Justin Long edited subsection_General_Relativity_Quantum_Field__.tex  over 8 years ago

Commit id: 899f319bfff7034203f9492265edeeaecbc5d358

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\begin{equation}  \usepackage{physics}  \xi_{ave}\left( \lvert{\Omega^{\prime}}\rangle \right) = \xi_{ave}\left( \lvert{\Omega}\rangle \right) - f \frac{\int_{V}\left( \vec{J}_{e} \cdot \vec{A}_{cl}(\vec{v}\vec{\chi}_{1}) \vec{A}_{cl}(\vec{x}\vec{\chi}_{1})  \right) d\vec{x} }{} \end{equation}  For the purpose of Alcubierre experimentation, we assume that negative energy densities in Quantum Field Theory are in fact similar to General Relativity's own interpretation. This assumption allows us to perform Alcubierre and negative energy experiments with the expectation that by mixing Quantum Field Theory, General Relativity, and semi-classical theory, we can obtain real results.