Nesse trabalho estudamos um laser de estado sólido sujeito a realimentação optica de frequência modificada de um ponto de vista da teoria de bifurcações. Fizemos uma an alise bastante ampla da dinâmica desse laser no espaço de dois parâmetros de injeção (a dessintonização de frequência e a intensidade da injeção) utilizando métodos de integração direta e continuação numérica. Enquanto o método de integração numérica nos possibilitou analisar as dinâmicas mais complexas, incluindo transições para o caos e hipercaos, o método de continuação numérica nos permitiu estudar curvas de bifurcações estáveis e instáveis. A análise foi realizada estudando os efeitos causados pela mudança dos parâmetros que representam o tempo de vida da inversão populacional e a saturação cruzada, responsável pelo acoplamento dos campos dentro do meio ativo. Mostramos que o parâmetro que descreve o tempo de vida da inversão populacional e responsável pelo surgimento de diversas instabilidades no sistema, como o fenômeno de multiestabilidade, surgimento de orbitas periódicas e quase-peri odicas, assim como rotas para o caos via dobramento de período e torus. Para o parâmetro de acoplamento dos campos, mostramos que ele possibilita a presença de hipercaos em nosso sistema, este podendo se apresentar no que denominamos de hipercaos \fraco" e \forte". Dentro da região de hipercaos \forte", mostramos transições determinísticas de dois regimes, em que num deles o laser opera no modo de Q-switching, enquanto que no outro o laser apresenta pequenas oscilações irregulares. Por m, mostramos a existência de uma estatística de eventos extremos dentro do regime hipercaótico. / In this work we studied a solid state laser subjected to frequency-shifted optical feedback from a bifurcation theory point of view. We performed a very broad analysis of the dynamics of this laser in the space of two injection parameters (frequency detuning and injection intensity) using direct integration and numerical continuation methods. While the numerical integration method allowed us to analyze the more complex dynamics, including chaos and hyperchaos transitions, the numerical continuation method allowed us to study stable and unstable bifurcation curves. The analysis was carried out by studying the e ects caused by the change of the parameters that represent the life time of the population inversion and the cross saturation, responsible for the coupling of the elds within the active medium. We show that the parameter that describes the life time of the population inversion is responsible for the appearance of several instabilities in the system, such as the multistability phenomenon, the appearance of periodic and quasi-periodic orbits, as well as routes to chaos via period doubling and torus . For the eld coupling parameter, we show that it allows the presence of hyperchaos in our system, which may present in what we call "weak"and "strong"hyperchaos. Within the "strong"hyperchaos region, we show deterministic transitions of two regimes, in which one laser operates in the Q-switching mode, while in the other the laser presents small irregular oscillations. Finally, we have shown the existence of a extreme events statistic within the hyperchaotic regime.

Chaos theory is well known as one of three revolutions in physical sciences in 20th-century, as one physicist called it: Relativity eliminated the Newtonian illusion of absolute space and time; quantum theory eliminated the Newtonian dream of a controllable measurable process; and chaos eliminates the Laplacian fantasy of deterministic predictability". Specially, when chaos synchronization was found in 1991, chaos theory becomes more and more attractive. Chaos has been widely applied to many scientific disciplines: mathematics, programming, microbiology, biology, computer science, economics, engineering, finance, philosophy, physics, politics, population dynamics, psychology, and robotics. One of most important engineering applications is secure communication because of the properties of random behaviours and sensitivity to initial conditions of chaos systems. Noise-like dynamical behaviours can be used to mask the original information in symmetric cryptography. Sensitivity to initial conditions and unpredictability make chaotic systems very suitable to construct one-way function in public-key cryptography. In chaos-based secure communication schemes, information signals are masked or modulated (encrypted) by chaotic signals at the transmitter and the resulting encrypted signals are sent to the corresponding receiver across a public channel (unsafe channel). Perfect chaos synchronization is usually expected to recover the original information signals. In other words, the recovery of the information signals requires the receiver's own copy of the chaotic signals which are synchronized with the transmitter ones. Thus, chaos synchronization is the key technique throughout this whole process. Due to the difficulties of generating and synchronizing chaotic systems and the limit of digital computer precision, there exist many challenges in chaos-based secure communication. In this thesis, we try to solve chaos generation and chaos synchronization problems. Starting from designing chaotic and hyperchaotic system by first-order delay differential equation, we present a family of novel cell attractors with multiple positive Lyapunov exponents. Compared with previously reported hyperchaos systems with complex mathematic structure (more than 3 dimensions), our system is relatively simple while its dynamical behaviours are very complicated. We present a systemic parameter control method to adjust the number of positive Lyapunov exponents, which is an index of chaos degree. Furthermore, we develop a delay feedback controller and apply it to Chen system to generate multi-scroll attractors. It can be generalized to Chua system, Lorenz system, Jerk equation, etc. Since chaos synchronization is the critical technique in chaos-based secure communication, we present corresponding impulsive synchronization criteria to guarantee that the receiver can generate the same chaotic signals at the receiver when time delay and uncertainty emerge in the transmission process. Aiming at the weakness of general impulsive synchronization scheme, i.e., there always exists an upper boundary to limit impulsive intervals during the synchronization process, we design a novel synchronization scheme, intermittent impulsive synchronization scheme (IISS). IISS can not only be flexibly applied to the scenario where the control window is restricted but also improve the security of chaos-based secure communication via reducing the control window width and decreasing the redundancy of synchronization signals. Finally, we propose chaos-based public-key cryptography algorithms which can be used to encrypt synchronization signals and guarantee their security across the public channel.

