Pub Date : 2024-03-19DOI: 10.1142/s0218127424500512
Jing Yuan, Lijuan Ning, Ze Li
Tri-rhythmical nature has attracted extensive attention from scholars in describing the dynamical behaviors of self-sustained systems. In this paper, we consider a tri-rhythmic van der Pol system and give a bifurcation analysis of a stochastic tri-rhythmic self-sustained system under joint noise perturbation. Based on an approximate approach, we give the stationary probability density function of amplitudes, and we find that the noise and time-delay feedback, regulating the velocity time-delay feedback strength parameter, may not cause transitions among unimodal, bimodal and trimodal in the tri-rhythmic system. More stochastic bifurcations appear by regulating the time delay in this system. The system, surprisingly, undergoes five times of stochastic bifurcations when the time delay is monotonically increased. It is shown that the time delay is more sensitive to the tri-rhythmic system and a much stronger dependence on the system. From a biological point of view, the reaction rate of biological molecules can be enhanced or diminished by the change of the noise intensity or correlation time of Gaussian colored noise. More surprisingly, an increase in displacement feedback will delay the reaction rate; however, the effect of an increase in velocity feedback on the reaction rate depends on the time delay. A detailed research on the parameter space indicates that time delay and colored noise parameters can effectively control the multirhythmicity of the system. Finally, this paper verifies the effectiveness of the theoretical solution through the numerical results of Monte Carlo simulation of the original system. These results may help to further explore forking bifurcations in real-world applications. This research provides new insight into the understanding of nontrivial effects of joint noise on the tri-rhythmic system.
{"title":"Bifurcation Regulations Induced by Joint Noise in a Tri-Rhythmic Van Der Pol System","authors":"Jing Yuan, Lijuan Ning, Ze Li","doi":"10.1142/s0218127424500512","DOIUrl":"https://doi.org/10.1142/s0218127424500512","url":null,"abstract":"<p>Tri-rhythmical nature has attracted extensive attention from scholars in describing the dynamical behaviors of self-sustained systems. In this paper, we consider a tri-rhythmic van der Pol system and give a bifurcation analysis of a stochastic tri-rhythmic self-sustained system under joint noise perturbation. Based on an approximate approach, we give the stationary probability density function of amplitudes, and we find that the noise and time-delay feedback, regulating the velocity time-delay feedback strength parameter, may not cause transitions among unimodal, bimodal and trimodal in the tri-rhythmic system. More stochastic bifurcations appear by regulating the time delay in this system. The system, surprisingly, undergoes five times of stochastic bifurcations when the time delay is monotonically increased. It is shown that the time delay is more sensitive to the tri-rhythmic system and a much stronger dependence on the system. From a biological point of view, the reaction rate of biological molecules can be enhanced or diminished by the change of the noise intensity or correlation time of Gaussian colored noise. More surprisingly, an increase in displacement feedback will delay the reaction rate; however, the effect of an increase in velocity feedback on the reaction rate depends on the time delay. A detailed research on the parameter space indicates that time delay and colored noise parameters can effectively control the multirhythmicity of the system. Finally, this paper verifies the effectiveness of the theoretical solution through the numerical results of Monte Carlo simulation of the original system. These results may help to further explore forking bifurcations in real-world applications. This research provides new insight into the understanding of nontrivial effects of joint noise on the tri-rhythmic system.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"2 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140205355","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-19DOI: 10.1142/s0218127424500445
Hidetaka Ito, Naohiko Inaba
<p>In previous works [Inaba & Kousaka, 2020; Inaba & Tsubone, 2020; Inaba <i>et al.</i>, 2023], significant bifurcation structures referred to as nested Mixed-Mode Oscillations (MMOs) were found to be present in forced Bonhoeffer–van der Pol (BVP) oscillators. It is well known that unnested Mixed-Mode Oscillation-Incrementing Bifurcations (MMOIBs) can generate <span><math altimg="eq-00001.gif" display="inline" overflow="scroll"><mo stretchy="false">[</mo><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>,</mo><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub><mo stretchy="false">×</mo><mi>m</mi><mo stretchy="false">]</mo></math></span><span></span> oscillations (i.e. <span><math altimg="eq-00002.gif" display="inline" overflow="scroll"><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> followed by <span><math altimg="eq-00003.gif" display="inline" overflow="scroll"><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> repeated <span><math altimg="eq-00004.gif" display="inline" overflow="scroll"><mi>m</mi></math></span><span></span> times) for successive values of <span><math altimg="eq-00005.gif" display="inline" overflow="scroll"><mi>m</mi></math></span><span></span>, where <span><math altimg="eq-00006.gif" display="inline" overflow="scroll"><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> and <span><math