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