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Table 3 Numerical solutions for ZnH molecule \(\mu = 0.9928\begin{array}{*{20}c} , & {D_{e} = 0.950352} \\ \end{array} \begin{array}{*{20}c} {\begin{array}{*{20}c} , & {D_{1} = 0.5} \\ \end{array} } & {\hbar = 1.0} \\ \end{array}\)

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

n

l

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.25\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.25\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.25\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.25\)

0

0

− 3.01741831265237

1

− 0.966141947220305

2

− 0.7261720947266

3

− 0.80743496303

1

0

− 0.96614194722030

1

− 0.726172094726617

2

− 0.8074349630339

3

− 1.02635346095

2

0

− 0.72617209472661

1

− 0.807434963033923

2

− 1.0263534609508

3

− 1.33762934519

3

0

− 0.80743496303392

1

− 1.026353460950897

2

− 1.3376293451965

3

− 1.72574152059

4

0

− 1.02635346095089

1

− 1.337629345196561

2

− 1.7257415205973

3

− 2.18420664567

5

0

− 1.33762934519656

1

− 1.725741520597305

2

− 2.1842066456738

3

− 2.70992743930

6

0

− 1.72574152059730

1

− 2.184206645673870

2

− 2.7099274393012

3

− 3.30127259166

7

0

− 2.18420664567387

1

− 2.709927439301256

2

− 3.3012725916680

3

− 3.95731658770

8

0

− 2.70992743930125

1

− 3.3012725916680234

2

− 3.9573165877025

3

− 4.67750262235