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pubfntandf(x: f64, odd: bool) f32 {
// |tan(x)/x - t(x)| < 2**-25.5 (~[-2e-08, 2e-08]).constT = [_]f64{
0x15554d3418c99f.0p-54, // 0.3333313950307913997580x1112fd38999f72.0p-55, // 0.1333920027129767427180x1b54c91d865afe.0p-57, // 0.05338123784456703935230x191df3908c33ce.0p-58, // 0.02452831811665472788730x185dadfcecf44e.0p-61, // 0.002974357433599673049270x1362b9bf971bcd.0p-59, // 0.00946564784943673166728
};
constz = x * x;
// Split up the polynomial into small independent terms to give
// opportunities for parallel evaluation. The chosen splitting is
// micro-optimized for Athlons (XP, X64). It costs 2 multiplications
// relative to Horner's method on sequential machines.
//
// We add the small terms from lowest degree up for efficiency on
// non-sequential machines (the lowest degree terms tend to be ready
// earlier). Apart from this, we don't care about order of
// operations, and don't need to to care since we have precision to
// spare. However, the chosen splitting is good for accuracy too,
// and would give results as accurate as Horner's method if the
// small terms were added from highest degree down.
constr = T[4] + z * T[5];
constt = T[2] + z * T[3];
constw = z * z;
consts = z * x;
constu = T[0] + z * T[1];
constr0 = (x + s * u) + (s * w) * (t + w * r);
return@floatCast(if (odd) -1.0 / r0elser0);
}