Skip to main content

Table 4 Numerical solutions for CdH molecule \(\mu = 0.9992\begin{array}{*{20}c} , & {D_{e} = 0.766272} \\ \end{array} \begin{array}{*{20}c} {\begin{array}{*{20}c} , & {D_{1} = 0.5} \\ \end{array} } & {\hbar = 1.0} \\ \end{array}\)

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

n

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.218\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.218\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.218\)

\(l\)

\(E_{n} \,\left( {{\text{eV}}} \right),\alpha = 0.218\)

0

0

− 2.67890597455055

1

− 0.840655336712097

2

− 0.6059319955710

3

− 0.64862920647

1

0

− 0.84065533671209

1

− 0.605931995571002

2

− 0.6486292064758

3

− 0.80537061848

2

0

− 0.60593199557100

1

− 0.648629206475862

2

− 0.8053706184856

3

− 1.03584258656

3

0

− 0.64862920647586

1

− 0.805370618485624

2

− 1.0358425865628

3

− 1.32623194984

4

0

− 0.80537061848562

1

− 1.035842586562886

2

− 1.3262319498409

3

− 1.67076879081

5

0

− 1.03584258656288

1

− 1.326231949840911

2

− 1.6707687908103

3

− 2.06669665176

6

0

− 1.32623194984091

1

− 1.670768790810318

2

− 2.0666966517630

3

− 2.51256373148

7

0

− 1.6707687908103

1

− 2.066696651763026

2

− 2.5125637314828

3

− 3.00754635815

8

0

− 2.06669665176302

1

− 2.5125637314828956

2

− 3.0075463581590

3

− 3.55114899732