Chaos theory is well known as one of three revolutions in physical sciences in 20th-century, as one physicist called it: Relativity eliminated the Newtonian illusion of absolute space and time; quantum theory eliminated the Newtonian dream of a controllable measurable process; and chaos eliminates the Laplacian fantasy of deterministic predictability". Specially, when chaos synchronization was found in 1991, chaos theory becomes more and more attractive. Chaos has been widely applied to many scientific disciplines: mathematics, programming, microbiology, biology, computer science, economics, engineering, finance, philosophy, physics, politics, population dynamics, psychology, and robotics. One of most important engineering applications is secure communication because of the properties of random behaviours and sensitivity to initial conditions of chaos systems. Noise-like dynamical behaviours can be used to mask the original information in symmetric cryptography. Sensitivity to initial conditions and unpredictability make chaotic systems very suitable to construct one-way function in public-key cryptography. In chaos-based secure communication schemes, information signals are masked or modulated (encrypted) by chaotic signals at the transmitter and the resulting encrypted signals are sent to the corresponding receiver across a public channel (unsafe channel). Perfect chaos synchronization is usually expected to recover the original information signals. In other words, the recovery of the information signals requires the receiver's own copy of the chaotic signals which are synchronized with the transmitter ones. Thus, chaos synchronization is the key technique throughout this whole process. Due to the difficulties of generating and synchronizing chaotic systems and the limit of digital computer precision, there exist many challenges in chaos-based secure communication. In this thesis, we try to solve chaos generation and chaos synchronization problems. Starting from designing chaotic and hyperchaotic system by first-order delay differential equation, we present a family of novel cell attractors with multiple positive Lyapunov exponents. Compared with previously reported hyperchaos systems with complex mathematic structure (more than 3 dimensions), our system is relatively simple while its dynamical behaviours are very complicated. We present a systemic parameter control method to adjust the number of positive Lyapunov exponents, which is an index of chaos degree. Furthermore, we develop a delay feedback controller and apply it to Chen system to generate multi-scroll attractors. It can be generalized to Chua system, Lorenz system, Jerk equation, etc. Since chaos synchronization is the critical technique in chaos-based secure communication, we present corresponding impulsive synchronization criteria to guarantee that the receiver can generate the same chaotic signals at the receiver when time delay and uncertainty emerge in the transmission process. Aiming at the weakness of general impulsive synchronization scheme, i.e., there always exists an upper boundary to limit impulsive intervals during the synchronization process, we design a novel synchronization scheme, intermittent impulsive synchronization scheme (IISS). IISS can not only be flexibly applied to the scenario where the control window is restricted but also improve the security of chaos-based secure communication via reducing the control window width and decreasing the redundancy of synchronization signals. Finally, we propose chaos-based public-key cryptography algorithms which can be used to encrypt synchronization signals and guarantee their security across the public channel.

