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Article

Piecewise Business Bubble System under Classical and Nonsingular Kernel of Mittag–Leffler Law

1
School of Management, Hefei University of Technology, Hefei 230002, China
2
School of Finance, Anhui University of Finance and Economics, Bengbu 233030, China
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Entropy 2023, 25(3), 459; https://doi.org/10.3390/e25030459
Submission received: 1 February 2023 / Revised: 1 March 2023 / Accepted: 5 March 2023 / Published: 6 March 2023

Abstract

:
This study aims to investigate the dynamics of three agents in the emerging business bubble model based on the Mittag–Leffler law pertaining to the piecewise classical derivative and non-singular kernel. By generalizing the business bubble dynamics in terms of fractional operators and the piecewise concept, this study presents a new perspective to the field. The entire set of intervals is partitioned into two piecewise intervals to analyse the classical order and conformable order derivatives of an Atangana–Baleanu operator. The subinterval analysis is critical for removing discontinuities in each sub-partition. The existence and uniqueness of the solution based on a piecewise global derivative are tested for the considered model. The approximate root of the system is determined using the piecewise numerically iterative technique of the Newton polynomial. Under the classical order and non-singular law, the approximate root scheme is applied to the piecewise derivative. The curve representation for the piece-wise globalised system is tested by applying the data for the classical and different conformable orders. This establishes the entire density of each compartment and shows a continuous spectrum instead of discrete dynamics. The concept of this study can also be applied to investigate crossover behaviours or abrupt changes in the dynamics of the values of each market.

1. Introduction

Our study focuses on the mechanisms of chaos and how they can be leveraged to develop new economic models using the available materials [1]. Specifically, we have discovered that the 3D saddle focusing on equilibrium points can generate spiral strange attractors that can result in unpredictable and unreliable economic behaviour, challenging the ability of an economy to reach a long-term steady equilibrium [2]. In light of these findings, we have identified various equilibria that are related to the starting values of the controlling parameters in the model. These equilibria can result in undesired low-growth equilibrium points, which can hinder economic progress. By understanding the dynamics of chaos and its potential implications for economic policy, we aim to contribute to the development of more robust and resilient economic systems.
In 2008, research was conducted to analyse the economic downturn triggered by the financial bubble in the banking sector. The collapse of the bubble caused the economy to plummet to low levels of equilibrium, resulting in the eventual collapse of the financial sector. The impact on the banking sector was evident in the reduction of household deposits which indirectly affected the lending to manufacturing firms, which resulted in a decline in the final output. The weakened state of the banking sector raised concerns over bank solvency, reduced credit availability, and eroded investor confidence, resulting in a decline in global stock markets.
Macroeconomists are facing a significant challenge in the aftermath of the recent financial crisis. Conventional macroeconomic models have ignored financial frictions and instead assumed the existence of perfect financial markets. Consequently, these models are of limited use in explaining financial crises [3,4,5,6]. Furthermore, these models tend to focus on financial frictions in non-financial firms, while overlooking the critical role of financial intermediation in the recent crisis. To gain a more comprehensive understanding of the crisis and inform policy decisions, macroeconomists must develop new models that account for the intricacies of financial markets. For more details, the readers are requested to review the published studies [7,8,9,10,11].
In this study, we consider a financial bubble model [12,13] that includes the three-dimensional system of differential equations:
d Q d t = r Q Q [ r k + ( r k r ) ξ Q ] θ ( 1 Q ) , d B d t = r B ( r k r ) Q B , d N d t = [ r k θ + ( r k r ) ξ Q ] N + ( r k r ) B .
Let Q denote the shadow price of the net worth of a bank N and B be the bubble component of the stock market value of the bank. Where θ ( 0 , 1 ) , r, and ξ ( 0 , 1 ) represent the share of bank dividends, rate of deposits, and degree of financial friction, respectively, and r k = α θ r r k r N α 1 ϑ .
Fractional calculus (FC), an extension of traditional calculus, has recently attracted considerable attention in academia [14,15]. Certain researchers argue that traditional calculus, while widely used as an analytical approach, does not significantly contribute to innovation and can be challenging for use for complex theoretical analyses. In contrast, FC provides a more flexible mathematical framework for solving problems that cannot be easily addressed using integer-order calculus. Introduced in 1967, modern calculus was popularised by Caputo in many fields [16]. However, integer-order dynamics a re limited to integer orders with a clear formulation. In contrast, fractional operators, such as the Caputo derivative, generalise the integer-order operators and are essential for solving many practical problems [17,18,19,20]. Researchers have tested various models using the Caputo framework to develop more accurate and robust fractional operators. Caputo and Fabrizio further modified the Caputo operator by introducing a non-singular kernel, and in 2016, Atangana and Baleanu proposed a new definition based on Caputo’s concept using a non-local and non-singular kernel [21,22]. Since then, researchers have conducted considerable research on these operators, exploring various mathematical properties and applications in various fields [23,24,25,26,27,28,29,30].
In a recent study, Araz and Atangana proposed a novel operator for a piecewise differential and integral [31]. The piecewise derivative is divided into two subintervals, where one subinterval is analysed using one fractional operator, and the other is analysed using a different fractional operator. This approach allows for greater flexibility and accuracy while dealing with complex systems with multiple characteristics. To address the issue of crossover behaviour dynamics, the researchers introduced a novel piecewise derivative method [31]. This new approach has been the subject of considerable discussion in the research community, with researchers exploring its potential applications in various fields. Several applications of fractional operators have already been reported in the literature [32,33,34,35,36,37]. These applications range from modelling complex physical systems, such as electrical circuits, to analysing and controlling biological processes. The versatility and effectiveness of fractional operators have rendered them an increasingly popular tool in the mathematical modelling of complex systems [38,39,40].
Using the new operator mentioned above, we analyse the model described in Equation (1) based on the non-singular Mittag–Leffler law and an integer order approach. This analysis provides valuable insights into the behaviour of the system and reveals its underlying dynamics.
Entropy 25 00459 i001
where P C A B C represents the piecewise classical and Atangana–Baleanu derivative with two subintervals in [ 0 , T ] . In the simplest form, we can write Equation (2) as
Entropy 25 00459 i002
where Entropy 25 00459 i003 and D t represent the Atangana—Baleanu and integer-order global derivative, respectively. i from i = 1 , 2 , 3 are defined in Equation (2).
The piecewise derivative of a function allows us to describe the continuity of the system on each interval, eliminating any discontinuities and rendering it differentiable. Additionally, we can apply a non-singular kernel based on the Mittag–Leffler law to the second interval which generalises the derivative and acts as a global operator. This approach provides a comprehensive description of the dynamics of the system over the entire range from 0 to 1.
The objective of this model is to examine the business dynamics of a system with three agents via a piecewise integer order approach and using a global ABC operator. This enables us to understand abrupt changes and the overall density of all agents within the system. By applying this methodology, we can gain insights into the interactions of the agents and the factors that drive changes in the system. Ultimately, this analysis enables us to make more informed decisions and better manage the system holistically.

