Table 1 Summary of representative machine learning works on the direct prediction of lattice thermal conductivities in recent 5 years.

From: Predicting lattice thermal conductivity via machine learning: a mini review

Training and testing sets

Input features

Algorithms

the κL of 120 compounds at 300 K, obtained from first-principles calculations15

maximum phonon frequency, integrated Grüneisen parameter up to 3 THz, average atomic mass, and volume of the unit cell

GPR, SISSO

the 2146 κL of 119 compounds at various temperatures from 100 to 1000 K, obtained from first-principles calculations16

before filtering: 126 crystal features mainly generated based on Wigner-Seitz cells, 145 elemental features, and temperature

RF

the κL of 110 compounds at 300 K, obtained from first-principles calculations28

a set of descriptors from simple elemental and structural representations

BO

the κL of 5486 compounds at 300 K, obtained from the AGL method44

7 crystal properties, 25 CW elemental properties, 25 crystal structure fingerprints, and 18 statistical properties

XGBoost

the κL of 1700 RMLs and their corresponding 1700 GMLs at 30 K, obtained from MD simulations45

the thickness sequence, the thickness- and period-based index of randomization, the standard deviation of thickness, the maximum and minimum deviation of layer thickness with respect to the mean layer thickness of RML

NN

the κL of 86 HH compounds at 300 K, obtained from first-principles calculations or experimental measurements46

lattice constants and 24 elemental features

SISSO

initialization: the κL of 100 porous graphene structures at 300 K, obtained from MD simulations47

a gray image representing the spatial distribution of the holes

CNN + active learning

initialization: the κL of 100 hybrid carbon-boron nitride honeycombs (C-BNHCs) at 300 K, obtained from MD simulations50

a grayscale image representing the top-view schematic of C-BNHC

CNN + active learning

(1) the κL of 2668 compounds at 300 K, obtained from high-throughput first-principles calculations. (2) the κL of 132 compounds at 300 K, obtained from experimental measurements51

a graph representing the connection of atoms in the crystal

CGCNN + transfer learning

(1) the harmonic three-phonon scattering phase space of 320 crystals, obtained from first-principles calculations. (2) the κL of 45 crystals at 300 K, obtained from first-principles calculations53

290 elemental features

NN, RF + transfer learning

initialization: the κL of 300 randomly generated Si/Ge RMLs at 300 K, obtained from MD simulations57

N-bit array: N is the number of unit cells in the RML, and one can input a value of 1 or 2 depending on whether the corresponding unit cell consists of Si or Ge atoms, respectively

CNN + active learning