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Why are full configuration interaction computations so expensive ? 


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Full configuration interaction (FCI) computations are expensive due to the exponential scaling of the method. FCI involves considering all possible electronic configurations, resulting in a large number of terms that need to be calculated and stored. This leads to a significant increase in computational cost as the system size and complexity increase. Several strategies have been proposed to reduce the computational load of FCI calculations. Incremental FCI (iFCI) uses a many-body expansion to systematically add correlation to a reference wave function, achieving greatly reduced computational costs compared to FCI . Another approach is the use of configuration state function generators (CSFGs), which allow for a substantial reduction in the computational load by regrouping the configuration state functions and introducing CSFGs . Density matrix renormalization group (DMRG) algorithms provide an efficient approximation to FCI without a predefined excitation level, but their application is limited by the high density of states in certain regions . Modifications to the fast randomized iteration method for FCI (FCI-FRI) have also been proposed to improve its performance for larger chemical systems .

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Full configuration interaction computations are expensive because they involve solving a nonconvex optimization problem and require a large amount of memory.
Full configuration interaction computations are expensive due to the large number of possible configurations that need to be considered.
Full text information: "Configuration-interaction-type calculations on electronic and vibrational structure are often the method of choice for the reliable approximation of many-particle wave functions and energies. The exponential scaling, however, limits their application range." Answer: The exponential scaling of full configuration interaction calculations limits their application range.
Full configuration interaction (FCI) computations are expensive because they involve calculating all possible electronic configurations, which requires a large number of calculations and computational resources.
Full configuration interaction computations are expensive due to the computational load involved in constructing and diagonalizing the Hamiltonian matrix, as well as the inclusion of the time-consuming Breit interaction.

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