altimg="eq-00007.gif" display="inline" overflow="scroll"><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> are adjacent fundamental simple MMOs, e.g. <span><math altimg="eq-00008.gif" display="inline" overflow="scroll"><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><msup><mrow><mn>1</mn></mrow><mrow><mi>s</mi></mrow></msup></math></span><span></span> and <span><math altimg="eq-00009.gif" display="inline" overflow="scroll"><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><msup><mrow><mn>1</mn></mrow><mrow><mi>s</mi><mo stretchy="false">+</mo><mn>1</mn></mrow></msup></math></span><span></span>, where <span><math altimg="eq-00010.gif" display="inline" overflow="scroll"><mi>s</mi></math></span><span></span> is an integer. Furthermore, it has been confirmed that MMOIBs can generate nested MMOs. Let two adjacent unnested MMOIB-generated MMOs be denoted <span><math altimg="eq-00011.gif" display="inline" overflow="scroll"><msub><mrow><mi>A</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy="false">(</mo><mo>=</mo><mo stretchy="false">[</mo><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>,</mo><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub><mo stretchy="false">×</mo><mi>m</mi><mo stretchy="false">]</mo><mo stretchy="false">)</mo></math></span><span></span> and <span><math altimg="eq-00012.gif" display="inline" overflow="scroll"><msub><mrow><mi>B</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy="false">(</mo>
{"title":"Analysis of Successive Doubly Nested Mixed-Mode Oscillations","authors":"Hidetaka Ito, Naohiko Inaba","doi":"10.1142/s0218127424500445","DOIUrl":"https://doi.org/10.1142/s0218127424500445","url":null,"abstract":"<p>In previous works [Inaba & Kousaka, 2020; Inaba & Tsubone, 2020; Inaba <i>et al.</i>, 2023], significant bifurcation structures referred to as nested Mixed-Mode Oscillations (MMOs) were found to be present in forced Bonhoeffer–van der Pol (BVP) oscillators. It is well known that unnested Mixed-Mode Oscillation-Incrementing Bifurcations (MMOIBs) can generate <span><math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">[</mo><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>,</mo><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub><mo stretchy=\"false\">×</mo><mi>m</mi><mo stretchy=\"false\">]</mo></math></span><span></span> oscillations (i.e. <span><math altimg=\"eq-00002.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> followed by <span><math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> repeated <span><math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"><mi>m</mi></math></span><span></span> times) for successive values of <span><math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"><mi>m</mi></math></span><span></span>, where <span><math altimg=\"eq-00006.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> and <span><math altimg=\"eq-00007.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span><span></span> are adjacent fundamental simple MMOs, e.g. <span><math altimg=\"eq-00008.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><msup><mrow><mn>1</mn></mrow><mrow><mi>s</mi></mrow></msup></math></span><span></span> and <span><math altimg=\"eq-00009.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><msup><mrow><mn>1</mn></mrow><mrow><mi>s</mi><mo stretchy=\"false\">+</mo><mn>1</mn></mrow></msup></math></span><span></span>, where <span><math altimg=\"eq-00010.gif\" display=\"inline\" overflow=\"scroll\"><mi>s</mi></math></span><span></span> is an integer. Furthermore, it has been confirmed that MMOIBs can generate nested MMOs. Let two adjacent unnested MMOIB-generated MMOs be denoted <span><math altimg=\"eq-00011.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>A</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy=\"false\">(</mo><mo>=</mo><mo stretchy=\"false\">[</mo><msub><mrow><mi>A</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>,</mo><msub><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msub><mo stretchy=\"false\">×</mo><mi>m</mi><mo stretchy=\"false\">]</mo><mo stretchy=\"false\">)</mo></math></span><span></span> and <span><math altimg=\"eq-00012.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>B</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy=\"false\">(</mo>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"266 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140202300","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-19DOI: 10.1142/s0218127424500524
Zhouchao Wei, Fanrui Wang
We take into consideration two different kinds of two-parameter bifurcations in a class of 3D linear Filippov systems, namely pseudo-Bautin bifurcation and boundary equilibrium bifurcations for two scenarios. The bifurcation conditions for generating rich dynamic behaviors are established. The main objective is to investigate the effects of two parameters interacting simultaneously on a variety of dynamic phenomena. In order to analyze the pseudo-Bautin bifurcation, we build the Poincaré map and analyze the number of fixed points whose types are related to the crossing limit cycles. In order to analyze boundary equilibrium bifurcations for two scenarios, we perform an analysis on the existence and admissibility of equilibria. Besides, a comprehensive investigation on hidden attractors induced by boundary equilibrium bifurcations is conducted. The novelty resides in overcoming the constraints of previous studies that solely take into account the dynamics of individual parameter variations. We innovatively characterize the two-parameter bifurcation mechanism of a new class of Filippov systems, and qualitatively demonstrate the coexistence of hidden attractor and stable pseudo-equilibrium.
