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2002
Let us consider the homogeneous wave equation1 $$\frac{{{\partial ^2}u}}{{\partial {t^2}}} - {c^2}\Delta u = 0$$ (3.1) and the direct and inverse Fourier transforms in space $$ {F_x}u = \hat u(k) = \frac{1}{{{{(2\pi )}^{d/2}}}}\int_{{R^d}} {u(x){e^{ - ik \cdot x}}} dx, $$ (3.2a) $$ F_x^{ - 1}\hat u = u(x) = \frac{1}{{{{(2\pi ...
openaire +1 more source
Let us consider the homogeneous wave equation1 $$\frac{{{\partial ^2}u}}{{\partial {t^2}}} - {c^2}\Delta u = 0$$ (3.1) and the direct and inverse Fourier transforms in space $$ {F_x}u = \hat u(k) = \frac{1}{{{{(2\pi )}^{d/2}}}}\int_{{R^d}} {u(x){e^{ - ik \cdot x}}} dx, $$ (3.2a) $$ F_x^{ - 1}\hat u = u(x) = \frac{1}{{{{(2\pi ...
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Challenges and opportunities of gravitational-wave searches at MHz to GHz frequencies
Living Reviews in Relativity, 2021Odylio D Aguiar +2 more
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The WASP–WAVE protein network: connecting the membrane to the cytoskeleton
Nature Reviews Molecular Cell Biology, 2007Shiro Suetsugu
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