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The (i,j)th element of a Toeplitz matrix depends only on i - ji. This property of the free propagator in eq 2 yields an efficient scheme where only the first (banded and sparse) row of the matrix representation of the time-evolution operator needs to be stored.
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The (i,j)th element of a Toeplitz matrix depends only on i - ji. This property of the free propagator in eq 2 yields an efficient scheme where only the first (banded and sparse) row of the matrix representation of the time-evolution operator needs to be stored.
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84 basis. The Hamiltonian is then projected onto the Krylov basis to obtain a smaller MxM matrix which can be diagonalized easily to obtain the first few eigenstates of the proton.
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84 basis. The Hamiltonian is then projected onto the Krylov basis to obtain a smaller MxM matrix which can be diagonalized easily to obtain the first few eigenstates of the proton.
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