Table 1 Bound state energy eigenvalues (eV) of the HHP at different values of quantum states, topological defect and fractional parameter, with \(\delta = 0.025\).

From: Eigensolutions of generalized fractional Schrödinger equation with Hulthén–Hellmann potential and topological defects

n

l

\(\beta = 0.35\)

\(\beta = 0.65\)

\(\beta = 0.85\)

 

\(\sigma =0.20\)

\(\sigma =0.50\)

\(\sigma =0.70\)

\({\sigma =1.00}\)

\(\sigma =0.20\)

\(\sigma =0.50\)

\(\sigma =0.70\)

\({\sigma =1.00}\)

\(\sigma =0.20\)

\(\sigma =0.50\)

\(\sigma =0.70\)

\({\sigma =1.00}\)

0

0

-127.2317

-20.3466

-10.3748

-5.0773

-52.4360

-8.3793

-4.2691

-2.0856

-47.5107

-7.5913

-3.8670

-1.8886

1

0

-31.7812

-5.0600

-2.5672

-1.2431

-13.0946

-2.0806

-1.0533

-0.5078

-11.8667

-1.8870

-0.9561

-0.4619

1

-0.8207

-0.5740

-0.4634

-0.3455

-0.7151

-0.4303

-0.3217

-0.2187

-0.7019

-0.4147

-0.3075

-0.2074

2

0

-14.1026

-2.2268

-1.1192

-0.5314

-5.8085

-0.9137

-0.4575

-0.2160

-5.2657

-0.8306

-0.4173

-0.1984

1

-0.6981

-0.4112

-0.3044

-0.2041

-0.5674

-0.2775

-0.1891

-0.1160

-0.5522

-0.2649

-0.1795

-0.1099

2

-0.2486

-0.1735

-0.1394

-0.1028

-0.2170

-0.1307

-0.0975

-0.0662

-0.2132

-0.1264

-0.0939

-0.0635

3

0

-7.9143

-1.2346

-0.6121

-0.2827

-3.2581

-0.5054

-0.2494

-0.1149

-2.9553

-0.4611

-0.2291

-0.1072

1

-0.6002

-0.3065

-0.2117

-0.1305

-0.4603

-0.1918

-0.1222

-0.0699

-0.4451

-0.1822

-0.1160

-0.0669

2

-0.2250

-0.1398

-0.1053

-0.0715

-0.1880

-0.0982

-0.0685

-0.0434

-0.1837

-0.0945

-0.0659

-0.0420

3

-0.1038

-0.0705

-0.0555

-0.0398

-0.0901

-0.0526

-0.0387

-0.0264

-0.0884

-0.0510

-0.0375

-0.0258

4

0

-5.0496

-0.7753

-0.3777

-0.1685

-2.0776

-0.3166

-0.1537

-0.0695

-1.8860

-0.2903

-0.1426

-0.0662

1

-0.5209

-0.2352

-0.1532

-0.0878

-0.3802

-0.1391

-0.0842

-0.0464

-0.3657

-0.1321

-0.0803

-0.0450

2

-0.2044

-0.1141

-0.0812

-0.0514

-0.1641

-0.0758

-0.0503

-0.0311

-0.1597

-0.0729

-0.0486

-0.0305

3

-0.0962

-0.0594

-0.0444

-0.0300

-0.0807

-0.0421

-0.0297

-0.0205

-0.0790

-0.0408

-0.0290

-0.0203

4

-0.0457

-0.0295

-0.0226

-0.0161

-0.0391

-0.0217

-0.0161

-0.0127

-0.0384

-0.0211

-0.0158

-0.0127