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* update SIAB codes
* add README.md in tools
* update SIAB package
* small fix for the file
* add geometry index for outputting density matrix in k space
* update output of dmk
* fix bug in io_dmk_test
* update output context of dmk
* rename io_dmk to write_dmk
* update dmr and dmk parameters, add precision control of the two parameters
* update sparse matrix format
* update write_dmk
* update write dmk
* update documents for out_dmk
* fix bug about dmk and dmr
* update input-main.md
* fix a bug in out_mat_hs and out_chg that cannot read notes
* fix bug when reading the second parameter of dmk, dmr, out_chg, out_mat_hs, out_mat_tk, out_mat_l
* update tests of input parameters
* update out_chg command
* fix exx error due to nrxx>0
* fix bug
* update makefile
* update assert of nrxx, which can be 0 in some cases
- nspin = 2: `dms1k1_nao.csr`... and `dms2k1_nao.csr`... for the two spin channels.
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- nspin = 1 and 4: `dmk1_nao.csr`, `dmk2_nao.csr`, ...;
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- nspin = 2: `dmk1s1_nao.csr`... and `dmk1s2_nao.csr`... for the two spin channels.
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-**Default**: False
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-**Note**: In the 3.10-LTS version, the parameter is named `out_dm` and the file names are SPIN1_DM and SPIN2_DM, etc.
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### out_dmr
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-**Type**: Boolean
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-**Type**: Boolean\[Integer\](optional)
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-**Availability**: Numerical atomic orbital basis (multi-k points)
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-**Description**: Whether to output the density matrix with Bravias lattice vector R index into files in the folder `OUT.${suffix}`. The files are named as `dmr{s}{spin index}{g}{geometry index}{_nao} + {".csr"}`. Here, 's' refers to spin, where s1 means spin up channel while s2 means spin down channel, and the sparse matrix format 'csr' is mentioned in [out_mat_hs2](#out_mat_hs2). Finally, if [out_app_flag](#out_app_flag) is set to false, the file name contains the optional 'g' index for each ionic step that may have different geometries, and if [out_app_flag](#out_app_flag) is set to true, the density matrix with respect to Bravias lattice vector R accumulates during ionic steps:
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