{"title":"Two-Parameter Bifurcations and Hidden Attractors in a Class of 3D Linear Filippov Systems","authors":"Zhouchao Wei, Fanrui Wang","doi":"10.1142/s0218127424500524","DOIUrl":"https://doi.org/10.1142/s0218127424500524","url":null,"abstract":"<p>We take into consideration two different kinds of two-parameter bifurcations in a class of 3D linear Filippov systems, namely pseudo-Bautin bifurcation and boundary equilibrium bifurcations for two scenarios. The bifurcation conditions for generating rich dynamic behaviors are established. The main objective is to investigate the effects of two parameters interacting simultaneously on a variety of dynamic phenomena. In order to analyze the pseudo-Bautin bifurcation, we build the Poincaré map and analyze the number of fixed points whose types are related to the crossing limit cycles. In order to analyze boundary equilibrium bifurcations for two scenarios, we perform an analysis on the existence and admissibility of equilibria. Besides, a comprehensive investigation on hidden attractors induced by boundary equilibrium bifurcations is conducted. The novelty resides in overcoming the constraints of previous studies that solely take into account the dynamics of individual parameter variations. We innovatively characterize the two-parameter bifurcation mechanism of a new class of Filippov systems, and qualitatively demonstrate the coexistence of hidden attractor and stable pseudo-equilibrium.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"23 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140196384","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-16DOI: 10.1142/s0218127424300088
Ta-Jen Peng, Ping-Huan Kuo, Wei-Cheng Huang, Cheng-Chi Wang
Symmetric Aerostatic Cavities Bearing (SACB) systems have attracted increasing attention in the field of high-precision machinery, particularly rotational mechanisms applied at ultra-high speeds. In an air bearing system, the air bearing serves as the main support, and the load-carrying capacity is not as high as that of oil film bearings. However, the aero-spindle can operate at considerably high rotational speeds with relatively lower heat generated from rotation compared with that of oil film bearings. In addition, the operating environment of air bearings does not easily cause the rotor to deform. Hence, through adequate design, air pressure systems exhibit a certain level of stability. In general, the pressure distribution function of air bearings exhibits strong nonlinearity when there are changes in the rotor mass or rotational speed, or when the bearing system is inadequately designed. These issues may lead to instabilities in the rotor, such as unpredictable nonperiodic movements, rotor collisions, or even chaotic movements under certain parameters. In this study, rotor oscillation was analyzed using the maximum Lyapunov exponent to identify whether chaotic behavior occurred. Machine learning methods were then used to establish models and predict the rotor behavior. Especially, random forest and extreme gradient boosting were combined to develop a new model and confirm whether this model offered higher prediction performance and more accurate results in predicting tendencies with considerable changes compared with other models. The results can be effectively used to predict the SACB system and prevent nonlinear behavior from occurring.
