Energy levels of P-wave states for a D-dimensional helium atom

2004 ◽  
Vol 322 (1-2) ◽  
pp. 96-104 ◽  
Author(s):  
Bin Duan ◽  
Xiao-Yan Gu ◽  
Zhong-Qi Ma
Keyword(s):  
P Wave ◽  
2021 ◽  
Vol 104 (7) ◽  
Author(s):  
Ming-Xiao Duan ◽  
Xiang Liu
Keyword(s):  
P Wave ◽  

2006 ◽  
Vol 174 (3) ◽  
pp. 241-251 ◽  
Author(s):  
Chao-Hsi Chang ◽  
Jian-Xiong Wang ◽  
Xing-Gang Wu
Keyword(s):  
P Wave ◽  

2018 ◽  
Vol 33 (26) ◽  
pp. 1850147
Author(s):  
Kai Lin ◽  
Xiao-Mei Kuang ◽  
Wei-Liang Qian ◽  
Qiyuan Pan ◽  
A. B. Pavan

In this work, the s-wave, p-wave and d-wave holographic superconductors in the Hořava–Lifshitz gravity are investigated in the probe limit. For this approach, it is shown that the equations of motion for different wave states in Einstein gravity can be written as a unified form, and condensates take place in all three cases. This scheme is then generalized to Hořava–Lifshitz gravity, and a unified equation for multiple holographic states is obtained. Furthermore, the properties of the condensation and the optical conductivity are studied numerically. It is found that, in the case of Hořava–Lifshitz gravity, it is always possible to find some particular parameters in the corresponding Einstein case where the condensation curves are identical. For fixed scalar field mass m, a nonvanishing [Formula: see text] makes the condensation easier than in Einstein gravity for s-wave superconductor. However, the p-wave and d-wave superconductors have T[Formula: see text] greater than the s-wave.


2021 ◽  
Vol 62 (3) ◽  
Author(s):  
E. Epelbaum ◽  
J. Gegelia ◽  
H. P. Huesmann ◽  
Ulf-G. Meißner ◽  
Xiu-Lei Ren

AbstractWe discuss the formulation of a non-relativistic effective field theory for two-body P-wave scattering in the presence of shallow states and critically address various approaches to renormalization proposed in the literature. It is demonstrated that the consistent renormalization involving only a finite number of parameters in the well-established formalism with auxiliary dimer fields corresponds to the inclusion of an infinite number of counterterms in the formulation with contact interactions only. We also discuss the implications from the Wilsonian renormalization group analysis of P-wave scattering.


2001 ◽  
Vol 64 (1) ◽  
Author(s):  
Bin Duan ◽  
Xiao-Yan Gu ◽  
Zhong-Qi Ma
Keyword(s):  

2019 ◽  
Vol 9 (1) ◽  
pp. 10 ◽  
Author(s):  
Redi Kristian Pingak ◽  
Rosara Kolmate ◽  
Bernandus Bernandus

Calculation of He atomic energy levels using the first order perturbation theory taught in the Basic Quantum Mechanics course has led to relatively large errors. To improve its accuracy, several methods have been developed but most of them are too complicated to be understood by undergraduate students. The purposes of this study are to apply a simple matrix method in calculating some of the lowest energy levels of He atom (1s2, triplet 1s2s, and singlet 1s2s states) and to reduce errors obtained from calculations using the standard perturbation theory. The convergence of solutions as a function of the number of bases is also examined. The calculation is done analytically for 3 bases and computationally with the number of bases using MATHEMATICA. First, the 2-electron wave function of the Helium atom is written as the multiplication of two He+ ion wave functions, which are then expanded into finite dimension bases. These bases are used to calculate the elements of the Hamiltonian matrix, which are then substituted back to the energy eigenvalue equation to determine the energy values of the system. Based on the calculation results, the error obtained for the He ground state energy using 3 bases is 2.51 %, smaller than the errors of the standard perturbation theory (5.28 %). Despite the fact that the error is still relatively large from the analytical calculations for singlet-triplet 1s2s energy splitting of He atom, this error is successfully reduced significantly as more bases were used in the numerical calculations. In particular, for n = 25, the current calculation error for all states is much smaller than the errors obtained from calculations using standard perturbation theory. In conclusion, the analytical calculations for the energy eigenvalue equation for the 3 lowest states of the Helium atom using 3 bases have been carried out. It was also found in this study that increasing the number of bases in our numerical calculations has significantly reduced the errors obtained from the analytical calculations.


2016 ◽  
Vol 79 (2) ◽  
pp. 243-246
Author(s):  
A. P. Martynenko ◽  
G. A. Martynenko ◽  
V. V. Sorokin ◽  
R. N. Faustov

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
E. F. Talantsev ◽  
K. Iida ◽  
T. Ohmura ◽  
T. Matsumoto ◽  
W. P. Crump ◽  
...  

Abstract The possibility of p-wave pairing in superconductors has been proposed more than five decades ago, but has not yet been convincingly demonstrated. One difficulty is that some p-wave states are thermodynamically indistinguishable from s-wave, while others are very similar to d-wave states. Here we studied the self-field critical current of NdFeAs(O,F) thin films in order to extract absolute values of the London penetration depth, the superconducting energy gap, and the relative jump in specific heat at the superconducting transition temperature, and find that all the deduced physical parameters strongly indicate that NdFeAs(O,F) is a bulk p-wave superconductor. Further investigation revealed that single atomic layer FeSe also shows p-wave pairing. In an attempt to generalize these findings, we re-examined the whole inventory of superfluid density measurements in iron-based superconductors and show quite generally that single-band weak-coupling p-wave superconductivity is exhibited in iron-based superconductors.


2004 ◽  
Vol 19 (31) ◽  
pp. 5501-5511 ◽  
Author(s):  
ALAKABHA DATTA

The three body decays [Formula: see text], may be used to measure both sin 2β and cos 2β. Crucial to the cos 2β measurement is the resonant contribution to the three body decay from p-wave excited Ds, states. If these p-wave states are the newly discovered Ds(2317) and Ds(2460) then they are below the D(*)K threshold and hence do not contribute to [Formula: see text]. The three body decays can then be used to measure sin 2β without resonant dilution and to look for new physics in [Formula: see text] transition.


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