Nesse trabalho estudamos um laser de estado sólido sujeito a realimentação optica de frequência modificada de um ponto de vista da teoria de bifurcações. Fizemos uma an alise bastante ampla da dinâmica desse laser no espaço de dois parâmetros de injeção (a dessintonização de frequência e a intensidade da injeção) utilizando métodos de integração direta e continuação numérica. Enquanto o método de integração numérica nos possibilitou analisar as dinâmicas mais complexas, incluindo transições para o caos e hipercaos, o método de continuação numérica nos permitiu estudar curvas de bifurcações estáveis e instáveis. A análise foi realizada estudando os efeitos causados pela mudança dos parâmetros que representam o tempo de vida da inversão populacional e a saturação cruzada, responsável pelo acoplamento dos campos dentro do meio ativo. Mostramos que o parâmetro que descreve o tempo de vida da inversão populacional e responsável pelo surgimento de diversas instabilidades no sistema, como o fenômeno de multiestabilidade, surgimento de orbitas periódicas e quase-peri odicas, assim como rotas para o caos via dobramento de período e torus. Para o parâmetro de acoplamento dos campos, mostramos que ele possibilita a presença de hipercaos em nosso sistema, este podendo se apresentar no que denominamos de hipercaos \fraco" e \forte". Dentro da região de hipercaos \forte", mostramos transições determinísticas de dois regimes, em que num deles o laser opera no modo de Q-switching, enquanto que no outro o laser apresenta pequenas oscilações irregulares. Por m, mostramos a existência de uma estatística de eventos extremos dentro do regime hipercaótico. / In this work we studied a solid state laser subjected to frequency-shifted optical feedback from a bifurcation theory point of view. We performed a very broad analysis of the dynamics of this laser in the space of two injection parameters (frequency detuning and injection intensity) using direct integration and numerical continuation methods. While the numerical integration method allowed us to analyze the more complex dynamics, including chaos and hyperchaos transitions, the numerical continuation method allowed us to study stable and unstable bifurcation curves. The analysis was carried out by studying the e ects caused by the change of the parameters that represent the life time of the population inversion and the cross saturation, responsible for the coupling of the elds within the active medium. We show that the parameter that describes the life time of the population inversion is responsible for the appearance of several instabilities in the system, such as the multistability phenomenon, the appearance of periodic and quasi-periodic orbits, as well as routes to chaos via period doubling and torus . For the eld coupling parameter, we show that it allows the presence of hyperchaos in our system, which may present in what we call "weak"and "strong"hyperchaos. Within the "strong"hyperchaos region, we show deterministic transitions of two regimes, in which one laser operates in the Q-switching mode, while in the other the laser presents small irregular oscillations. Finally, we have shown the existence of a extreme events statistic within the hyperchaotic regime.

Nesse trabalho estudamos um laser de estado sólido sujeito a realimentação optica de frequência modificada de um ponto de vista da teoria de bifurcações. Fizemos uma an alise bastante ampla da dinâmica desse laser no espaço de dois parâmetros de injeção (a dessintonização de frequência e a intensidade da injeção) utilizando métodos de integração direta e continuação numérica. Enquanto o método de integração numérica nos possibilitou analisar as dinâmicas mais complexas, incluindo transições para o caos e hipercaos, o método de continuação numérica nos permitiu estudar curvas de bifurcações estáveis e instáveis. A análise foi realizada estudando os efeitos causados pela mudança dos parâmetros que representam o tempo de vida da inversão populacional e a saturação cruzada, responsável pelo acoplamento dos campos dentro do meio ativo. Mostramos que o parâmetro que descreve o tempo de vida da inversão populacional e responsável pelo surgimento de diversas instabilidades no sistema, como o fenômeno de multiestabilidade, surgimento de orbitas periódicas e quase-peri odicas, assim como rotas para o caos via dobramento de período e torus. Para o parâmetro de acoplamento dos campos, mostramos que ele possibilita a presença de hipercaos em nosso sistema, este podendo se apresentar no que denominamos de hipercaos \fraco" e \forte". Dentro da região de hipercaos \forte", mostramos transições determinísticas de dois regimes, em que num deles o laser opera no modo de Q-switching, enquanto que no outro o laser apresenta pequenas oscilações irregulares. Por m, mostramos a existência de uma estatística de eventos extremos dentro do regime hipercaótico. / In this work we studied a solid state laser subjected to frequency-shifted optical feedback from a bifurcation theory point of view. We performed a very broad analysis of the dynamics of this laser in the space of two injection parameters (frequency detuning and injection intensity) using direct integration and numerical continuation methods. While the numerical integration method allowed us to analyze the more complex dynamics, including chaos and hyperchaos transitions, the numerical continuation method allowed us to study stable and unstable bifurcation curves. The analysis was carried out by studying the e ects caused by the change of the parameters that represent the life time of the population inversion and the cross saturation, responsible for the coupling of the elds within the active medium. We show that the parameter that describes the life time of the population inversion is responsible for the appearance of several instabilities in the system, such as the multistability phenomenon, the appearance of periodic and quasi-periodic orbits, as well as routes to chaos via period doubling and torus . For the eld coupling parameter, we show that it allows the presence of hyperchaos in our system, which may present in what we call "weak"and "strong"hyperchaos. Within the "strong"hyperchaos region, we show deterministic transitions of two regimes, in which one laser operates in the Q-switching mode, while in the other the laser presents small irregular oscillations. Finally, we have shown the existence of a extreme events statistic within the hyperchaotic regime.