2. Basic Results

We discuss the fundamentals of FC in addition to the piecewise Atangana–Baleanu global operator and its antiderivative.
Definition 1.
The definition of the A B C operator of the function F ( t ) under the condition F ( t ) H 1 ( 0 , T ) is
Entropy 25 00459 i004
One can replace Entropy 25 00459 i005 by Entropy 25 00459 i006 in (4) to obtain the Caputo–Fabrizio operator.
Definition 2.
Consider F ( t ) P [ 0 , T ] , then the A B C integral is
Entropy 25 00459 i007
Definition 3
([31]). Suppose F ( t ) is differentiable and the increasing mapping is f ( t ) ; accordingly, the integer-order piecewise differentiation can be formulated as
0 P F D t F ( t ) = F ( t ) , 0 < t t 1 , F ( t ) f ( t ) t 1 < t t 2 = T ,
and the integration can be written as
0 P F I t F ( t ) = 0 t F ( τ ) d τ , 0 < t t 1 , t 1 t F ( τ ) f ( τ ) d ( τ ) t 1 < t t 2 ,
where 0 P F D t F ( t ) and 0 P F I t F ( t ) are used for the classical derivative and integration for 0 < t t 1 , and the global derivative and integral for t 1 < t t 2 , respectively.
Definition 4
([31]). Let function F ( t ) be derivable; accordingly, the integer-order and global-order piecewise derivatives can be written as
Entropy 25 00459 i008
while the integration is defined as
Entropy 25 00459 i009
where 0 P F D t r F ( t ) and 0 P F I t F ( t ) are used for the integer-order derivative on 0 < t t 1 and the arbitrary-order derivative and integration for t 1 < t t 2 , respectively.

