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\begin{align}
& u\left( \bar{r},t \right)=\frac{1}{{{\left( 2\pi  \right)}^{4}}}\int_{{{R}^{3}}}^{{}}{{{d}^{3}}q\int_{-\infty }^{\infty }{d\omega }}\frac{{{e}^{i\left( \bar{q}\bar{r}-\omega t \right)}}}{\left( {{q}^{2}}-\frac{{{\omega }^{2}}}{{{c}^{2}}} \right)}\int_{{{R}^{3}}}^{{}}{{{d}^{3}}r\acute{\ }\int_{-\infty }^{\infty }{dt}}\acute{\ }f\left( \bar{r}\acute{\ },t\acute{\ } \right){{e}^{-i\left( \bar{q}\bar{r}-\omega t \right)}} \\
& u\left( \bar{r},t \right)=\int_{{{R}^{3}}}^{{}}{{{d}^{3}}r\acute{\ }\int_{-\infty }^{\infty }{dt}}\acute{\ }\left\{ \frac{1}{{{\left( 2\pi  \right)}^{4}}}\int_{{{R}^{3}}}^{{}}{{{d}^{3}}q\int_{-\infty }^{\infty }{d\omega }}\frac{{{e}^{i\bar{q}\left( \bar{r}-\bar{r}\acute{\ } \right)-i\omega \left( t-t\acute{\ } \right)}}}{\left( {{q}^{2}}-\frac{{{\omega }^{2}}}{{{c}^{2}}} \right)} \right\}f\left( \bar{r}\acute{\ },t\acute{\ } \right) \\
& \Rightarrow \frac{1}{{{\left( 2\pi  \right)}^{4}}}\int_{{{R}^{3}}}^{{}}{{{d}^{3}}q\int_{-\infty }^{\infty }{d\omega }}\frac{{{e}^{i\bar{q}\left( \bar{r}-\bar{r}\acute{\ } \right)-i\omega \left( t-t\acute{\ } \right)}}}{\left( {{q}^{2}}-\frac{{{\omega }^{2}}}{{{c}^{2}}} \right)}=G\left( \bar{r}-\bar{r}\acute{\ },t-t\acute{\ } \right) \\
\end{align}

TeX (checked):

{\begin{aligned}&u\left({\bar {r}},t\right)={\frac {1}{{\left(2\pi \right)}^{4}}}\int _{{R}^{3}}^{}{{{d}^{3}}q\int _{-\infty }^{\infty }{d\omega }}{\frac {{e}^{i\left({\bar {q}}{\bar {r}}-\omega t\right)}}{\left({{q}^{2}}-{\frac {{\omega }^{2}}{{c}^{2}}}\right)}}\int _{{R}^{3}}^{}{{{d}^{3}}r{\acute {\ }}\int _{-\infty }^{\infty }{dt}}{\acute {\ }}f\left({\bar {r}}{\acute {\ }},t{\acute {\ }}\right){{e}^{-i\left({\bar {q}}{\bar {r}}-\omega t\right)}}\\&u\left({\bar {r}},t\right)=\int _{{R}^{3}}^{}{{{d}^{3}}r{\acute {\ }}\int _{-\infty }^{\infty }{dt}}{\acute {\ }}\left\{{\frac {1}{{\left(2\pi \right)}^{4}}}\int _{{R}^{3}}^{}{{{d}^{3}}q\int _{-\infty }^{\infty }{d\omega }}{\frac {{e}^{i{\bar {q}}\left({\bar {r}}-{\bar {r}}{\acute {\ }}\right)-i\omega \left(t-t{\acute {\ }}\right)}}{\left({{q}^{2}}-{\frac {{\omega }^{2}}{{c}^{2}}}\right)}}\right\}f\left({\bar {r}}{\acute {\ }},t{\acute {\ }}\right)\\&\Rightarrow {\frac {1}{{\left(2\pi \right)}^{4}}}\int _{{R}^{3}}^{}{{{d}^{3}}q\int _{-\infty }^{\infty }{d\omega }}{\frac {{e}^{i{\bar {q}}\left({\bar {r}}-{\bar {r}}{\acute {\ }}\right)-i\omega \left(t-t{\acute {\ }}\right)}}{\left({{q}^{2}}-{\frac {{\omega }^{2}}{{c}^{2}}}\right)}}=G\left({\bar {r}}-{\bar {r}}{\acute {\ }},t-t{\acute {\ }}\right)\\\end{aligned}}

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u(r¯,t)=1(2π)4R3d3qdωei(q¯r¯ωt)(q2ω2c2)R3d3r´dt´f(r¯´,t´)ei(q¯r¯ωt)u(r¯,t)=R3d3r´dt´{1(2π)4R3d3qdωeiq¯(r¯r¯´)iω(tt´)(q2ω2c2)}f(r¯´,t´)1(2π)4R3d3qdωeiq¯(r¯r¯´)iω(tt´)(q2ω2c2)=G(r¯r¯´,tt´)
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