definition 17.38 Schwartz space and tempered distributions

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definition 17.38: Schwartz space and tempered distributions17.38definition 17.40: Transform and derivative of a distribution17.40definition 10.83: Weak solution10.83proposition A.522: The Newtonian potential inverts the LaplacianA.522proposition 17.52: Linear translation-invariant systems17.52proposition 17.42: Sokhotski–Plemelj17.42proposition 17.39: The transform preserves S17.39proposition 10.67: The Newtonian potential is the fundamental solution10.67definition 10.42: Green's function10.42proposition 17.41: The identities physics uses17.41definition 10.3: Principal part and principal symbol10.3definition 10.87: Weak form of an elliptic problem10.87definition 10.85: Sobolev space10.85definition 10.95: Weak solution of a conservation law10.95proposition 10.84: Consistency10.84proposition A.521: Every derivative passes onto gA.521theorem A.523: Helmholtz decomposition: existenceA.523proof : app:A-long-proofs@proof-313proofdefinition 17.50: Convolution17.50definition 28.25: Complex susceptibility28.25proposition 17.61: Mean-square response of a damped resonator17.61proof : ch:15-fourier-integral-transforms@proof-33prooftheorem 17.32: Fourier inversion17.32proposition 105.22: The two-state effective generator105.22theorem 17.78: Causality implies dispersion relations17.78proof : ch:15-fourier-integral-transforms@proof-27proofproposition 17.30: Elementary properties17.30proof : ch:15-fourier-integral-transforms@proof-25prooflemma 10.44: Green's identities10.44example 10.49: The method of images10.49lemma A.94: Fundamental solution of \pp_\bar zA.94proposition 10.71: Green's representation formula10.71remark 10.73: What compact support is doing, and the rate that replaces it10.73theorem 7.137: Helmholtz decomposition7.137proof : ch:08-pdes@proof-27proof

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depends_on Transform and derivative of a distribution declared parts/02-mathematical-methods/15-fourier-integral-transforms.tex:1581
depends_on Weak solution declared parts/02-mathematical-methods/08-pdes.tex:2256
depends_on The Newtonian potential inverts the Laplacian declared appendices/A-long-proofs.tex:25502
depends_on Linear translation-invariant systems declared parts/02-mathematical-methods/15-fourier-integral-transforms.tex:1992
depends_on Sokhotski–Plemelj declared parts/02-mathematical-methods/15-fourier-integral-transforms.tex:1661
depends_on The transform preserves $\mathcal{S}$ declared parts/02-mathematical-methods/15-fourier-integral-transforms.tex:1544
depends_on The Newtonian potential is the fundamental solution declared parts/02-mathematical-methods/08-pdes.tex:1798