Question Number 219355 by SdC355 last updated on 23/Apr/25

$$\int_{\mathrm{0}} ^{\:\infty} \:\:\frac{\mathrm{sin}\left({z}\right)}{{z}}{e}^{−{zt}} \mathrm{d}{z}=?? \\ $$
Answered by breniam last updated on 23/Apr/25

$$={I}\left({t}\right) \\ $$$${I}'\left({t}\right)=\underset{{t}_{\mathrm{0}} \rightarrow{t}} {\mathrm{lim}}\underset{\mathrm{0}} {\overset{\infty} {\int}}\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{zt}_{\mathrm{0}} } }{{t}−{t}_{\mathrm{0}} }\mathrm{d}{z} \\ $$$$\mathrm{By}\:\mathrm{the}\:\mathrm{mean}\:\mathrm{value}\:\mathrm{theorem},\:\mathrm{f}.\mathrm{a}.\:{t}\in\mathbb{R}\:\mathrm{and}\:\mathrm{f}.\mathrm{a}.\:{t}_{\mathrm{0}} \in\mathbb{R}\backslash\left\{{t}\right\} \\ $$$$\mathrm{there}\:\mathrm{exists}\:\xi\in\left(\mathrm{min}\left(\left\{{t},{t}_{\mathrm{0}} \right\}\right),\mathrm{max}\left(\left\{{t},{t}_{\mathrm{0}} \right\}\right)\right)\:\mathrm{s}.\mathrm{t}. \\ $$$$\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{zt}_{\mathrm{0}} } }{{t}−{t}_{\mathrm{0}} }=−\mathrm{sin}\left({z}\right){e}^{−{z}\xi} \\ $$$$\mathrm{Let}\:\xi\left({t}_{\mathrm{0}} \right)\:\mathrm{be}\:\mathrm{any}\:\mathrm{function}\:\mathrm{which} \\ $$$$\mathrm{for}\:\mathrm{every}\:{t}_{\mathrm{0}} \in\mathbb{R}\backslash\left\{{t}\right\}\:\mathrm{gives}\:\mathrm{one}\:\mathrm{of}\:\mathrm{the} \\ $$$$\mathrm{values}\:\mathrm{guaranteed}\:\mathrm{by}\:\mathrm{theorem}.\: \\ $$$$\mathrm{Then},\:\mathrm{for}\:\mathrm{each}\:{t}_{\mathrm{0}} \:\mathrm{close}\:\mathrm{enought}\:\mathrm{to}\:{t}\:\mathrm{we}\:\mathrm{have} \\ $$$$−\mathrm{sin}\left({z}\right){e}^{−\mathrm{2}{z}} \geqslant\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{zt}_{\mathrm{0}} } }{{t}−{t}_{\mathrm{0}} }=−\mathrm{sin}\left({z}\right){e}^{−{z}\xi\left({t}_{\mathrm{0}} \right)} \geqslant−\mathrm{sin}\left({z}\right) \\ $$$$\mathrm{What}\:\mathrm{more}, \\ $$$$\underset{{t}_{\mathrm{0}} \rightarrow{t}} {\mathrm{lim}}\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{zt}_{\mathrm{0}} } }{{t}−{t}_{\mathrm{0}} }=−\mathrm{sin}\left({z}\right){e}^{−{tz}} \\ $$$$\mathrm{So},\:\mathrm{by}\:\mathrm{Lebesgues}\:\mathrm{diminated}\:\mathrm{convergence}\:\mathrm{theorem},\:\mathrm{for}\:\mathrm{each}\:\left({t}_{\mathrm{0}} \right)_{{n}} \:\mathrm{convergent}\:\mathrm{to}\:{t} \\ $$$${I}'\left({t}\right)=\underset{{n}\rightarrow\infty} {\mathrm{lim}}\underset{\mathrm{0}} {\overset{\infty} {\int}}\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{z}\left({t}_{\mathrm{0}} \right)_{{n}} } }{{t}−\left({t}_{\mathrm{0}} \right)_{{n}} }\mathrm{d}{z}= \\ $$$${I}'\left({t}\right)=\underset{\mathrm{0}} {\overset{\infty} {\int}}\underset{{n}\rightarrow\infty} {\mathrm{lim}}\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{z}\left({t}_{\mathrm{0}} \right)_{{n}} } }{{t}−\left({t}_{\mathrm{0}} \right)_{{n}} }\mathrm{d}{z}=−\underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{sin}\left({z}\right){e}^{−{tz}} \mathrm{d}{z} \\ $$$$\mathrm{So},\:\mathrm{by}\:\mathrm{Haine}'\mathrm{s}\:\mathrm{continous}\:\mathrm{limit}\:\mathrm{definition} \\ $$$${I}'\left({t}\right)=\underset{{t}_{\mathrm{0}} \rightarrow{t}} {\mathrm{lim}}\underset{\mathrm{0}} {\overset{\infty} {\int}}\frac{\mathrm{sin}\left({z}\right)}{{z}}×\frac{{e}^{−{zt}} −{e}^{−{zt}_{\mathrm{0}} } }{{t}−{t}_{\mathrm{0}} }\mathrm{d}{z}=−\underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{sin}\left({z}\right){e}^{−{tz}} \mathrm{d}{z}= \\ $$$$−\underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{sin}\left({z}\right){e}^{−{tz}} \mathrm{d}{z}=\underset{\mathrm{0}} {\overset{\infty} {\int}}\left(\mathrm{cos}\left({z}\right)\right)'{e}^{−{tz}} \mathrm{d}{z}=−\mathrm{1}+{t}\underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{cos}\left({z}\right){e}^{−{tz}} \mathrm{d}{z}=−\mathrm{1}+{t}\underset{\mathrm{0}} {\overset{\infty} {\int}}\left(\mathrm{sin}\left({z}\right)\right)'{e}^{−{tz}} \mathrm{d}{z}=−\mathrm{1}−{t}^{\mathrm{2}} \underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{sin}\left({z}\right){e}^{−{tz}} \mathrm{d}{z}\Rightarrow \\ $$$$\Rightarrow\left({t}^{\mathrm{2}} +\mathrm{1}\right)\underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{sin}\left({z}\right){e}^{−{tz}} \mathrm{d}{z}=−\mathrm{1}\Rightarrow\underset{\mathrm{0}} {\overset{\infty} {\int}}\mathrm{sin}\left({z}\right){e}^{−{tz}} \mathrm{d}{z}=\frac{−\mathrm{1}}{{t}^{\mathrm{2}} +\mathrm{1}} \\ $$$${I}\left({t}\right)\in−\int\frac{\mathrm{1}}{{t}^{\mathrm{2}} +\mathrm{1}}\mathrm{d}{t}=−\mathrm{arctan}\left({t}\right)+{C} \\ $$$$\underset{{t}\rightarrow\infty} {\mathrm{lim}}{I}\left({t}\right)=\mathrm{0}\Rightarrow{C}=\frac{\pi}{\mathrm{2}} \\ $$$$ \\ $$$$ \\ $$