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Table 2 Numerical solutions for HgH molecule \(\mu = 1.0031\begin{array}{*{20}c} , & {D_{e} = 0.46130} \\ \end{array} \begin{array}{*{20}c} {\begin{array}{*{20}c} , & {D_{1} = 0.5} \\ \end{array} } & {\hbar = 1.0} \\ \end{array}\)

From: Bound state solutions and thermodynamic properties of modified exponential screened plus Yukawa potential

n

l

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.312\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.312\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.312\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.312\)

0

0

− 0.974788199

1

− 0.5426529864

2

− 0.980486992

3

− 0.6782794

1

0

− 0.542652986

1

− 0.678279427

2

− 1.399850241

3

− 0.9804869

2

0

− 0.678279427

1

− 0.980486992

2

− 1.924173282

3

− 1.3998502

3

0

− 0.980486992

1

− 1.39985024

2

− 2.549277298

3

− 1.9241732

4

0

− 1.399850241

1

− 1.92417328

2

− 3.273416733

3

− 2.5492772

5

0

− 1.924173286

1

− 2.54927729

2

− 4.095757694

3

− 3.2734167

6

0

− 2.549277298

1

− 3.27341673

2

− 5.015860975

3

− 4.0957576

7

0

− 3.273416733

1

− 4.09575769

2

− 6.033477393

3

− 5.0158609

8

0

− 4.095757694

1

− 5.0158609754

2

− 7.148457039

3

− 6.0334773