{"title":"Nonlinear Dynamic Analysis and Forecasting of Symmetric Aerostatic Cavities Bearing Systems","authors":"Ta-Jen Peng, Ping-Huan Kuo, Wei-Cheng Huang, Cheng-Chi Wang","doi":"10.1142/s0218127424300088","DOIUrl":"https://doi.org/10.1142/s0218127424300088","url":null,"abstract":"<p>Symmetric Aerostatic Cavities Bearing (SACB) systems have attracted increasing attention in the field of high-precision machinery, particularly rotational mechanisms applied at ultra-high speeds. In an air bearing system, the air bearing serves as the main support, and the load-carrying capacity is not as high as that of oil film bearings. However, the aero-spindle can operate at considerably high rotational speeds with relatively lower heat generated from rotation compared with that of oil film bearings. In addition, the operating environment of air bearings does not easily cause the rotor to deform. Hence, through adequate design, air pressure systems exhibit a certain level of stability. In general, the pressure distribution function of air bearings exhibits strong nonlinearity when there are changes in the rotor mass or rotational speed, or when the bearing system is inadequately designed. These issues may lead to instabilities in the rotor, such as unpredictable nonperiodic movements, rotor collisions, or even chaotic movements under certain parameters. In this study, rotor oscillation was analyzed using the maximum Lyapunov exponent to identify whether chaotic behavior occurred. Machine learning methods were then used to establish models and predict the rotor behavior. Especially, random forest and extreme gradient boosting were combined to develop a new model and confirm whether this model offered higher prediction performance and more accurate results in predicting tendencies with considerable changes compared with other models. The results can be effectively used to predict the SACB system and prevent nonlinear behavior from occurring.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"42 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140205354","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-15DOI: 10.1142/s0218127424500299
Abdelaziz Salah Saidi, Muneer Parayangat, Mohamed Ali Rakrouki, Saad M. Saad, Naser El Naily
In this paper, we propose a novel codimension-three-parameter bifurcation analysis of equilibria and limit cycles when integrating Renewable Energy Sources (RESs) power plants with an exponential static load model. The study investigates the effect of solar photovoltaic generation margin, wind power generation margin, and loading factor on the local bifurcation of the modified IEEE nine-bus system. The proposed technique considers the real case of the West System Coordination Council (WSCC), the western states of the USA, by using specific models of RES power plants and static loads. The proposed technique helps to create a set of linearly varying parameters for critical operating points of nonlinear systems. The study explores detailed voltage stability analysis through the examination of bifurcation diagrams. The Hopf, limit-induced, and saddle-node bifurcation branches are identified, defining the parameter space’s stable and unstable operational regions. Additionally, the stability regions surrounding the equilibrium points are diligently explored, clarifying the consequences that various bifurcations may exert on these regions. The study offered in this proposed work aids in determining the best ways to monitor and improve these margins while considering system variables and load design.
{"title":"Multiparameter Bifurcation Analysis of Power Systems Integrating Large-Scale Solar Photovoltaic and Wind Farms Power Plants","authors":"Abdelaziz Salah Saidi, Muneer Parayangat, Mohamed Ali Rakrouki, Saad M. Saad, Naser El Naily","doi":"10.1142/s0218127424500299","DOIUrl":"https://doi.org/10.1142/s0218127424500299","url":null,"abstract":"<p>In this paper, we propose a novel codimension-three-parameter bifurcation analysis of equilibria and limit cycles when integrating Renewable Energy Sources (RESs) power plants with an exponential static load model. The study investigates the effect of solar photovoltaic generation margin, wind power generation margin, and loading factor on the local bifurcation of the modified IEEE nine-bus system. The proposed technique considers the real case of the West System Coordination Council (WSCC), the western states of the USA, by using specific models of RES power plants and static loads. The proposed technique helps to create a set of linearly varying parameters for critical operating points of nonlinear systems. The study explores detailed voltage stability analysis through the examination of bifurcation diagrams. The Hopf, limit-induced, and saddle-node bifurcation branches are identified, defining the parameter space’s stable and unstable operational regions. Additionally, the stability regions surrounding the equilibrium points are diligently explored, clarifying the consequences that various bifurcations may exert on these regions. The study offered in this proposed work aids in determining the best ways to monitor and improve these margins while considering system variables and load design.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"28 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140196380","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-12DOI: 10.1142/s0218127424500160
