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Table 2 Numerical results of \(\Gamma _{ q}(\theta + \vartheta + \lambda +1)\), \(\Gamma _{ q}(\theta + \vartheta + \lambda )\), \(\Gamma _{ q}( \lambda + 1)\), \(\Gamma _{ q}(\theta + \vartheta +1)\), \(\Gamma _{ q}(\theta + \vartheta )\), \(\Gamma _{ q}(\theta + \vartheta + \lambda -\mu +1)\), \(\Gamma _{ q}(\theta + \vartheta + \lambda -\mu )\), \(\Gamma _{ q}(\theta -\mu +1)\), and \(\aleph _{1}\), \(\aleph _{2}\) of \(\mathbb{F}\mathrm{D}q-\mathbb{DP}\) (24) with \(q=\frac{1}{2}\)

From: On a Duffing-type oscillator differential equation on the transition to chaos with fractional q-derivatives

n

\(q = \frac{1}{2}\)

\(\Gamma _{ q}(\theta + \vartheta + \lambda +1)\)

\(\Gamma _{ q}(\theta + \vartheta + \lambda )\)

\(\Gamma _{ q}(\lambda + 1 )\)

\(\Gamma _{ q}(\theta + \vartheta +1)\)

\(\Gamma _{ q}(\theta + \vartheta )\)

\(\aleph _{1}\)

1

2.8428

1.9971

2.4929

2.2164

2.0510

1.1087

2

2.6015

1.9154

2.6121

2.0773

2.0696

1.1497

3

2.4936

1.8780

2.6690

2.0144

2.0783

1.1710

9

2.3945

1.8431

2.7233

1.9562

2.0866

1.1924

10

2.3938

1.8429

2.7237

1.9558

2.0867

1.1926

11

2.3934

1.8427

2.7239

1.9556

2.0867

1.1927

12

2.3932

1.8427

2.7240

1.9554

2.0867

1.1927

13

2.3931

1.8426

2.7241

1.9554

2.0867

1.1927

14

2.3930

1.8426

2.7241

1.9554

2.0867

15

2.3930

1.8426

2.7241

1.9554

2.0867

1.1928

16

2.3930

1.8426

2.7241

1.9553

2.0867

1.1928

17

2.3930

1.8426

2.7241

1.9553

2.0867

1.1928

n

\(\Gamma _{ q}(\theta + \vartheta + \lambda -\mu +1)\)

\(\Gamma _{ q}(\theta + \vartheta + \lambda -\mu )\)

\(\Gamma _{ q}( \theta -\mu +1)\)

\(\aleph _{2}\)

1

2.5368

1.9488

3.6511

0.6997

2

2.3418

1.9037

3.9742

0.7367

3

2.2542

1.8829

4.1309

0.7561

11

2.1726

1.8631

4.2842

0.7760

12

2.1725

1.8631

4.2845

13

2.1724

1.8631

4.2846

0.7761

14

2.1724

1.8630

4.2847

0.7761

15

2.1724

1.8630

4.2847

0.7761

16

2.1723

1.8630

4.2848

0.7761

17

2.1723

1.8630

4.2848

0.7761