When two or more chaotic systems are coupled, they may exhibit synchronized chaotic oscillations. The synchronization of chaos is usually understood as the regime of chaotic oscillations in which the corresponding variables or coupled systems are equal to each other. This kind of synchronized chaos is most frequently observed in systems specifically designed to be able to produce this behaviour. In this thesis, one particular type of synchronization, called impulsive synchronization, is investigated and applied to low dimensional chaotic, hyperchaotic and spatiotemporal chaotic systems. This synchronization technique requires driving one chaotic system, called response system, by samples of the state variables of the other chaotic system, called drive system, at discrete moments. Equi-Lagrange stability and equi-attractivity in the large property of the synchronization error become our major concerns when discussing the dynamics of synchronization to guarantee the convergence of the error dynamics to zero. Sufficient conditions for equi-Lagrange stability and equi-attractivity in the large are obtained for the different types of chaos-generating systems used. The issue of robustness of synchronized chaotic oscillations with respect to parameter variations and time delay, is also addressed and investigated when dealing with impulsive synchronization of low dimensional chaotic and hyperchaotic systems. Due to the fact that it is impossible to design two identical chaotic systems and that transmission and sampling delays in impulsive synchronization are inevitable, robustness becomes a fundamental issue in the models considered. Therefore it is established, in this thesis, that under relatively large parameter perturbations and bounded delay, impulsive synchronization still shows very desired behaviour. In fact, criteria for robustness of this particular type of synchronization are derived for both cases, especially in the case of time delay, where sufficient conditions for the synchronization error to be equi-attractivity in the large, are derived and an upper bound on the delay terms is also obtained in terms of the other parameters of the systems involved. The theoretical results, described above, regarding impulsive synchronization, are reconfirmed numerically. This is done by analyzing the Lyapunov exponents of the error dynamics and by showing the simulations of the different models discussed in each case. The application of the theory of synchronization, in general, and impulsive synchronization, in particular, to communication security, is also presented in this thesis. A new impulsive cryptosystem, called induced-message cryptosystem, is proposed and its properties are investigated. It was established that this cryptosystem does not require the transmission of the encrypted signal but instead the impulses will carry the information needed for synchronization and for retrieving the message signal. Thus the security of transmission is increased and the time-frame congestion problem, discussed in the literature, is also solved. Several other impulsive cryptosystems are also proposed to accommodate more solutions to several security issues and to illustrate the different properties of impulsive synchronization. Finally, extending the applications of impulsive synchronization to employ spatiotemporal chaotic systems, generated by partial differential equations, is addressed. Several possible models implementing this approach are suggested in this thesis and few questions are raised towards possible future research work in this area.

When two or more chaotic systems are coupled, they may exhibit synchronized chaotic oscillations. The synchronization of chaos is usually understood as the regime of chaotic oscillations in which the corresponding variables or coupled systems are equal to each other. This kind of synchronized chaos is most frequently observed in systems specifically designed to be able to produce this behaviour. In this thesis, one particular type of synchronization, called impulsive synchronization, is investigated and applied to low dimensional chaotic, hyperchaotic and spatiotemporal chaotic systems. This synchronization technique requires driving one chaotic system, called response system, by samples of the state variables of the other chaotic system, called drive system, at discrete moments. Equi-Lagrange stability and equi-attractivity in the large property of the synchronization error become our major concerns when discussing the dynamics of synchronization to guarantee the convergence of the error dynamics to zero. Sufficient conditions for equi-Lagrange stability and equi-attractivity in the large are obtained for the different types of chaos-generating systems used. The issue of robustness of synchronized chaotic oscillations with respect to parameter variations and time delay, is also addressed and investigated when dealing with impulsive synchronization of low dimensional chaotic and hyperchaotic systems. Due to the fact that it is impossible to design two identical chaotic systems and that transmission and sampling delays in impulsive synchronization are inevitable, robustness becomes a fundamental issue in the models considered. Therefore it is established, in this thesis, that under relatively large parameter perturbations and bounded delay, impulsive synchronization still shows very desired behaviour. In fact, criteria for robustness of this particular type of synchronization are derived for both cases, especially in the case of time delay, where sufficient conditions for the synchronization error to be equi-attractivity in the large, are derived and an upper bound on the delay terms is also obtained in terms of the other parameters of the systems involved. The theoretical results, described above, regarding impulsive synchronization, are reconfirmed numerically. This is done by analyzing the Lyapunov exponents of the error dynamics and by showing the simulations of the different models discussed in each case. The application of the theory of synchronization, in general, and impulsive synchronization, in particular, to communication security, is also presented in this thesis. A new impulsive cryptosystem, called induced-message cryptosystem, is proposed and its properties are investigated. It was established that this cryptosystem does not require the transmission of the encrypted signal but instead the impulses will carry the information needed for synchronization and for retrieving the message signal. Thus the security of transmission is increased and the time-frame congestion problem, discussed in the literature, is also solved. Several other impulsive cryptosystems are also proposed to accommodate more solutions to several security issues and to illustrate the different properties of impulsive synchronization. Finally, extending the applications of impulsive synchronization to employ spatiotemporal chaotic systems, generated by partial differential equations, is addressed. Several possible models implementing this approach are suggested in this thesis and few questions are raised towards possible future research work in this area.