Consider real roots. Every zero at is , , and its derivative is nonzero. For a regular perturbation, write . The Taylor seriesgives . Thus, through the requested order,There is no quadratic term. The exact parametrization also verifies completeness and the remainder order for .
Take . There are two real branches, on different scales. For a root tending to zero, the Taylor series givesThe dominant balance is , so a fractional-power root expansion yieldsMore precisely . An ordinary power series in integer powers of would miss this scale.
There is also a root escaping to positive infinity. Boundedness of the sine term makes the leading dominant balance . The nonzero branch isIndeed the equation rearranges to , which yields on this branch. The bounded oscillatory correction need not have a constant limiting value.
To check that these are all the real solutions, solve for the parameter:Positive values occur only on and ; are not roots. A useful exact derivative isIt vanishes only at isolated points, so is strictly decreasing on each of these intervals. Its endpoint limits are and zero on each interval. This monotone parametrization of sine perturbation roots gives exactly one root in each interval for every , proving that both asymptotic branches, and no others, have been included. If negative small parameters are allowed, the transformation reflects these two branches and gives all real solutions for that sign as well.
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