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Sam Hopkins
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I see many mathematicians misleadingconflating the definitions of traveling waves and solitons, and I am unable to understand, from a mathematical point of view, the differences between these two types of solutions for a nonlinear dispersive PDE. All I know is the following:

Consider for example a nonlinear dispersive PDE which is completely integrable, i.e. has infinite conservation laws, ( I think the property of complete integrability will not probably add something to the question)

  • The traveling waves are solutions of the form $u_0(x+ct)$ where $u_0$ is the initial data and $c\in\mathbb{R}$.

  • The Solitons are subset of the traveling waves, that remain with the same shape even after colliding with another soliton. The phenomena of solitons appear after a cancelation between the dispersive effects and the nonlinearity of the equation.

So here are my questions:

  1. How do we know if a nonlinear PDE has solitons as solutions, knowing that it has traveling wave solutions ? On other words, how do we prove mathematically that a traveling wave is a soliton (without using simulation).
  2. For example, solutions of the form $u(t,x)=e^{i(x-t)}$ or $u(t,x)=\frac{1}{1-\frac12 e^{i(x-ct)}}$, $x\in \mathbb{T}:=\mathbb{R}/(2\pi\mathbb{Z}),$ can be considered as solitons?
  3. Does a traveling wave that is almost periodic solution, i.e. the set $\{u(\cdot+\tau), \tau\in \mathbb{R}\}$ is relatively compact, can lead to the fact that it is a soliton ?

I see many mathematicians misleading the definitions of traveling waves and solitons, and I am unable to understand, from a mathematical point of view, the differences between these two types of solutions for a nonlinear dispersive PDE. All I know is the following:

Consider for example a nonlinear dispersive PDE which is completely integrable, i.e. has infinite conservation laws, ( I think the property of complete integrability will not probably add something to the question)

  • The traveling waves are solutions of the form $u_0(x+ct)$ where $u_0$ is the initial data and $c\in\mathbb{R}$.

  • The Solitons are subset of the traveling waves, that remain with the same shape even after colliding with another soliton. The phenomena of solitons appear after a cancelation between the dispersive effects and the nonlinearity of the equation.

So here are my questions:

  1. How do we know if a nonlinear PDE has solitons as solutions, knowing that it has traveling wave solutions ? On other words, how do we prove mathematically that a traveling wave is a soliton (without using simulation).
  2. For example, solutions of the form $u(t,x)=e^{i(x-t)}$ or $u(t,x)=\frac{1}{1-\frac12 e^{i(x-ct)}}$, $x\in \mathbb{T}:=\mathbb{R}/(2\pi\mathbb{Z}),$ can be considered as solitons?
  3. Does a traveling wave that is almost periodic solution, i.e. the set $\{u(\cdot+\tau), \tau\in \mathbb{R}\}$ is relatively compact, can lead to the fact that it is a soliton ?

I see many mathematicians conflating the definitions of traveling waves and solitons, and I am unable to understand, from a mathematical point of view, the differences between these two types of solutions for a nonlinear dispersive PDE. All I know is the following:

Consider for example a nonlinear dispersive PDE which is completely integrable, i.e. has infinite conservation laws, ( I think the property of complete integrability will not probably add something to the question)

  • The traveling waves are solutions of the form $u_0(x+ct)$ where $u_0$ is the initial data and $c\in\mathbb{R}$.

  • The Solitons are subset of the traveling waves, that remain with the same shape even after colliding with another soliton. The phenomena of solitons appear after a cancelation between the dispersive effects and the nonlinearity of the equation.

So here are my questions:

  1. How do we know if a nonlinear PDE has solitons as solutions, knowing that it has traveling wave solutions ? On other words, how do we prove mathematically that a traveling wave is a soliton (without using simulation).
  2. For example, solutions of the form $u(t,x)=e^{i(x-t)}$ or $u(t,x)=\frac{1}{1-\frac12 e^{i(x-ct)}}$, $x\in \mathbb{T}:=\mathbb{R}/(2\pi\mathbb{Z}),$ can be considered as solitons?
  3. Does a traveling wave that is almost periodic solution, i.e. the set $\{u(\cdot+\tau), \tau\in \mathbb{R}\}$ is relatively compact, can lead to the fact that it is a soliton ?
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Niser
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Mathematical difference between solitons and traveling waves for a non-linear dispersive PDE

I see many mathematicians misleading the definitions of traveling waves and solitons, and I am unable to understand, from a mathematical point of view, the differences between these two types of solutions for a nonlinear dispersive PDE. All I know is the following:

Consider for example a nonlinear dispersive PDE which is completely integrable, i.e. has infinite conservation laws, ( I think the property of complete integrability will not probably add something to the question)

  • The traveling waves are solutions of the form $u_0(x+ct)$ where $u_0$ is the initial data and $c\in\mathbb{R}$.

  • The Solitons are subset of the traveling waves, that remain with the same shape even after colliding with another soliton. The phenomena of solitons appear after a cancelation between the dispersive effects and the nonlinearity of the equation.

So here are my questions:

  1. How do we know if a nonlinear PDE has solitons as solutions, knowing that it has traveling wave solutions ? On other words, how do we prove mathematically that a traveling wave is a soliton (without using simulation).
  2. For example, solutions of the form $u(t,x)=e^{i(x-t)}$ or $u(t,x)=\frac{1}{1-\frac12 e^{i(x-ct)}}$, $x\in \mathbb{T}:=\mathbb{R}/(2\pi\mathbb{Z}),$ can be considered as solitons?
  3. Does a traveling wave that is almost periodic solution, i.e. the set $\{u(\cdot+\tau), \tau\in \mathbb{R}\}$ is relatively compact, can lead to the fact that it is a soliton ?