3. Theoretical Analysis

We test whether the piecewise system solution exists, and if it does, we test whether it is unique. To this end, we express the model (2) under
Entropy 25 00459 i010
as
Entropy 25 00459 i011
where
F ( t ) = Q ( t ) B ( t ) N ( t ) F 0 = Q ( 0 ) B ( 0 ) N ( 0 ) F t 1 = Q t 1 B t 1 N t 1 ( t , F ( t ) ) = i = d d t i ( Q , B , N , t ) A B C i ( Q , B , N , t ) ,
where i = 1 , 2 , 3 .
Let > t 2 t > t 1 > 0 with a closed norm space E 1 = C [ 0 , T ] have the norm defined as
F = max t [ 0 , T ] | F ( t ) | .
We use the following condition for the non-linear operator to achieve the results related to uniqueness and existence as
(A1) 
L F > 0 ; ∀ , F ¯ E we have
| ( t , F ) ( t , F ¯ ) | L | m a t h c a l F F ¯ | ,
(A2) 
C > 0 & M > 0 , ;
| ( t , F ( t ) ) | C | F | + M .
Theorem 1.
Let G be a piecewise derivative defined on the intervals 0 < t t 1 and t 1 < t t 2 on [ 0 , T ] that obeys ( A 2 ) ; accordingly, the piecewise defined derivable system (3) has a 1 root on the two subintervals.
Proof. 
By applying Schauder’s theorem of fixed point theory, we selected the close subset for both intervals of 0 , T as B of E as
B = { F E : F R 1 , 2 , R > 0 } ,
Further, we also chose a mapping T : B B and used (6) as
Entropy 25 00459 i012
On some F B ,
Entropy 25 00459 i013
This implies that, as F B , T ( B ) B . Further, this indicates that T is closed and in the given space. Moreover, for complete continuity, we process t i < t j [ 0 , t 1 ] for the 1st interval of integer derivative and assume
Entropy 25 00459 i055
Equation (9) implies t j t i ; accordingly,
| T ( F ) ( t i ) T ( F ) ( t j ) | 0 , as t j t i .
Hence, T is equi-continuous on the [ 0 , t 1 ] set of the interval. Next, we consider the second set of interval t p , t r [ t 1 , T ] in terms of A B C as
Entropy 25 00459 i014
Equation (10) implies t n t m , and accordingly,
Entropy 25 00459 i030
Therefore, T is equi-continuous in the [ t 1 , t 2 ] set of the interval, and therefore, T is the equi-continuous operator. Based on the Ascoli–Arzelá result, the operator T is completely continuous, which implies that T is continuously uniform with bounds. Finally, based on Schauder’s findings of the fixed point theory, the piecewise global derivative model (3) has at least one root on every set of partitioned intervals. □
Theorem 2.
According to assumption ( A 1 ) , the suggested piecewise problem has one solution if T is constructed.
Proof. 
Previously, we defined T : B B to be piecewise continuous, and we considered F and F ¯ B on [ 0 , t 1 ] in the integer-order derivative as
T ( F ) T ( F ¯ ) = max t [ 0 , t 1 ] | 0 t 1 G ( Z , F ( Z ) ) d Z 0 t 1 G ( Z , F ¯ ( Z ) ) d Z | t 1 L G F F ¯ .
Equation (11) implies that
T ( F ) T ( F ¯ ) t 1 L G F F ¯ .
In this equation, T is the contracted operator. Therefore, based on the findings of Banach’s theorem of contraction, the investigated system has one root in the set of all intervals. Furthermore, for other sets of intervals t [ t 1 , t 2 ] through the global A B C operator,
Entropy 25 00459 i015
From (13), we have
Entropy 25 00459 i016
Thus, operator T is contracted. Finally, based on Banach’s contraction theorem, the suggested model has one root in the 2nd interval. Therefore, based on Equations (12) and (14), the piecewise derivative problem has one root on every set of the interval. □

4. Numerical Scheme

We have developed an approximate method for the piecewise global model described in Equation (3). This method involves deriving a numerical technique for each of the two sets of intervals in the context of both the integer order and A B C operator frameworks. The technique we use for the piecewise model is an integer-order technique. To apply this method to the model using Equation (3), we use a piecewise integral approach within the frameworks of the integer order and A B C operator. This approach provides a more accurate approximation of the behaviour of the system and allows us to gain valuable insights into its dynamics.
Entropy 25 00459 i017
Now, we derive the numerical technique for one of the equations of problem (15), and the remaining equations are derived similarly.
At t = t p + 1 ,
Entropy 25 00459 i056
By expressing Equation (16) in the Newton scheme of interpolation from [31] as follows:
Entropy 25 00459 i019
For the remaining two equations, we write the scheme as follows:
Entropy 25 00459 i020
Entropy 25 00459 i021
where
Entropy 25 00459 i022

