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DBAR problem

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The DBAR problem, or the ¯ {\displaystyle {\bar {\partial }}} -problem, is the problem of solving the differential equation ¯ f ( z , z ¯ ) = g ( z ) {\displaystyle {\bar {\partial }}f(z,{\bar {z}})=g(z)} for the function f ( z , z ¯ ) {\displaystyle f(z,{\bar {z}})} , where g ( z ) {\displaystyle g(z)} is assumed to be known and z = x + i y {\displaystyle z=x+iy} is a complex number in a domain R C {\displaystyle R\subseteq \mathbb {C} } . The operator ¯ {\displaystyle {\bar {\partial }}} is called the DBAR operator: ¯ = 1 2 ( x + i y ) {\displaystyle {\bar {\partial }}={\frac {1}{2}}\left({\frac {\partial }{\partial x}}+i{\frac {\partial }{\partial y}}\right)}

The DBAR operator is nothing other than the complex conjugate of the operator = z = 1 2 ( x i y ) {\displaystyle \partial ={\frac {\partial }{\partial z}}={\frac {1}{2}}\left({\frac {\partial }{\partial x}}-i{\frac {\partial }{\partial y}}\right)} denoting the usual differentiation in the complex z {\displaystyle z} -plane.

The DBAR problem is of key importance in the theory of integrable systems, Schrödinger operators and generalizes the Riemann–Hilbert problem.

Citations

  1. ^ Ablowitz & Fokas 2003.
  2. Haslinger 2014.
  3. Konopelchenko 2000.

References

  • Konopelchenko, B. G. (2000). "On dbar-problem and integrable equations". arXiv:nlin/0002049.
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