  Y. P. Varshni,et al.  Ionization energy of the helium atom in a plasma , 1983 .

[11]  P. Mukherjee,et al.  and states of two electron atoms under Debye plasma screening , 2010 .

[12]  Zishi Jiang,et al.  Energies and transition wavelengths for two-electron atoms under Debye screening , 2015 .

[13]  E. Davidson Single‐Configuration Calculations on Excited States of Helium. II , 1964 .

[14]  J. Katriel,et al.  Atomic vs. quantum dot open shell spectra. , 2017, The Journal of chemical physics.

[15]  Yi Wang,et al.  Dynamic Polarizability for Metastable Helium in Debye Plasmas , 2016 .

[16]  J. Katriel An interpretation of Hund's rule , 1972 .

[17]  Daniel Jean Baye,et al.  Generalised meshes for quantum mechanical problems , 1986 .

[18]  D. Baye,et al.  Confined hydrogen atom by the Lagrange-mesh method: energies, mean radii, and dynamic polarizabilities. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[19]  Y. K. Ho,et al.  Calculation of screened Coulomb potential matrices and its application to He bound and resonant states , 2014 .

[20]  T. N. Chang,et al.  Atomic photoionization in a changing plasma environment , 2013 .

[21]  Vrscay Hydrogen atom with a Yukawa potential: Perturbation theory and continued-fractions-Padé approximants at large order. , 1986, Physical review. A, General physics.

[22]  Winkler,et al.  Pair-function calculations for two-electron systems in model plasma environments. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[23]  A. Solovyova,et al.  Calculations of properties of screened He-like systems using correlated wave functions. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.

[24]  Geerd H. F. Diercksen,et al.  On the influence of the Debye screening on the spectra of two-electron atoms , 2002 .

[25]  M. N. Guimarães,et al.  A study of the confined hydrogen atom using the finite element method , 2005 .

[26]  M. Hesse,et al.  Lagrange-mesh calculations of excited states of three-body atoms and molecules , 2001 .

[27]  Daniel Jean Baye,et al.  The Lagrange-mesh method , 2015 .

[28]  Daniel Jean Baye,et al.  Lagrange-mesh calculations of three-body atoms and molecules , 1999 .

[29]  G. Diercksen,et al.  Origin of the first Hund rule and the structure of Fermi holes in two-dimensional He-like atoms and two-electron quantum dots , 2012 .

[30]  J. Katriel A study of the interpretation of Hund's rule , 1972 .

[31]  Jacob Katriel,et al.  Critical screening in the one- and two-electron Yukawa atoms , 2018 .

[32]  Yew Kam Ho,et al.  Quantum entanglement for helium atom in the Debye plasmas , 2015 .