Quanquan Yao, Peiyong Zhu
<p>Let <span><math altimg="eq-00001.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy="false">)</mo></math></span><span></span> be a linear dynamical system, where <span><math altimg="eq-00002.gif" display="inline" overflow="scroll"><mi>X</mi></math></span><span></span> is a separable Banach space and <span><math altimg="eq-00003.gif" display="inline" overflow="scroll"><mi>T</mi><mo>:</mo><mi>X</mi><mo>→</mo><mi>X</mi></math></span><span></span> is a bounded linear operator. We show that if <span><math altimg="eq-00004.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy="false">)</mo></math></span><span></span> is invertible, then <span><math altimg="eq-00005.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy="false">)</mo></math></span><span></span> is weakly sensitive compact if and only if <span><math altimg="eq-00006.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy="false">)</mo></math></span><span></span> is thickly weakly sensitive compact; and that there exists a system <span><math altimg="eq-00007.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo stretchy="false">×</mo><mi>Y</mi><mo>,</mo><mi>T</mi><mo stretchy="false">×</mo><mi>S</mi><mo stretchy="false">)</mo></math></span><span></span> such that:</p><table border="0" list-type="order" width="95%"><tr><td valign="top">(1)</td><td colspan="5" valign="top"><p><span><math altimg="eq-00008.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo stretchy="false">×</mo><mi>Y</mi><mo>,</mo><mi>T</mi><mo stretchy="false">×</mo><mi>S</mi><mo stretchy="false">)</mo></math></span><span></span> is cofinitely weakly sensitive compact;</p></td></tr><tr><td valign="top">(2)</td><td colspan="5" valign="top"><p><span><math altimg="eq-00009.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy="false">)</mo></math></span><span></span> and <span><math altimg="eq-00010.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>Y</mi><mo>,</mo><mi>S</mi><mo stretchy="false">)</mo></math></span><span></span> are weakly sensitive compact; and</p></td></tr><tr><td valign="top">(3)</td><td colspan="5" valign="top"><p><span><math altimg="eq-00011.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy="false">)</mo></math></span><span></span> and <span><math altimg="eq-00012.gif" display="inline" overflow="scroll"><mo stretchy="false">(</mo><mi>Y</mi><mo>,</mo><mi>S</mi><mo stretchy="false">)</mo></math></span><span></span> are not syndetically weakly sensitive compact.</p></td></tr></table><p>We also show that if <span><math altimg="eq-00013.gif" display="inline" overflow="scroll"><mo stretchy="false">(
设 (X,T) 是线性动力系统,其中 X 是可分离的巴拿赫空间,T:X→X 是有界线性算子。我们证明,如果(X,T)是可逆的,那么当且仅当(X,T)是厚弱敏感紧凑时,(X,T)才是弱敏感紧凑的;并且存在这样一个系统(X×Y,T×S):(1)(X×Y,T×S)是共弱敏感紧凑的;(2)(X,T)和(Y,S)是弱敏感紧凑的;(3)(X,T)和(Y,S)不是联合弱敏感紧凑的。我们还证明,如果 (X,T) 是弱敏感紧凑的,其中 X 是复巴纳赫空间,那么 T 的谱满足单位圆。
{"title":"Weak Sensitive Compactness for Linear Operators","authors":"Quanquan Yao, Peiyong Zhu","doi":"10.1142/s0218127424500160","DOIUrl":"https://doi.org/10.1142/s0218127424500160","url":null,"abstract":"<p>Let <span><math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">)</mo></math></span><span></span> be a linear dynamical system, where <span><math altimg=\"eq-00002.gif\" display=\"inline\" overflow=\"scroll\"><mi>X</mi></math></span><span></span> is a separable Banach space and <span><math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"><mi>T</mi><mo>:</mo><mi>X</mi><mo>→</mo><mi>X</mi></math></span><span></span> is a bounded linear operator. We show that if <span><math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">)</mo></math></span><span></span> is invertible, then <span><math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">)</mo></math></span><span></span> is weakly sensitive compact if and only if <span><math altimg=\"eq-00006.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">)</mo></math></span><span></span> is thickly weakly sensitive compact; and that there exists a system <span><math altimg=\"eq-00007.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo stretchy=\"false\">×</mo><mi>Y</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">×</mo><mi>S</mi><mo stretchy=\"false\">)</mo></math></span><span></span> such that:</p><table border=\"0\" list-type=\"order\" width=\"95%\"><tr><td valign=\"top\">(1)</td><td colspan=\"5\" valign=\"top\"><p><span><math altimg=\"eq-00008.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo stretchy=\"false\">×</mo><mi>Y</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">×</mo><mi>S</mi><mo stretchy=\"false\">)</mo></math></span><span></span> is cofinitely weakly sensitive compact;</p></td></tr><tr><td valign=\"top\">(2)</td><td colspan=\"5\" valign=\"top\"><p><span><math altimg=\"eq-00009.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">)</mo></math></span><span></span> and <span><math altimg=\"eq-00010.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>Y</mi><mo>,</mo><mi>S</mi><mo stretchy=\"false\">)</mo></math></span><span></span> are weakly sensitive compact; and</p></td></tr><tr><td valign=\"top\">(3)</td><td colspan=\"5\" valign=\"top\"><p><span><math altimg=\"eq-00011.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>X</mi><mo>,</mo><mi>T</mi><mo stretchy=\"false\">)</mo></math></span><span></span> and <span><math altimg=\"eq-00012.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(</mo><mi>Y</mi><mo>,</mo><mi>S</mi><mo stretchy=\"false\">)</mo></math></span><span></span> are not syndetically weakly sensitive compact.</p></td></tr></table><p>We also show that if <span><math altimg=\"eq-00013.gif\" display=\"inline\" overflow=\"scroll\"><mo stretchy=\"false\">(","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"1 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140154037","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-12DOI: 10.1142/s0218127424500196
