Theoretical study on regularity of changes in quantum defects in Rydberg state series of many-valence electron atoms within WBEPM theory

Author(s):  
Neng Wu Zheng ◽  
Yujie Sun ◽  
Dongxia Ma ◽  
Ruyi Yang ◽  
Tao Zhou ◽  
...  
2019 ◽  
Vol 10 (26) ◽  
pp. 6494-6502 ◽  
Author(s):  
David V. Chicharro ◽  
Sonia Marggi Poullain ◽  
Alexandre Zanchet ◽  
Aymen Bouallagui ◽  
Alberto García-Vela ◽  
...  

The photochemistry of the ethyl radical following excitation to the 3p Rydberg state is investigated in a joint experimental and theoretical study.


2015 ◽  
Vol 70 (4) ◽  
pp. 265-277
Author(s):  
Marco Wendorff ◽  
Caroline Röhr

AbstractStarting from the new compound SrHg2Sn2, which is isoelectronic and also isotypic to the indide SrIn4, the successive substitution of Sn against the electron poor Hg has been investigated in a combined synthetic, crystallographic, and bond-theoretical study. Along the 1:4 section Sr(Hg1–xSnx)4 a series of compounds with Sn contents x between 0.5 and 0.2 were synthesized from stoichiometric ratios of the elements. Their crystal structures, which represent three different variants of the EuIn4-type structure, have been determined using single crystal X-ray data. The most electron rich compound SrHg2Sn2 crystallizes in the original EuIn4-type [monoclinic, C2/m, a = 1257.9(14), b = 490.1(4), c = 997.8(12) pm, β = 117.60(6)°, Z = 4, R1 = 0.0838], with a fully ordered Hg and Sn distribution. The four atom sites form two different folded ladders with an alternating Hg/Sn distribution. Like in the KHg2-type, the ladders are connected via six-membered rings. In between, double tubes with an internal Sn–Sn bond are connected via further Sn–Sn bonds to form sheets similar to those observed in SiAs. The most electron-poor phase SrHg3.2Sn0.8 crystallizes in a strongly distorted variant of this structure [a = 1172.8(4), b = 497.9(2), c = 1010.0(4) pm, β = 118.860(7)°, Z = 4, R1 = 0.0549]. Herein, additional Hg–Hg bonds are formed, and the open tubes are distorted into rods of edge-sharing rhombohedra resembling the structure motifs of elemental Hg. At an intermediate valence electron (v.e.) number, i.e., in SrHg2.5Sn1.5, an isomorphous tripled superstructure (a = 2704.4(5), b = 493.87(7), c = 1197.1(2) pm, β = 90.838(14)°, Z = 12, R1 = 0.0475) occurs, where the building blocks of the two variants of the EuIn4-type structure alternate in a 1:2 ratio. The bonding situation and the “coloring,” i.e., the Hg/Sn distribution in the polyanionic network, are discussed considering the different sizes of the atoms and the charge distribution (Bader AIM charges), which has been calculated within the framework of the FP-LAPW density functional theory for SrHg2Sn2 and the model compounds “SrHg3Sn” and “SrHg4.”


2004 ◽  
Vol 82 (7) ◽  
pp. 523-529 ◽  
Author(s):  
N W Zheng ◽  
Z Li ◽  
D Ma ◽  
T Zhou ◽  
J Fan

There are few documented values of the energy levels of the gallium atom. The values in some series remain blank and some series have no values in high Rydberg states. In this paper, based on the weakest bound electron potential model theory we treat the many-valence electron system of the excited gallium atom as a single-electron system of the weakest bound electron and use Martin's expression to determine the parameters. Most of the results are satisfying with deviations less than 1 cm–1 compared with the documented values in the National Institute of Standards and Technology. In addition, we fill many blanks in some high Rydberg energy levels of the gallium atom. PACS Nos.: 31.15.Ct, 32.10.Fn


1988 ◽  
Vol 152 (4-5) ◽  
pp. 393-396 ◽  
Author(s):  
David L. Cooper ◽  
Kate Kirby

1988 ◽  
Vol 37 (5) ◽  
pp. 831-835 ◽  
Author(s):  
S Stafström ◽  
J O Nilsson ◽  
W R Salaneck

2006 ◽  
Vol 125 (4) ◽  
pp. 044311 ◽  
Author(s):  
Yang Liu ◽  
Jian-Kang Yu ◽  
Xu-Ri Huang ◽  
Chia-Chung Sun

2021 ◽  
Vol 922 (2) ◽  
pp. 100
Author(s):  
A. M. Velasco ◽  
J. L. Alonso ◽  
P. Redondo ◽  
C. Lavín

Abstract We have theoretically determined the absorption oscillator strengths and wavenumbers for rotationally resolved transitions of the c4′1Σu + (6)-X1Σg +(0–9) bands of N2, which are relevant to analyze the spectra of planetary atmospheres. The Molecular Quantum Defect Orbital method has been used in our calculations. The interaction between the c4′1Σu + (6) Rydberg state and the b′1Σu + valence states has been considered using an adequate rovibronic energy matrix. In addition, we have calculated the lifetimes of the rotational levels of the c4′1Σu + (6) state. We hope that the reported data, most of them for the first time, can be useful in the interpretation of planetary atmospheres where N2 is present.


Author(s):  
Hong Van Nguyen ◽  
That Van Nguyen ◽  
Bong Thi Le ◽  
Huong Thi Thanh Do ◽  
Truc Thi Thanh Huynh

Na8TM (TM = Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn) clusters are optimized by DFT calculations combining the Triple zeta valence plus polarization (TZVP) method to determine magnetic torque values on orbits, point groups, electron structures, and spin density images of the atomic groups. The results indicate that Na atoms in Na8TM cluster strongly affect the total magnetic moment of the whole group of atoms. In a cluster, each Na atom contributes one electron which combines with valence electron of transition metal for creating a sum of valence electron of the cluster. Atomic groups with the highest magnetic moments are Na8V (5 B) and non-magnetic clusters are Na8Ni and Na8Zn. The electronic structure and magnetic properties of the clusters resemble those of some metals and transition metal ions. This study will orientate to substitution in magnetic materials by metal clusters.


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