IMA 2013 UQ: DFT-based Thermal Properties: Three Levels of Error Management

By Kurt Lejaeghere

Center for Molecular Modeling, Ghent University, Ghent, Belgium

Published on

Abstract

It is often computationally expensive to predict finite-temperature properties of a crystal from density-functional theory (DFT). The temperature-dependent thermal expansion coefficient α, for example, is calculated from the phonon spectrum, and the melting temperature Tm can only be obtained from ab initio molecular dynamics. Alternatively, semi-empirical relations already provide good estimates at a significantly lower computational cost. These relations link complex quantities, such as α and Tm, to much simpler DFT predictors, such as the cohesive energy or the bulk modulus. The difference between these semi-empirical estimates and experiment is governed by three sources of errors: the numerical accuracy of the DFT implementation [1,2], the limitations of the exchange-correlation functional [1], and the approximations involved in the semi-empirical relation itself [3]. We quantify each of these errors, and find them to contribute according to the order of listing: least for the implementation dependence and most for the effect of the semi-empirical relation. Despite these deviations, some semi-empirical relations do outperform more fundamental methods. An estimate for the Grüneisen parameter that is based on the pressure derivative of the bulk modulus, for example, yields better predictions for the thermal expansion coefficient at room temperature than quasiharmonic phonon theory [3].

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References

  1. K. Lejaeghere, V. Van Speybroeck, G. Van Oost, and S. Cottenier, ' Error Estimates for Solid-State Density-Functional Theory Predictions: An Overview by Means of the Ground-State Elemental Crystals', Crit. Rev. Solid State 39, 1-24 (2014). [open access at DOI: 10.1080/10408436.2013.772503]
  2. https://molmod.ugent.be/DeltaCodesDFT
  3. K. Lejaeghere, J. Jaeken, V. Van Speybroeck, and S. Cottenier, 'Ab-initio-based thermal property predictions at a low cost: an error analysis', submitted to Phys. Rev. B.

Cite this work

Researchers should cite this work as follows:

  • Kurt Lejaeghere (2014), "IMA 2013 UQ: DFT-based Thermal Properties: Three Levels of Error Management," https://nanohub.org/resources/20311.

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Location

Lind Hall, University of Minnesota, Minneapolis, MN

Tags

IMA 2013 UQ: DFT-based Thermal Properties: Three Levels of Error Management
  • DFT-based thermal properties: three levels of error management 1. DFT-based thermal properties: … 0
    00:00/00:00
  • Temperature can critically change materials properties 2. Temperature can critically cha… 12.645979312645979
    00:00/00:00
  • Temperature can critically change materials properties 3. Temperature can critically cha… 58.758758758758759
    00:00/00:00
  • First-principles predictions of thermal properties are not trivial 4. First-principles predictions o… 75.508842175508846
    00:00/00:00
  • First-principles predictions of thermal properties are not trivial 5. First-principles predictions o… 155.7223890557224
    00:00/00:00
  • Semi-empirical predictions: the best of both worlds? 6. Semi-empirical predictions: th… 264.76476476476478
    00:00/00:00
  • Semi-empirical predictions: the best of both worlds? 7. Semi-empirical predictions: th… 474.40774107440774
    00:00/00:00
  • Three levels of error management 8. Three levels of error manageme… 507.17384050717385
    00:00/00:00
  • Three levels of error management 9. Three levels of error manageme… 536.50316983650316
    00:00/00:00
  • Three levels of error management 10. Three levels of error manageme… 575.90924257590927
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  • Three levels of error management 11. Three levels of error manageme… 612.21221221221219
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  • Three levels of error management 12. Three levels of error manageme… 630.73073073073078
    00:00/00:00
  • A comprehensive solid-state benchmark set is needed 13. A comprehensive solid-state be… 707.70770770770775
    00:00/00:00
  • Content 14. Content 730.69736403069737
    00:00/00:00
  • The Δ-gauge compares equations of state 15. The Δ-gauge compares equation… 734.76810143476814
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  • How to compare implementations 16. How to compare implementations 793.5935935935936
    00:00/00:00
  • How to compare implementations 17. How to compare implementations 839.73973973973978
    00:00/00:00
  • Δ as a numerical quality factor 18. Δ as a numerical quality fact… 886.15281948615291
    00:00/00:00
  • Δ as a numerical quality factor 19. Δ as a numerical quality fact… 920.72072072072081
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  • Δ as a numerical quality factor 20. Δ as a numerical quality fact… 1072.2055388722056
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  • Content 21. Content 1100.3003003003003
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  • Systematic and residual errors 22. Systematic and residual errors 1118.7854521187855
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  • Outliers are not representative 23. Outliers are not representativ… 1162.6626626626628
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  • Outliers are not representative 24. Outliers are not representativ… 1178.2449115782449
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  • Outliers are not representative 25. Outliers are not representativ… 1188.4551217884552
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  • Automatic outlier detection 26. Automatic outlier detection 1247.3139806473141
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  • From statistics to intrinsic errors 27. From statistics to intrinsic e… 1291.358024691358
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  • Overview for different properties 28. Overview for different propert… 1328.6286286286286
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  • Content 29. Content 1362.7961294627962
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  • Thermal expansion 30. Thermal expansion 1368.4017350684019
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  • Thermal expansion 31. Thermal expansion 1411.0110110110111
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  • Melting temperature 32. Melting temperature 1415.8491825158492
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  • Semi-empirical errors 33. Semi-empirical errors 1426.6266266266266
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  • Two possible reasons for outliers 34. Two possible reasons for outli… 1463.2298965632299
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  • Semi-empirical ≈ high-level theory 35. Semi-empirical ≈ high-level … 1616.016016016016
    00:00/00:00
  • Content 36. Content 1768.2015348682016
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  • Intrinsic >> numerical errors 37. Intrinsic >> numerical errors 1778.4784784784786
    00:00/00:00
  • Semi-empirical >> intrinsic errors 38. Semi-empirical >> intrinsic er… 1826.4931598264932
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  • Content 39. Content 1898.3650316983651
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  • Conclusion 40. Conclusion 1902.5358692025359
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  • Acknowledgments 41. Acknowledgments 1942.9095762429097
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  • More information? 42. More information? 1964.964964964965
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