Soumitra Pal, Sarbari Karmakar, Saheb Pal, Nikhil Pal, A. K. Misra, Joydev Chattopadhyay
To reduce the chance of predation, many prey species adopt group defense mechanisms. While it is commonly believed that such defense mechanisms lead to positive feedback on prey density, a closer observation reveals that it may impact the growth rate of species. This is because individuals invest more time and effort in defense rather than reproductive activities. In this study, we delve into a predator–prey system where predator-induced fear influences the birth rate of prey, and the prey species exhibit group defense mechanism. We adopt a nonmonotonic functional response to govern the predator–prey interaction, which effectively captures the group defense mechanism. We present a detailed mathematical analysis, encompassing the determination of feasible equilibria and their stability conditions. Through the analytical approach, we demonstrate the occurrence of Hopf and Bogdanov–Takens (BT) bifurcations. We observe two distinct types of bistabilities in the system: one between interior and predator-free equilibria, and another between limit cycle and predator-free equilibrium. Our findings reveal that the parameters associated with group defense and predator-induced fear play significant roles in the survival and extinction of populations.
{"title":"Impact of Fear and Group Defense on the Dynamics of a Predator–Prey System","authors":"Soumitra Pal, Sarbari Karmakar, Saheb Pal, Nikhil Pal, A. K. Misra, Joydev Chattopadhyay","doi":"10.1142/s0218127424500196","DOIUrl":"https://doi.org/10.1142/s0218127424500196","url":null,"abstract":"<p>To reduce the chance of predation, many prey species adopt group defense mechanisms. While it is commonly believed that such defense mechanisms lead to positive feedback on prey density, a closer observation reveals that it may impact the growth rate of species. This is because individuals invest more time and effort in defense rather than reproductive activities. In this study, we delve into a predator–prey system where predator-induced fear influences the birth rate of prey, and the prey species exhibit group defense mechanism. We adopt a nonmonotonic functional response to govern the predator–prey interaction, which effectively captures the group defense mechanism. We present a detailed mathematical analysis, encompassing the determination of feasible equilibria and their stability conditions. Through the analytical approach, we demonstrate the occurrence of Hopf and Bogdanov–Takens (BT) bifurcations. We observe two distinct types of bistabilities in the system: one between interior and predator-free equilibria, and another between limit cycle and predator-free equilibrium. Our findings reveal that the parameters associated with group defense and predator-induced fear play significant roles in the survival and extinction of populations.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"23 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140154128","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-12DOI: 10.1142/s0218127424500159
Shaoli Wang, Tengfei Wang, Xiyan Bai, Shaoping Ji, Tianhai Tian
Tumor immune escape refers to the inability of the immune system to clear tumor cells, which is one of the major obstacles in designing effective treatment schemes for cancer diseases. Although clinical studies have led to promising treatment outcomes, it is imperative to design theoretical models to investigate the long-term treatment effects. In this paper, we develop a mathematical model to study the interactions among tumor cells, immune escape tumor cells, and T lymphocyte. The chimeric antigen receptor (CAR) T-cell therapy is also described by the mathematical model. Bifurcation analysis shows that there exists backward bifurcation and saddle-node bifurcation when the immune intensity is used as the bifurcation parameter. The proposed model also exhibits bistability when its parameters are located between the saddle-node threshold and backward bifurcation threshold. Sensitivity analysis is performed to illustrate the effects of different mechanisms on the backward bifurcation threshold and basic immune reproduction number. Simulation studies confirm the bifurcation analysis results and predict various types of treatment outcomes using different CAR T-cell therapy strengths. Analysis and simulation results show that the immune intensity can be used to control the tumor size, but it has no effect on the control of the immune escape tumor size. The introduction of the CAR T-cell therapy will reduce the immune escape tumor size and the treatment effect depends on the CAR T-cell therapy strength.
