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 Post subject: conservation laws for nonlinear schrodinger equations
PostPosted: Thu, 18 Jun 2009 04:02:44 UTC 
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nonlinear schrodinger equations
i\psi_t+\psi_{xx}+\gamma |\psi|^2\psi=0
what's the invariants? how to prove?
the first three :
\int_{-\infty}^\infty |\psi|^2 dx
\int_{-\infty}^\infty( \psi \overline{\psi}_x-\overline{\psi}\psi_x)dx
\int_{-\infty}^\infty (|\psi_x|^2-\frac{\gamma}{2}|\psi|^4)dx


Last edited by gylpm on Thu, 18 Jun 2009 11:34:44 UTC, edited 1 time in total.

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 Post subject: Re: conservation laws for nonlinear schrodinger equations
PostPosted: Thu, 18 Jun 2009 09:56:04 UTC 
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gylpm wrote:
nonlinear schrodinger equations
i\psi_t+\psi_{xx}+\gamma |\psi|^2\psi=0
what's the invariants? how to prove?
the first three :
\int_{-\infty}^\infty |\psi|^2 dx
\int_{-\infty}^\infty( \psi \overline{\psi}_x-\overline{\psi}\psi_x)dx
\int_{-\infty}^\infty (|\psi_x|^2-|\psi|^4)dx


You are looking at Hamiltonian density
\displaystyle
H=\lvert\psi_x\rvert^2+\frac{\gamma}{2}\lvert\psi\rvert^4
So it is just a matter of finding self-adjoint operators commuting with Hamiltonian, then take integrals.

Of course, if you are asking how to prove the three you gave are invariants, then it is simpler to just differentiate them with respect to t.

_________________
\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


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 Post subject:
PostPosted: Thu, 18 Jun 2009 11:44:53 UTC 
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Joined: Mon, 12 Jan 2009 14:48:04 UTC
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Not only these three invariants, it is an infinit sequence,
Can you tell me where i can get the knowledge about this topic, i am an autodidact


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