System of coupled first order PDE

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SUMMARY

The discussion centers on solving a system of coupled first-order partial differential equations (PDEs) derived from the Dirac equation with a space-time dependent mass in two spatial dimensions. The initial approach using Fourier methods was unsuccessful, but the user, Blue2script, later discovered that the system can be decoupled into four second-order PDEs, simplifying the problem significantly. This transformation is crucial for further analysis and solution of the equations.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with the Dirac equation in quantum field theory (QFT)
  • Knowledge of linear algebra, particularly matrix operations
  • Experience with mathematical methods for solving PDEs
NEXT STEPS
  • Study methods for decoupling systems of PDEs
  • Learn about the application of Fourier transforms in solving PDEs
  • Explore the implications of space-time dependent mass in quantum field theory
  • Investigate numerical techniques for solving second-order PDEs
USEFUL FOR

Researchers and students in theoretical physics, particularly those focused on quantum field theory and mathematical physics, will benefit from this discussion. It is also relevant for mathematicians working on PDEs and their applications in physics.

blue2script
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Hello everybody,

I have a problem here related to QFT in a research project. I end up with some Dirac equation with space-time dependent mass in 2 spatial dimensions.

More mathematically, the PDE to solve is

<br /> \left( {i\left( {\sigma ^i \otimes I_2 } \right)\partial _i + g_y \varphi ^a \left( {I_2 \otimes \sigma ^a } \right)} \right)\psi = 0<br />

where \varphi = \varphi\left(x,y\right) is a (given) function of x,y.

More explicit, the system looks like:
<br /> \left[ {i\left( {\begin{array}{*{20}c}<br /> 0 &amp; 1 &amp; 0 &amp; 0 \\<br /> 1 &amp; 0 &amp; 0 &amp; 0 \\<br /> 0 &amp; 0 &amp; 0 &amp; 1 \\<br /> 0 &amp; 0 &amp; 1 &amp; 0 \\<br /> <br /> \end{array} } \right)\partial _1 + i\left( {\begin{array}{*{20}c}<br /> 0 &amp; { - i} &amp; 0 &amp; 0 \\<br /> i &amp; 0 &amp; 0 &amp; 0 \\<br /> 0 &amp; 0 &amp; 0 &amp; { - i} \\<br /> 0 &amp; 0 &amp; i &amp; 0 \\<br /> <br /> \end{array} } \right)\partial _2 + g_y \left\{ {\varphi ^1 \left( {\begin{array}{*{20}c}<br /> 0 &amp; 0 &amp; 1 &amp; 0 \\<br /> 0 &amp; 0 &amp; 0 &amp; 1 \\<br /> 1 &amp; 0 &amp; 0 &amp; 0 \\<br /> 0 &amp; 1 &amp; 0 &amp; 0 \\<br /> <br /> \end{array} } \right) + \varphi ^2 \left( {\begin{array}{*{20}c}<br /> 0 &amp; 0 &amp; { - i} &amp; 0 \\<br /> 0 &amp; 0 &amp; 0 &amp; { - i} \\<br /> i &amp; 0 &amp; 0 &amp; 0 \\<br /> 0 &amp; i &amp; 0 &amp; 0 \\<br /> <br /> \end{array} } \right) + \varphi ^3 \left( {\begin{array}{*{20}c}<br /> 1 &amp; 0 &amp; 0 &amp; 0 \\<br /> 0 &amp; 1 &amp; 0 &amp; 0 \\<br /> 0 &amp; 0 &amp; { - 1} &amp; 0 \\<br /> 0 &amp; 0 &amp; 0 &amp; { - 1} \\<br /> <br /> \end{array} } \right)} \right\}} \right]\left( {\begin{array}{*{20}c}<br /> {\psi _1 } \\<br /> {\psi _2 } \\<br /> {\psi _3 } \\<br /> {\psi _4 } \\<br /> <br /> \end{array} } \right) = \left( {\begin{array}{*{20}c}<br /> 0 \\<br /> 0 \\<br /> 0 \\<br /> 0 \\<br /> <br /> \end{array} } \right)<br />

with \psi_i = \psi_i\left(x,y\right). I tried some Fourier-method, but that wouldn't work out. I am completely stuck here and have no idea how to proceed. Could anyone give me a hint?

A big thanks in advance!

Blue2script
 
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Ok, sorry guys, I got it. Its pretty simple to decouple this linear PDE. I am left now with four second order PDEs.

Thanks!

Blue2script
 

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