equation 39.3 eq:mink-noncompact

open in the book · parts/04-special-relativity/03-minkowski-lorentz-poincare.tex:133

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equation 39.3: eq:mink-noncompact39.3equation 39.2: eq:mink-lorentz-condition39.2definition 39.7: Antichronous transformations39.7definition 39.5: Orthochronous Lorentz group39.5proposition 39.6: L^\uparrow and L^\uparrow_+ are subgroups39.6definition 39.4: Improper Lorentz transformations39.4proposition 39.9: The generators39.9proposition 39.2: L is a Lie group39.2proposition 39.11: Invariance of the interval39.11definition 39.1: Lorentz group39.1lemma 109.42: Total inversion is a complex Lorentz transformation109.42proposition 39.8: Component structure39.8theorem 105.34: CPT105.34theorem 38.23: Polar decomposition of a Lorentz transformation38.23proof : ch:03-minkowski-lorentz-poincare@proof-3proof

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typedirectionnode provenancewhere
step_from eq:mink-lorentz-condition declared — the $\mu=\nu=0$ component of the defining relation parts/04-special-relativity/03-minkowski-lorentz-poincare.tex:136
depends_on Antichronous transformations declared parts/04-special-relativity/03-minkowski-lorentz-poincare.tex:284
depends_on Orthochronous Lorentz group declared parts/04-special-relativity/03-minkowski-lorentz-poincare.tex:223
depends_on $L^{\uparrow}$ and $L^{\uparrow}_{+}$ are subgroups declared parts/04-special-relativity/03-minkowski-lorentz-poincare.tex:233