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demolishka
demolishka
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For your basic question (topic name) the classical reference is

Henry D. Geometric Theory of Semilinear Parabolic Equations. SpringerVerlag, 1981.

However, you will not find there general recipes for your second question and that's why. A stationary state, say $y_{0}(x)$, can be homogeneous (given by constant functions $y_{0}(x) \equiv y_{0})$ and non-homogeneous ($y_{0}(x)$ is not constant). For Robin conditions the only homogeneous state is $0$ (I assume $b \not = 0$ and $F(0)=0$). To find non-homogeneous states you have to solve a nonlinear PDE that is impossible to do analytically. So, the only way is to provide qualitative analysis of the equation that shows at least the existence (or non-existence) of non-homogeneous states (and their number if we get lucky). This highly relies on the structure of the nonlineraity $F$. For example, when $F$ is Lipschitz with a small Lipschitz constant, then the zero will be usually globally stable and there cannot be non-homogeneous states. Increasing the Lipschitz constant you may get the pitchfork bifurcation (the appearance of two non-homogeneous stationary states in a neighbourhood of zero) and so on. So, the result you mentioned (on the exsitence and number of non-homogeneous states) must use some very specifity of $F$.

For general approaches, I would also recommend the paper

Ni W. M., Tang M. (2005). Turing patterns in the Lengyel-Epstein system for the CIMA reaction. Transactions of the American Mathematical Society, 357(10), 3953--3969,

where with the aid of topological methods and a priori estimates for certain parameters it is proved the uniqueness of the zero stationary state or the existence of non-homogeneous states.

For your basic question (topic name) the classical reference is

Henry D. Geometric Theory of Semilinear Parabolic Equations. SpringerVerlag, 1981.

However, you will not find there general recipes for your second question and that's why. A stationary state, say $y_{0}(x)$, can be homogeneous (given by constant functions $y_{0}(x) \equiv y_{0})$ and non-homogeneous ($y_{0}(x)$ is not constant). For Robin conditions the only homogeneous state is $0$ (I assume $b \not = 0$ and $F(0)=0$). To find non-homogeneous states you have to solve a nonlinear PDE that is impossible to do analytically. So, the only way is to provide qualitative analysis of the equation that shows at least the existence (or non-existence) of non-homogeneous states (and their number if we get lucky). This highly relies on the structure of the nonlineraity $F$. For example, when $F$ is Lipschitz with a small Lipschitz constant, then the zero will be usually globally stable and there cannot be non-homogeneous states. Increasing the Lipschitz constant you may get the pitchfork bifurcation (the appearance of two non-homogeneous stationary states in a neighbourhood of zero) and so on. So, the result you mentioned (on the exsitence and number of non-homogeneous states) must use some very specifity of $F$.

For general approaches, I would also recommend the paper

Ni W. M., Tang M. (2005). Turing patterns in the Lengyel-Epstein system for the CIMA reaction. Transactions of the American Mathematical Society, 357(10), 3953--3969,

where with the aid of topological methods and a priori estimates for certain parameters it is proved the uniqueness of the zero stationary state or the existence of non-homogeneous states.

For your basic question (topic name) the classical reference is

Henry D. Geometric Theory of Semilinear Parabolic Equations. SpringerVerlag, 1981.

However, you will not find there general recipes for your second question and that's why. A stationary state, say $y_{0}(x)$, can be homogeneous (given by constant functions $y_{0}(x) \equiv y_{0})$ and non-homogeneous ($y_{0}(x)$ is not constant). For Robin conditions the only homogeneous state is $0$ (I assume $b \not = 0$ and $F(0)=0$). To find non-homogeneous states you have to solve a nonlinear PDE that is impossible to do analytically. So, the only way is to provide qualitative analysis of the equation that shows at least the existence (or non-existence) of non-homogeneous states (and their number if we get lucky). This highly relies on the structure of the nonlineraity $F$. For example, when $F$ is Lipschitz with a small Lipschitz constant, then the zero will be usually globally stable and there cannot be non-homogeneous states. Increasing the Lipschitz constant you may get the pitchfork bifurcation (the appearance of two non-homogeneous stationary states in a neighbourhood of zero) and so on. So, the result you mentioned (on the exsitence and number of non-homogeneous states) must use some very specifity of $F$.

For general approaches, I would also recommend the paper

Ni W. M., Tang M. (2005). Turing patterns in the Lengyel-Epstein system for the CIMA reaction. Transactions of the American Mathematical Society, 357(10), 3953-3969,

where with the aid of topological methods and a priori estimates for certain parameters it is proved the uniqueness of the zero stationary state or the existence of non-homogeneous states.

Source Link
demolishka
demolishka
  • 798
  • 5
  • 13

For your basic question (topic name) the classical reference is

Henry D. Geometric Theory of Semilinear Parabolic Equations. SpringerVerlag, 1981.

However, you will not find there general recipes for your second question and that's why. A stationary state, say $y_{0}(x)$, can be homogeneous (given by constant functions $y_{0}(x) \equiv y_{0})$ and non-homogeneous ($y_{0}(x)$ is not constant). For Robin conditions the only homogeneous state is $0$ (I assume $b \not = 0$ and $F(0)=0$). To find non-homogeneous states you have to solve a nonlinear PDE that is impossible to do analytically. So, the only way is to provide qualitative analysis of the equation that shows at least the existence (or non-existence) of non-homogeneous states (and their number if we get lucky). This highly relies on the structure of the nonlineraity $F$. For example, when $F$ is Lipschitz with a small Lipschitz constant, then the zero will be usually globally stable and there cannot be non-homogeneous states. Increasing the Lipschitz constant you may get the pitchfork bifurcation (the appearance of two non-homogeneous stationary states in a neighbourhood of zero) and so on. So, the result you mentioned (on the exsitence and number of non-homogeneous states) must use some very specifity of $F$.

For general approaches, I would also recommend the paper

Ni W. M., Tang M. (2005). Turing patterns in the Lengyel-Epstein system for the CIMA reaction. Transactions of the American Mathematical Society, 357(10), 3953--3969,

where with the aid of topological methods and a priori estimates for certain parameters it is proved the uniqueness of the zero stationary state or the existence of non-homogeneous states.