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Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

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Integrability of SDYM Equations for the Moyal Bracket Lie Algebra<br />

where is a complex parameter <strong>and</strong> are the charges<br />

<strong>de</strong>f<strong>in</strong>ed <strong>in</strong> the previous section. Then we easily get<br />

Differentiat<strong>in</strong>g the first equation of (14) with respect to <strong>and</strong> the second<br />

one with respect to then employ<strong>in</strong>g Eq. (14) once more one obta<strong>in</strong>s<br />

As (15) is satisfied for every it follows that<br />

i.e. fulfills ME. Thus substitut<strong>in</strong>g the <strong>de</strong>f<strong>in</strong>ition of <strong>and</strong> <strong>in</strong>to<br />

(14) <strong>and</strong> chang<strong>in</strong>g by the general solution we arrive at the l<strong>in</strong>ear<br />

system for ME<br />

Integrability condition of the system (17) is given by ME. The solution<br />

is analytic <strong>in</strong> <strong>and</strong> is assumed to be of the form<br />

where exp st<strong>and</strong>s for the exponential <strong>in</strong> associative Moyal algebra,<br />

i.e.<br />

Analogously, we can consi<strong>de</strong>r another l<strong>in</strong>ear system for ME<br />

As before, ME is the <strong>in</strong>tegrability condition of (18). The solution<br />

has the Laurent series expansion<br />

81

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