5. Numerical Simulation

We have conducted various curve simulations for all three agents using the available data on both arbitrary and classical orders and time duration in days. Our simulations use the initial values of Q ( 0 ) = 1.5 , B ( 0 ) = 2.36 , and N ( 0 ) = 1.09 , along with the parameter values of α = 0.33 , δ = 0.1 , r = 0.015 , θ = 0.05 , and ξ = 0.5556 . The graphical representations are provided for the integer order and ABC operators on each interval set. Figure 1a–c depict the plots of the three classes of the proposed piecewise model for finance bubbles in the stock market on two subintervals. The first set of intervals is analysed in terms of the integer-order derivative, whereas the other interval is treated under the Atangana–Baleanu fractional operator. These show two different dynamics with bending behaviours. We observe that an increase in the shadow price of the net worth results in a decrease in the stock market bubbles and net worth quantity.
Figure 2a–c illustrate the simulation results of the three agents of the proposed piecewise model for finance bubbles in the stock market within two different subintervals. The first interval is analysed in terms of the natural-order derivative, whereas the dynamics of the other interval are considered under the Atangana–Baleanu fractional operator, displaying two different dynamics with bending behaviours. The first interval shows only natural-order dynamics on one curve, whereas the second interval shows more curve dynamics. At the beginning of the simulation, we observe a rapid increase in the shadow price of the net worth, which results in a decline in the bubbles of the stock market and the net worth quantities that tend toward zero. Here, we observe a change in the fractional orders.
Figure 3a–c display the dynamical behaviour of the three classes on another set of fractional orders of the proposed piecewise model for finance bubbles in the stock market on two subintervals. The first interval is analysed in terms of the natural-order derivative, whereas the dynamics of the other intervals are considered under the Atangana–Baleanu fractional operator, displaying two different dynamics with bending behaviours. In this set of data, we observe a greater increase in the shadow price of net worth, which moves towards stability. The bubbles of the stock market and the net worth quantities slightly decrease with time in this set of data and eventually become stable.
Figure 4a–c illustrate the plots of the three classes for the proposed piecewise model of finance bubbles in the stock market on two subintervals of classical and fractional ABC orders while considering longer time durations and changing the order of derivatives. We observe that an increase in the shadow price of the net worth results in a decrease in the bubbles of the stock market and the net worth quantity. Stability is reached rapidly in this case.
Figure 5a–c show the plots of the three classes based on a change in the value of fractional orders to small fractional orders of the considered piecewise model for the finance bubbles of the stock market on two subintervals showing the sensitivity of the fractional order parameter Entropy 25 00459 i023.
Figure 6a–c show the plots of the three classes by changing the value of δ = 0.01 for the proposed piecewise model for the finance bubbles of the stock market on two subintervals, showing the sensitivity of the said parameter on the same fractional orders as before. Here, we consider both intervals as fractional orders.
Figure 7a–c show the three classes of the proposed piecewise model for the finance bubbles of the stock market on two subintervals. The first interval is treated under the Caputo fractional derivative, and the other interval is treated under the ABC derivative. For the sensitivity of the parameter r, we change the value of r.
Figure 8a–c show the results of the three classes of the proposed piecewise model for the finance bubbles of the stock market on the two subintervals. Here, the first interval is tested in the Caputo fractional derivative, and the other interval is used for the ABC derivative. To address the sensitivity of parameter ζ , we change the value of ζ .

