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docs/advanced/input_files/input-main.md

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- [out\_mat\_dh](#out_mat_dh)
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- [out\_mat\_xc](#out_mat_xc)
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- [out\_mat\_xc2](#out_mat_xc2)
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- [out\_mat\_l](#out_mat_l)
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- [out\_eband\_terms](#out_eband_terms)
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- [out\_hr\_npz/out\_dm\_npz](#out_hr_npzout_dm_npz)
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- [dm\_to\_rho](#dm_to_rho)
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- **Description**: Whether to print the exchange-correlation matrices in **numerical orbital representation** (unit: Ry): $\braket{\phi_i|V_\text{xc}^\text{(semi-)local}+V_\text{exx}+V_\text{DFTU}|\phi_j}(\mathbf{R})$ in CSR format (the same format as [out_mat_hs2](../elec_properties/hs_matrix.md#out_mat_hs2)) in the directory `OUT.${suffix}`. (Note that currently DeePKS term is not included. ) The files are named `Vxc_R_spin$s`.
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- **Default**: False
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### out_mat_l
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- **Type**: Boolean [Integer\](optional)
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- **Availability**: Numerical atomic orbital (NAO) basis
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- **Description**: Whether to print the expectation value of the angular momentum operator $\hat{L}_x$, $\hat{L}_y$, and $\hat{L}_z$ in the basis of the localized atomic orbitals. The files are named `OUT.${suffix}/${suffix}_Lx.dat`, `OUT.${suffix}/${suffix}_Ly.dat`, and `OUT.${suffix}/${suffix}_Lz.dat`. The second integer controls the precision of the output.
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- **Default**: False 8
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### out_eband_terms
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- **Type**: Boolean

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