肿瘤免疫逃逸是指免疫系统无法清除肿瘤细胞,这是设计癌症疾病有效治疗方案的主要障碍之一。虽然临床研究取得了可喜的治疗效果,但设计理论模型来研究长期治疗效果也势在必行。本文建立了一个数学模型来研究肿瘤细胞、免疫逃逸肿瘤细胞和 T 淋巴细胞之间的相互作用。数学模型还描述了嵌合抗原受体(CAR)T 细胞疗法。分岔分析表明,当使用免疫强度作为分岔参数时,存在向后分岔和鞍节点分岔。当参数位于鞍节点阈值和向后分叉阈值之间时,所提出的模型也表现出双稳态。通过敏感性分析,说明了不同机制对向后分叉阈值和基本免疫繁殖数的影响。模拟研究证实了分叉分析结果,并预测了使用不同 CAR T 细胞疗法强度的各类治疗结果。分析和模拟结果表明,免疫强度可以用来控制肿瘤大小,但对控制免疫逃逸肿瘤大小没有影响。CAR T 细胞疗法的引入将减少免疫逃逸肿瘤的大小,治疗效果取决于 CAR T 细胞疗法的强度。
{"title":"Bistability and Bifurcations of Tumor Dynamics with Immune Escape and the Chimeric Antigen Receptor T-Cell Therapy","authors":"Shaoli Wang, Tengfei Wang, Xiyan Bai, Shaoping Ji, Tianhai Tian","doi":"10.1142/s0218127424500159","DOIUrl":"https://doi.org/10.1142/s0218127424500159","url":null,"abstract":"<p>Tumor immune escape refers to the inability of the immune system to clear tumor cells, which is one of the major obstacles in designing effective treatment schemes for cancer diseases. Although clinical studies have led to promising treatment outcomes, it is imperative to design theoretical models to investigate the long-term treatment effects. In this paper, we develop a mathematical model to study the interactions among tumor cells, immune escape tumor cells, and T lymphocyte. The chimeric antigen receptor (CAR) T-cell therapy is also described by the mathematical model. Bifurcation analysis shows that there exists backward bifurcation and saddle-node bifurcation when the immune intensity is used as the bifurcation parameter. The proposed model also exhibits bistability when its parameters are located between the saddle-node threshold and backward bifurcation threshold. Sensitivity analysis is performed to illustrate the effects of different mechanisms on the backward bifurcation threshold and basic immune reproduction number. Simulation studies confirm the bifurcation analysis results and predict various types of treatment outcomes using different CAR T-cell therapy strengths. Analysis and simulation results show that the immune intensity can be used to control the tumor size, but it has no effect on the control of the immune escape tumor size. The introduction of the CAR T-cell therapy will reduce the immune escape tumor size and the treatment effect depends on the CAR T-cell therapy strength.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"15 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140154129","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-12DOI: 10.1142/s021812742450041x
Fasma Diele, Deborah Lacitignola, Angela Monti
Bursting behaviors, driven by environmental variability, can substantially influence ecosystem services and functions and have the potential to cause abrupt population breakouts in host–parasitoid systems. We explore the impact of environment on the host–parasitoid interaction by investigating separately the effect of grazing-dependent habitat variation on the host density and the effect of environmental fluctuations on the average host population growth rate. We hence focus on the discrete host–parasitoid Beddington–Free–Lawton model and show that a more comprehensive mathematical study of the dynamics behind the onset of on–off intermittency in host–parasitoid systems may be achieved by considering a deterministic, chaotic system that represents the dynamics of the environment. To this aim, some of the key model parameters are allowed to vary in time according to an evolution law that can exhibit chaotic behavior. Fixed points and stability properties of the resulting 3D nonlinear discrete dynamical system are investigated and on–off intermittency is found to emerge strictly above the blowout bifurcation threshold. We show, however, that, in some cases, this phenomenon can also emerge in the sub-threshold. We hence introduce the novel concept of long-term reactivity and show that it can be considered as a necessary condition for the onset of on–off intermittency. Investigations in the time-dependent regimes and kurtosis maps are provided to support the above results. Our study also suggests how important it is to carefully monitor environmental variability caused by random fluctuations in natural factors or by anthropogenic disturbances in order to minimize its effects on throphic interactions and protect the potential function of parasitoids as biological control agents.