6. Conclusions

This paper presents a novel framework of piecewise global derivatives, which has been successfully applied to the analysis of financial bubbles in the stock market. The problem is formulated using the integer order and Atangana–Baleanu derivative on two sets of partitioned intervals, resulting in piecewise dynamics. Through a fixed point theory analysis, the existence and uniqueness of the considered problem are established for each interval. A numerical solution method is developed based on the interpolation of Newton’s polynomial in an integer order derivative for each sub-interval and the Atangana–Baleanu operator for global orders. The fractional order derivative parameter in the numerical scheme provides a continuous and density spectrum of all financial bubble agents. The numerical simulation of the total compartments provides six data points, and the piecewise influences on t 1 are analysed. The first interval is simulated in the integer order, whereas the second interval is tested at various fractional orders. All curves converge to the integer order as the derivative order increases. This type of development can be applied to various global phenomena where sudden variations occur in the dynamics of different densities, and the instability can be stabilised by dividing the time interval into two or more intervals. The study shows how shadow prices can be controlled by including various financial bubbles in the stock market to affect the net worth, demonstrating the potential applications of the framework. The control strategy is implemented more effectively on smaller fractional orders. Therefore, through this analysis, we can manage the variability in shadow prices using piecewise analysis. This is because non-linear and piecewise derivative systems can account for most of the irregular activities and dynamics.

Author Contributions

Conceptualization, B.L.; methodology, B.L.; software, B.L.; validation, B.L. and C.Z.; formal analysis, B.L. and C.Z.; data curation, B.L.; writing—original draft preparation, B.L. and C.Z.; writing—review and editing, B.L. and C.Z.; funding acquisition, B.L. All authors have read and agreed to the published version of the manuscript.

Funding

This work has been supported by Natural Science Foundation of Anhui Province (Grant No. 2008085QA09) and Science Foundation of the Anhui Education Department (Grant No. KJ2021A0482).

