Bound State Solution Schrodinger Equation for Extended Cornell Potential at Finite Temperature

被引：11
作者：
Ahmadov, A., I [1 ,2 ]
Abasova, K. H. [1 ]
Orucova, M. Sh [3 ]
机构：
[1] Baku State Univ, Dept Theoret Phys, Z Khalilov St 23, AZ-1148 Baku, Azerbaijan
[2] Baku State Univ, Inst Phys Problems, Z Khalilov St 23, AZ-1148 Baku, Azerbaijan
[3] Azerbaijan State Univ Econ, Istiglaliyyat St 22, AZ-1001 Baku, Azerbaijan
来源：
ADVANCES IN HIGH ENERGY PHYSICS | 2021年 / 2021卷
关键词：
HEAVY QUARKONIA; CHARMONIUM; SPECTRUM; PLASMA; QCD;
D O I：
10.1155/2021/1861946
中图分类号：
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号：
摘要：
In this paper, we study the finite temperature-dependent Schrodinger equation by using the Nikiforov-Uvarov method. We consider the sum of the Cornell, inverse quadratic, and harmonic-type potentials as the potential part of the radial Schrodinger equation. Analytical expressions for the energy eigenvalues and the radial wave function are presented. Application of the results for the heavy quarkonia and Bc meson masses are in good agreement with the current experimental data except for zero angular momentum quantum numbers. Numerical results for the temperature dependence indicates a different behaviour for different quantum numbers. Temperature-dependent results are in agreement with some QCD sum rule results from the ground states.
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页数：13
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