{"title":"On–Off Intermittency and Long-Term Reactivity in a Host–Parasitoid Model with a Deterministic Driver","authors":"Fasma Diele, Deborah Lacitignola, Angela Monti","doi":"10.1142/s021812742450041x","DOIUrl":"https://doi.org/10.1142/s021812742450041x","url":null,"abstract":"<p>Bursting behaviors, driven by environmental variability, can substantially influence ecosystem services and functions and have the potential to cause abrupt population breakouts in host–parasitoid systems. We explore the impact of environment on the host–parasitoid interaction by investigating separately the effect of grazing-dependent habitat variation on the host density and the effect of environmental fluctuations on the average host population growth rate. We hence focus on the discrete host–parasitoid Beddington–Free–Lawton model and show that a more comprehensive mathematical study of the dynamics behind the onset of on–off intermittency in host–parasitoid systems may be achieved by considering a deterministic, chaotic system that represents the dynamics of the environment. To this aim, some of the key model parameters are allowed to vary in time according to an evolution law that can exhibit chaotic behavior. Fixed points and stability properties of the resulting 3D nonlinear discrete dynamical system are investigated and on–off intermittency is found to emerge strictly above the blowout bifurcation threshold. We show, however, that, in some cases, this phenomenon can also emerge in the sub-threshold. We hence introduce the novel concept of long-term reactivity and show that it can be considered as a necessary condition for the onset of on–off intermittency. Investigations in the time-dependent regimes and kurtosis maps are provided to support the above results. Our study also suggests how important it is to carefully monitor environmental variability caused by random fluctuations in natural factors or by anthropogenic disturbances in order to minimize its effects on throphic interactions and protect the potential function of parasitoids as biological control agents.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"23 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140154122","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-12DOI: 10.1142/s021812742450024x
Michiru Katayama, Kenji Ikeda, Tetsushi Ueta
Chaos intermittency is composed of a laminar regime, which exhibits almost periodic motion, and a burst regime, which exhibits chaotic motion; it is known that in chaos intermittency, switching between these regimes occurs irregularly. In the laminar regime of chaos intermittency, the periodic solution before the saddle node bifurcation is closely related to its generation, and its behavior becomes periodic in a short time; the laminar is not, however, a periodic solution, and there are no unstable periodic solutions nearby. Most chaos control methods cannot be applied to the problem of stabilizing a laminar response to a periodic solution since they refer to information about unstable periodic orbits. In this paper, we demonstrate a control method that can be applied to the control target with laminar phase of a dynamical system exhibiting chaos intermittency. This method records the time series of a periodic solution prior to the saddle node bifurcation as a pseudo-periodic orbit and feeds it back to the control target. We report that when this control method is applied to a circuit model, laminar motion can be stabilized to a periodic solution via control inputs of very small magnitude, for which robust control can be obtained.
{"title":"Stabilization of Laminars in Chaos Intermittency","authors":"Michiru Katayama, Kenji Ikeda, Tetsushi Ueta","doi":"10.1142/s021812742450024x","DOIUrl":"https://doi.org/10.1142/s021812742450024x","url":null,"abstract":"<p>Chaos intermittency is composed of a laminar regime, which exhibits almost periodic motion, and a burst regime, which exhibits chaotic motion; it is known that in chaos intermittency, switching between these regimes occurs irregularly. In the laminar regime of chaos intermittency, the periodic solution before the saddle node bifurcation is closely related to its generation, and its behavior becomes periodic in a short time; the laminar is not, however, a periodic solution, and there are no unstable periodic solutions nearby. Most chaos control methods cannot be applied to the problem of stabilizing a laminar response to a periodic solution since they refer to information about unstable periodic orbits. In this paper, we demonstrate a control method that can be applied to the control target with laminar phase of a dynamical system exhibiting chaos intermittency. This method records the time series of a periodic solution prior to the saddle node bifurcation as a pseudo-periodic orbit and feeds it back to the control target. We report that when this control method is applied to a circuit model, laminar motion can be stabilized to a periodic solution via control inputs of very small magnitude, for which robust control can be obtained.</p>","PeriodicalId":50337,"journal":{"name":"International Journal of Bifurcation and Chaos","volume":"16 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140154298","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}