The Laplace transform of |sin| #
For 0 < a the rectified sine |sin t| has the Laplace transform
∫_{t > 0} |sin t| e^{-a t} dt = (1 + e^{-π a}) / ((1 - e^{-π a}) (1 + a²)),
and, since |sin| is even, the two-sided transform
∫_ℝ |sin t| e^{-a |t|} dt is twice that. One arch contributes
∫_0^π sin t e^{-a t} dt = (1 + e^{-π a}) / (1 + a²), and since |sin| is π-periodic every
later arch contributes the same amount damped by a further factor e^{-π a}; summing the
geometric series gives the closed form.
Main declarations #
TauCeti.integral_sin_mul_exp_neg_mul_zero_pi: the integral over one arch;TauCeti.integral_abs_sin_mul_exp_neg_mul_Ioi: the one-sided Laplace transform of|sin|;TauCeti.integral_abs_sin_mul_exp_neg_mul_abs: the two-sided transform∫_ℝ |sin t| e^{-a |t|} dt = 2 (1 + e^{-π a}) / ((1 - e^{-π a}) (1 + a²)).
For 0 < a, the function t ↦ |sin t| e^{-a t} is integrable on (0, ∞): it is
dominated by e^{-a t}.
The Laplace transform of |sin|. For 0 < a,
∫_{t > 0} |sin t| e^{-a t} dt = (1 + e^{-π a}) / ((1 - e^{-π a}) (1 + a²)).
The two-sided Laplace transform of |sin|. For 0 < a,
∫_ℝ |sin t| e^{-a |t|} dt = 2 (1 + e^{-π a}) / ((1 - e^{-π a}) (1 + a²)).