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Methods | Analytical model | ALD calculation | MD simulation |
Standard SMRTA | Iterative Scheme | Time NMA | Frequency NMA |
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Equations | Table 1 | Equations (14), (15), and (16) | Equations (14), (15), (16), (17), and (18) | Equations (30), (31), and (33) | Equations (33) and (35) | Equations (33) and (36) |
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Characteristics | Lots of approximations, need fitting parameters | and processes are independent thermal resistant sources | process does not provide thermal resistant itself | Eigenvectors needed | Eigenvectors not needed |
Need 2nd- and 3rd-order IFCs | Need interatomic potential (or ab initio MD) |
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Suitable for | Long wavelength, Debye model |
Low temperature higher-order anharmonicity not large | Higher than Debye temperature |
Temperature not too low, quantum effect negligible |
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Accuracy | Low | Medium | Higher | Higher |
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Computational complexity | | High | Higher | Low |
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Applications so far | Some thermal conductivity analysis and prediction |
Pure and isotope-doped bulk, alloy superlattice, nanostructures | Pure lattice Materials with surrounding influences |
Further research |
Temperature dependent IFCs, 4th- and higher-order phonon scattering |
Accurate interatomic potential, large domain first principle MD, defects, boundaries |
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