=========================================================== .___ __ __ _________________ __ __ __| _/|__|/ |_ / ___\_` __ \__ \ | | \/ __ | | \\_ __\ / /_/ > | \// __ \| | / /_/ | | || | \___ /|__| (____ /____/\____ | |__||__| /_____/ \/ \/ grep rough audit - static analysis tool v2.8 written by @Wireghoul =================================[justanotherhacker.com]=== chemps2-1.8.9/CMake/CheMPS2Config.cmake.in-143- if(${_fext} STREQUAL ${CMAKE_SHARED_LIBRARY_SUFFIX}) chemps2-1.8.9/CMake/CheMPS2Config.cmake.in:144: include("${CMAKE_CURRENT_LIST_DIR}/${PN}Targets-shared.cmake") chemps2-1.8.9/CMake/CheMPS2Config.cmake.in-145- else() chemps2-1.8.9/CMake/CheMPS2Config.cmake.in:146: include("${CMAKE_CURRENT_LIST_DIR}/${PN}Targets-static.cmake") chemps2-1.8.9/CMake/CheMPS2Config.cmake.in-147- endif() ############################################## chemps2-1.8.9/CheMPS2/include/chemps2/Correlations.h-43- \f] chemps2-1.8.9/CheMPS2/include/chemps2/Correlations.h:44: where \f$trace_{B}\f$ denotes the summation over the occupations of the orbitals in \f$B\f$. The (nonnegative) eigenspectrum of \f$\mathbf{\rho}_A\f$ directly reflects the quantum entanglement between the orbitals in \f$A\f$ and the ones in \f$B\f$. If there is only one nonzero eigenvalue, \f$A\f$ and \f$B\f$ are not entangled. The total wavefunction can then be factorized: \f$\ket{\Psi} = \ket{\Psi_A}\ket{\Psi_B}\f$. A measurement of an occupation in \f$B\f$ does not influence the outcome of a measurement in \f$A\f$. If there are several nonzero eigenvalues, \f$A\f$ and \f$B\f$ are entangled, and measurements in \f$A\f$ and \f$B\f$ are correlated. The total wavefunction can not be factorized in that case. chemps2-1.8.9/CheMPS2/include/chemps2/Correlations.h-45- ############################################## chemps2-1.8.9/CheMPS2/include/chemps2/Correlations.h-83- \f] chemps2-1.8.9/CheMPS2/include/chemps2/Correlations.h:84: where \f$\hat{d}_{i\sigma} = \hat{n}_{i\sigma} (1 - \hat{n}_{i~-\sigma})\f$. chemps2-1.8.9/CheMPS2/include/chemps2/Correlations.h-85- ############################################## chemps2-1.8.9/CheMPS2/include/chemps2/EdmistonRuedenberg.h-77- \f] chemps2-1.8.9/CheMPS2/include/chemps2/EdmistonRuedenberg.h:78: where the (continuous) variable \f$z_k\f$ denotes the optimal position of orbital \f$k\f$. In order to fix translational invariance and normalization of the solution, the constraints \f$\sum_i z_i = 0\f$ and \f$\vec{z}^T \vec{z} = 1\f$ are imposed. The cost function can be rewritten as chemps2-1.8.9/CheMPS2/include/chemps2/EdmistonRuedenberg.h-79- \f[