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Shilnikov, L.P. A case of the existence of a denumerable set of periodic motion. Sov. Math. Dokl. 1965, 6, 163–166. [Google Scholar]
  2. Bella, G.; Mattana, P.; Venturi, B. Shilnikov chaos in the Lucas model of endogenous growth. J. Econ. Theory 2017, 172, 451–477. [Google Scholar] [CrossRef]
  3. Bernanke, B.; Mark, G. VAgency costs. Net Worth and Business Fluctuations. Am. Econ. Rev. 1989, 14, 14–31. [Google Scholar]
  4. Carlstrom, C.T.; Fuerst, T.S. Agency costs, net worth, and business fluctuations: A computable general equilibrium analysis. Am. Econ. Rev. 1997, 87, 893–910. [Google Scholar]
  5. Kiyotaki, N.; Moore, J. Credit cycles. J. Political Econ. 1997, 105, 211–248. [Google Scholar] [CrossRef]
  6. Bernanke, B.S.; Gertler, M.; Gilchrist, S. The financial accelerator in a quantitative business cycle framework. Handb. Macroecon. 1999, 1, 1341–1393. [Google Scholar]
  7. Blanchard, O.; Watson, M. Bubbles, Rational Expectations and Financial Markets; D.C. Heathand Company: Lexington, MA, USA, 1982. [Google Scholar]
  8. Kocherlakota, N. Bursting Bubbles: Consequences and Cures; Federal Reserve Bank of Minneapolis: Minneapolis, MN, USA, 2009; Volume 84, Unpublished manuscript. [Google Scholar]
  9. Miao, J.; Wang, P. Bubbles and total factor productivity. Am. Econ. Rev. 2012, 102, 82–87. [Google Scholar] [CrossRef] [Green Version]
  10. Weil, P. Confidence and the real value of money in an overlapping generations economy. Q. J. Econ. 1987, 102, 1–22. [Google Scholar] [CrossRef]
  11. Miao, J.; Wang, P.; Zhou, J. Housing Bubbles and Policy Analysis; Unpublished Working Paper; Boston University and HKUST: Boston, MA, USA, 2014. [Google Scholar]
  12. Bella, G.; Mattana, P. Chaos control in presence of financial bubbles. Econ. Lett. 2020, 193, 109314. [Google Scholar] [CrossRef]
  13. Miao, J.; Wang, P. Banking bubbles and financial crises. J. Econ. Theory 2015, 157, 763–792. [Google Scholar] [CrossRef]
  14. Podlubny, I. Fractional Differential Equations, Mathematics in Science and Engineering; Academic Press: New York, NY, USA, 1999. [Google Scholar]
  15. Miller, K.S.; Ross, B. An Introduction to the Fractional Calculus and Fractional Differential Equations; John Wiley and Sons: New York, NY, USA, 1993. [Google Scholar]
  16. Schiessel, H.; Metzler, R.; Blumen, A.; Nonnenmacher, T.F. Generalized viscoelastic models: Their fractional equations with solutions. J. Phys. A 1995, 28, 6567–6584. [Google Scholar] [CrossRef]
  17. Kilbas, A.; Srivastava, H.M.; Trujillo, J. Theory and Applications of Fractional Differential Equations; Elsevier Science: Amsterdam, The Netherlands, 2006. [Google Scholar]
  18. Hilfer, R. Threefold Introduction to Fractional Derivatives. In Anomalous Transport: Foundations and Applications; Wiley-VCH Verlag: Weinheim, Germany, 2008. [Google Scholar]
  19. Miller, K.S. Fractional differential equations. J. Fract. Calc. 1993, 3, 49–57. [Google Scholar]
  20. Sabatier, J.; Agrawal, O.P.; Machado, J.A.T. Advances in Fractional Calculus; Springer: Dordrecht, The Netherlands, 2007. [Google Scholar]
  21. Caputo, M.; Fabrizio, M. A new definition of fractional derivative without singular kernel. Prog. Fract. Differ. Appl. 2015, 1, 73–85. [Google Scholar]
  22. Atangana, A.; Baleanu, D. New fractional derivatives with nonlocal and non-singular kernel: Theory and application to heat transfer model. arXiv 2016, arXiv:1602.03408. [Google Scholar] [CrossRef] [Green Version]
  23. Xuan, L.; Arfan, M.; Rahman, M.u.; Fatima, B. Analysis of SIQR type mathematical model under Atangana-Baleanu fractional differential operator. Comput. Methods Biomech. Biomed. Eng. 2022, 26, 98–112. [Google Scholar]
  24. Zhang, L.; Rahman, M.u.; Arfan, M.; Ali, A. Investigation of mathematical model of transmission co-infection TB in HIV community with a non-singular kernel. Results Phys. 2021, 28, 104559. [Google Scholar] [CrossRef]
  25. Liu, X.; ur Rahmamn, M.; Ahmad, S.; Baleanu, D.; Nadeem Anjam, Y. A new fractional infectious disease model under the non-singular Mittag–Leffler derivative. Waves Random Complex Media 2022, 1–27, Unpublished manuscript. [Google Scholar] [CrossRef]
  26. Mahmood, T.; Al-Duais, F.S.; Sun, M. Dynamics of Middle East Respiratory Syndrome Coronavirus (MERS-CoV) involving fractional derivative with Mittag-Leffler kernel. Phys. A Stat. Mech. Appl. 2022, 606, 128144. [Google Scholar] [CrossRef]
  27. Li, B.; Liang, H.; He, Q. Multiple and generic bifurcation analysis of a discrete Hindmarsh-Rose model. Chaos Solitons Fractals 2021, 146, 110856. [Google Scholar] [CrossRef]
  28. Li, B.; Liang, H.; Shi, L.; He, Q. Complex dynamics of Kopel model with nonsymmetric response between oligopolists. Chaos Solitons Fractals 2022, 156, 111860. [Google Scholar] [CrossRef]
  29. Eskandari, Z.; Avazzadeh, Z.; Ghaziani, R.K.; Li, B. Dynamics and bifurcations of a discrete-time Lotka–Volterra model using nonstandard finite difference discretization method. Math. Methods Appl. Sci. 2022; Unpublished manuscript. [Google Scholar]
  30. Li, B.; Zhang, Y.; Li, X.; Eskandari, Z.; He, Q. Bifurcation analysis and complex dynamics of a Kopel triopoly model. J. Comput. Appl. Math. 2023, 426, 115089. [Google Scholar] [CrossRef]
