|
140 | 140 | - [out\_wfc\_r](#out_wfc_r) |
141 | 141 | - [out\_wfc\_lcao](#out_wfc_lcao) |
142 | 142 | - [out\_dos](#out_dos) |
| 143 | + - [out\_ldos](#out_ldos) |
143 | 144 | - [out\_band](#out_band) |
144 | 145 | - [out\_proj\_band](#out_proj_band) |
145 | 146 | - [out\_stru](#out_stru) |
|
154 | 155 | - [out\_mat\_dh](#out_mat_dh) |
155 | 156 | - [out\_mat\_xc](#out_mat_xc) |
156 | 157 | - [out\_mat\_xc2](#out_mat_xc2) |
| 158 | + - [out\_mat\_l](#out_mat_l) |
157 | 159 | - [out\_eband\_terms](#out_eband_terms) |
158 | 160 | - [out\_hr\_npz/out\_dm\_npz](#out_hr_npzout_dm_npz) |
159 | 161 | - [dm\_to\_rho](#dm_to_rho) |
|
174 | 176 | - [dos\_emin\_ev](#dos_emin_ev) |
175 | 177 | - [dos\_emax\_ev](#dos_emax_ev) |
176 | 178 | - [dos\_nche](#dos_nche) |
| 179 | + - [stm\_bias](#stm_bias) |
177 | 180 | - [NAOs](#naos) |
178 | 181 | - [bessel\_nao\_ecut](#bessel_nao_ecut) |
179 | 182 | - [bessel\_nao\_tolerence](#bessel_nao_tolerence) |
@@ -1706,6 +1709,12 @@ These variables are used to control the output of properties. |
1706 | 1709 | - lcao-only: output the density of states (DOS) and the projected density of states (PDOS) |
1707 | 1710 | - **Default**: 0 |
1708 | 1711 |
|
| 1712 | +### out_ldos |
| 1713 | + |
| 1714 | +- **Type**: Boolean |
| 1715 | +- **Description**: Whether to output the local density of states for given bias in cube file format, which is controlled by [stm_bias](#stm_bias). |
| 1716 | +- **Default**: False |
| 1717 | + |
1709 | 1718 | ### out_band |
1710 | 1719 |
|
1711 | 1720 | - **Type**: Boolean \[Integer\](optional) |
@@ -1807,6 +1816,13 @@ The band (KS orbital) energy for each (k-point, spin, band) will be printed in t |
1807 | 1816 | - **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`. |
1808 | 1817 | - **Default**: False |
1809 | 1818 |
|
| 1819 | +### out_mat_l |
| 1820 | + |
| 1821 | +- **Type**: Boolean [Integer\](optional) |
| 1822 | +- **Availability**: Numerical atomic orbital (NAO) basis |
| 1823 | +- **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. |
| 1824 | +- **Default**: False 8 |
| 1825 | + |
1810 | 1826 | ### out_eband_terms |
1811 | 1827 |
|
1812 | 1828 | - **Type**: Boolean |
@@ -1955,9 +1971,16 @@ These variables are used to control the calculation of DOS. [Detailed introducti |
1955 | 1971 | ### dos_nche |
1956 | 1972 |
|
1957 | 1973 | - **Type**: Integer |
1958 | | -The order of Chebyshev expansions when using Stochastic Density Functional Theory (SDFT) to calculate DOS. |
| 1974 | +- **Description**: The order of Chebyshev expansions when using Stochastic Density Functional Theory (SDFT) to calculate DOS. |
1959 | 1975 | - **Default**: 100 |
1960 | 1976 |
|
| 1977 | +### stm_bias |
| 1978 | + |
| 1979 | +- **Type**: Real |
| 1980 | +- **Description**: The bias voltage used to calculate local density of states to simulate scanning tunneling microscope, see details in [out_ldos](#out_ldos). |
| 1981 | +- **Default**: 1.0 |
| 1982 | +- **Unit**: V |
| 1983 | + |
1961 | 1984 | [back to top](#full-list-of-input-keywords) |
1962 | 1985 |
|
1963 | 1986 | ## NAOs |
|
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