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Resumen:
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By an application of the geometrical techniques of Lie, Cohen, and Dickson it is shown that a system of differential equations of the form [x^(r_i)]_i = F_i; (where r_i > 1 for every i = 1 , ... ,n) cannot admit an infinite number of pointlike symmetry vectors. When r_i = r for every i = 1, ... ,n, upper bounds have been computed for the maximum number of independent symmetry vectors that these systems can possess: The upper bounds are given by 2n _2 + nr + 2 (when r> 2), and by 2n_2 + 4n + 2 (when r = 2). The group of symmetries of ?x_r = 0?? (r> 1) has also been computed, and the result obtained shows that when n > 1 and r> 2 the number of independent symmetries of these equations does not attain the upper bound 2n_ 2 + nr + 2, which is a common bound for all systems of differential equations of the form x?_r = F? (t, x?, ... ,?x (r - 1 ) when r> 2. On the other hand, when r = 2 the first upper bound obtained has been reduced to the value n_2 + 4n + 3; this number is equal to the number of independent symmetry vectors of the system ¨x? = 0?, and is also a common bound for all systems of the form x? = F? (t, x?, x?).
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