Publication date: Mar 08, 2023
First-principles calculations of phonons are often based on the adiabatic approximation, and Brillouin-zone samplings that might not always be sufficient to capture the subtleties of Kohn anomalies. These shortcomings can be addressed through corrections to the phonon self-energy arising from the low-energy electrons. A well-founded correction method exists [Phys. Rev. B 82, 165111 (2010)], which only relies on adiabatically screened quantities. However, many-body theory suggests to use one bare electron-phonon vertex in the phonon self-energy [Rev. Mod. Phys. 89, 015003 (2017)] to avoid double counting. We assess the accuracy of both approaches in estimating the low-temperature phonons of monolayer TaS₂ and doped MoS₂. We find that the former yields excellent results at low computational cost due to its designed error cancellation to first order, while the latter becomes exact in the many-body limit but is not accurate in approximate contexts. We offer a third strategy based on downfolding to partially screened phonons and interactions [Phys. Rev. B 92, 245108 (2015)] to keep both advantages. This is the natural scheme to include the electron-electron interaction and tackle phonons in strongly correlated materials and nonadiabatic renormalization of the electron-phonon vertex. This record contains (i) a patch for the PHonon and EPW codes of Quantum ESPRESSO, (ii) the Python scripts and data necessary to create all figures shown in our paper, (iii) a minimal working example of the optimization of quadrupole tensors, and (iv) the Quantum ESPRESSO input files we have used.
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File name | Size | Description |
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README.md
MD5md5:70499f843ea92442729fb2caea309527
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7.0 KiB | Installation and usage instructions |
qe2screen.patch
MD5md5:6d6762f6910e250ac72ed75552986945
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296.1 KiB | Quantum ESPRESSO source-code modifications |
requirements.txt
MD5md5:d9a4c00e608a3537bf4642d3df2ad4da
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59 Bytes | List of Python dependencies |
fig01.tar.gz
MD5md5:c60c28dbaa8978c7b5f53bcc49692824
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1.2 KiB | Python script and data to create Fig. 1 |
fig02.tar.gz
MD5md5:5ccbcb726dc4d127e0cd1785f9011f0c
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1.3 KiB | Python script and data to create Fig. 2 |
fig03.tar.gz
MD5md5:a74c6d6f5f88f5810ddf663cd16c8543
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346.9 KiB | Python script and data to create Fig. 3 |
fig04.tar.gz
MD5md5:f4e270639430063f692d693c023e159f
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117.4 KiB | Python script and data to create Fig. 4 |
fig05.tar.gz
MD5md5:892b890550167c8199e42f2d3f18ba17
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387.3 KiB | Python script and data to create Fig. 5 |
fig06.tar.gz
MD5md5:156f23a5c536abecdce504c68d246135
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31.5 KiB | Python script and data to create Fig. 6 |
fig07.tar.gz
MD5md5:8fbc989f96ac45e408322b8479e68898
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217.7 KiB | Python script and data to create Fig. 7 |
fig08.tar.gz
MD5md5:ed653639bfe8151db1dc3fdcf16ffc4f
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96.0 KiB | Python script and data to create Fig. 8 |
fig09.tar.gz
MD5md5:d85033bd2de7ef362db358c3b557692d
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55.9 KiB | Python script and data to create Fig. 9 |
fig10.tar.gz
MD5md5:5c4cfe42cf5cff5e652013170510c229
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228.8 KiB | Python script and data to create Fig. 10 |
fig11.tar.gz
MD5md5:505577b648c8c496b6863d798e512d0e
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149.2 KiB | Python script and data to create Fig. 11 |
fitQ.tar.gz
MD5md5:cee0f6719bc9f2870867f6f7637fd4d1
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3.3 KiB | Example of optimization of quadrupole tensors |
input.tar.gz
MD5md5:f0bbc234d05b8adeccb1aa9a9d5bdb09
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3.3 KiB | Quantum ESPRESSO input files |
2023.146 (version v3) | Sep 21, 2023 | DOI10.24435/materialscloud:he-pv |
2023.103 (version v2) | Jul 03, 2023 | DOI10.24435/materialscloud:dx-bw |
2023.39 (version v1) [This version] | Mar 08, 2023 | DOI10.24435/materialscloud:9f-dn |