bolbteppa
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If |a_{mn}x_0^my_0^n| \leq M then a double power series f(x,y) = \sum a_{mn} x^m y^n can be 'bounded' by a dominant function of the form \phi(x,y) = \tfrac{M}{(1-\tfrac{x}{x_0})(1-\tfrac{y}{y_0})}, obviously derived from a geometric series argument. This is useful when proving that analytic solutions exist to y' = f(x,y) in the case that f is analytic.
A more useful dominant function when proving existence for an integrable pfaffian of the form dz = f_1dx_1 + f_2dx_2 is given by \psi(x,y) = \tfrac{M}{1-(\tfrac{x}{x_0}+\tfrac{y}{y_0})}. The coefficients of x^my^n in the taylor expansion of \psi is equal to the coefficients of x^my^n in the taylor expansion of M(\tfrac{x}{x_0}+\tfrac{y}{y_0})^{m+n}, and are at least equal to the coefficients of the taylor expansion of \phi.
My question is, how in the world does one gain any intuition for all of this? I can understand, derive & use \phi(x,y) = \tfrac{M}{(1-\tfrac{x}{x_0})(1-\tfrac{y}{y_0})} perfectly, however motivating, deriving & using the alternative function \psi(x,y) = \tfrac{M}{1-(\tfrac{x}{x_0}+\tfrac{y}{y_0})} is too arbitrary for me, is there a nice way to see the use of this second dominant function as obvious? Page 397 if needed
A more useful dominant function when proving existence for an integrable pfaffian of the form dz = f_1dx_1 + f_2dx_2 is given by \psi(x,y) = \tfrac{M}{1-(\tfrac{x}{x_0}+\tfrac{y}{y_0})}. The coefficients of x^my^n in the taylor expansion of \psi is equal to the coefficients of x^my^n in the taylor expansion of M(\tfrac{x}{x_0}+\tfrac{y}{y_0})^{m+n}, and are at least equal to the coefficients of the taylor expansion of \phi.
My question is, how in the world does one gain any intuition for all of this? I can understand, derive & use \phi(x,y) = \tfrac{M}{(1-\tfrac{x}{x_0})(1-\tfrac{y}{y_0})} perfectly, however motivating, deriving & using the alternative function \psi(x,y) = \tfrac{M}{1-(\tfrac{x}{x_0}+\tfrac{y}{y_0})} is too arbitrary for me, is there a nice way to see the use of this second dominant function as obvious? Page 397 if needed