  31. Atangana, A.; Araz, S.I. New concept in calculus:Piecewise differential and integral operators. Chaos Soliton Fractals 2021, 145, 110638. [Google Scholar] [CrossRef]
  32. Sohail, A.; Yu, Z.; Arif, R.; Nutini, A.; Nofal, T.A. Piecewise differentiation of the fractional order CAR-T cells-SARS-2 virus model. Results Phys. 2022, 33, 105046. [Google Scholar] [CrossRef]
  33. Atangana, A.; Toufik, M. A piecewise heat equation with constant and variable order coefficients: A new approach to capture crossover behaviors in heat diffusion. AIMS Math. 2022, 7, 8374–8389. [Google Scholar] [CrossRef]
  34. Heydari, M.H.; Razzaghi, M. A numerical approach for a class of nonlinear optimal control problems with piecewise fractional derivative. Chaos Solitons Fractals 2021, 152, 111465. [Google Scholar] [CrossRef]
  35. Shah, K.; Abdeljawad, T.; Ali, A. Mathematical analysis of the Cauchy type dynamical system under piecewise equations with Caputo fractional derivative. Chaos Solitons Fractals 2022, 161, 112356. [Google Scholar] [CrossRef]
  36. Xu, C.; Liu, Z.; Pang, Y.; Saifullah, S.; Inc, M. Oscillatory, crossover behavior and chaos analysis of HIV-1 infection model using piece-wise Atangana–Baleanu fractional operator: Real data approach. Chaos, Solitons Fractals 2022, 164, 112662. [Google Scholar] [CrossRef]
  37. Mahmood, T.; Rahman, M.u.; Arfan, M.; Kayani, S.I.; Sun, M. Mathematical study of Algae as a bio-fertilizer using fractal–fractional dynamic model. Math. Comput. Simul. 2023, 203, 207–222. [Google Scholar] [CrossRef]
  38. Shah, K.; Abdeljawad, T. Study of a mathematical model of COVID-19 outbreak using some advanced analysis. Waves Random Complex Media, 2022; 1–18, Unpublished manuscript. [Google Scholar]
  39. Shah, K.; Abdeljawad, T.; Abdalla, B.; Abualrub, M.S. Utilizing fixed point approach to investigate piecewise equations with non-singular type derivative. AIMS Math. 2022, 7, 14614–14630. [Google Scholar] [CrossRef]
  40. Shah, K.; Naz, H.; Abdeljawad, T.; Abdalla, B. Study of Fractional Order Dynamical System of Viral Infection Disease under Piecewise Derivative. Comput. Model. Eng. Sci. 2023, 136, 921–941. [Google Scholar]
Figure 1. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) and ( N ( t ) ) on different arbitrary orders Entropy 25 00459 i023  = 0.99 , 0.97 , 0.95 , 0.93 and the time durations on the subintervals.
Figure 1. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) and ( N ( t ) ) on different arbitrary orders Entropy 25 00459 i023  = 0.99 , 0.97 , 0.95 , 0.93 and the time durations on the subintervals.
Entropy 25 00459 g001
Figure 2. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.99 , 0.98 , 0.97 , 0.96 , and the time durations on two sets of intervals.
Figure 2. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.99 , 0.98 , 0.97 , 0.96 , and the time durations on two sets of intervals.
Entropy 25 00459 g002aEntropy 25 00459 g002b
Figure 3. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.80 , 0.75 , 0.70 , 0.65 and the time durations on the two sets of intervals.
Figure 3. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.80 , 0.75 , 0.70 , 0.65 and the time durations on the two sets of intervals.
Entropy 25 00459 g003
Figure 4. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.60 , 0.55 , 0.50 , 0.45 , and the time durations on two set of intervals.
Figure 4. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.60 , 0.55 , 0.50 , 0.45 , and the time durations on two set of intervals.
Entropy 25 00459 g004
Figure 5. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.25 , 0.20 , 0.15 , 0.10 , and the time durations on two sets of intervals.
Figure 5. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023  = 0.25 , 0.20 , 0.15 , 0.10 , and the time durations on two sets of intervals.
Entropy 25 00459 g005
Figure 6. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023 and the time durations on the two set of intervals.
Figure 6. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023 and the time durations on the two set of intervals.
Entropy 25 00459 g006
Figure 7. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023, and the time durations on the two set of intervals.
Figure 7. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023, and the time durations on the two set of intervals.
Entropy 25 00459 g007
Figure 8. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023 and the time durations on the two set of intervals.
Figure 8. Dynamics of classes ( Q ( t ) ) , ( B ( t ) ) , and ( N ( t ) ) on different arbitrary fractional orders Entropy 25 00459 i023 and the time durations on the two set of intervals.
Entropy 25 00459 g008aEntropy 25 00459 g008b
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Zhang, C.; Li, B. Piecewise Business Bubble System under Classical and Nonsingular Kernel of Mittag–Leffler Law. Entropy 2023, 25, 459. https://doi.org/10.3390/e25030459

AMA Style

Zhang C, Li B. Piecewise Business Bubble System under Classical and Nonsingular Kernel of Mittag–Leffler Law. Entropy. 2023; 25(3):459. https://doi.org/10.3390/e25030459

Chicago/Turabian Style

Zhang, Chao, and Bo Li. 2023. "Piecewise Business Bubble System under Classical and Nonsingular Kernel of Mittag–Leffler Law" Entropy 25, no. 3: 459. https://doi.org/10.3390/e25030459

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