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The Novikov-Veselov(NV) Equation as an example of Invariant Form Equations

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Abstract (2. Language): 
In this paper we will consider two scalar di erential operators L and M. We call them scalar because their coecients are functions rather than matrices. Our aim is to obtain some gauge invariant equations. In order to achieve this goal we rstly nd the gauge invariants of L and M by using the gauge transformation on L and M. And then we apply `L-M-f triad' representation [L;M] + fL = 0 which gives us some linear and nonlinear equations such as the NV equation in invariant form.
Abstract (Original Language): 
Bu makalede L ve M'yi iki skaler diferansiyel operator olarak gozonune alaca~gz. Burada L ve M skaler operatorlerdir, cunku bu operatorlerin katsaylar matrisler de~gil fonksiyonlardr. Bizim amacmz 'gauge invariant' denklemlerini elde etmektir. Bu amaca ulas.mak icin ilk once L ve M uzerinde 'gauge transformasyon' kullanarak L ve M nin 'gauge invariant' larn bulaca~gz. Daha sonra `L-M-f triad' denklemine, [L;M] + fL = 0 , bas.vurarak baz lineer ve lineer olmayan, orne~gin Novikov-Veselov(NV), denklemleri invariant form'da elde edilir.
160-172

REFERENCES

References: 

[1] B G Konopelchenko, The two dimensioanal second-order dierential
spectral problem: compatibility conditions, general Bts and
integrable equations, Invers problems 4 (1988) 151-163
[2] C.Athorne, A Z2 R3 Toda system, Phys. Lett.A 206 (1995) 162-
166
[3] S.P.Novikov and A.P.Veselov, Two-Dimensional Schrodinger operator:
Inverse Scattering Transform and Evolutional Equations, Physica
18D (1986) 267-273

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