2012
DOI: 10.1103/physrevb.86.104301
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Thermal transport in phase-change materials from atomistic simulations

Abstract: We computed the thermal conductivity (κ) of amorphous GeTe by means of classical molecular dynamics and lattice dynamics simulations. GeTe is a phase change material of interest for applications in nonvolatile memories. An interatomic potential with close-to-ab initio accuracy was used as generated by fitting a huge ab initio database with a neural network method. It turns out that the majority of heat carriers are nonpropagating vibrations (diffusons), the small percentage of propagating modes giving a neglig… Show more

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Cited by 97 publications
(99 citation statements)
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“…Structures were visualized using AtomEye. 9 deed, the only reported ML potential dealing with amorphous matter is a neural-network potential for the phasechange data-storage material GeTe 46 that enabled largescale simulations of thermal transport 47 and atomistic processes during crystallization. 48 Amorphous materials are structurally much more diverse than their crystalline counterparts, and despite the lack of long-range translational symmetry, their properties depend crucially on structural order on the local and intermediate length scales.…”
Section: -6mentioning
confidence: 99%
“…Structures were visualized using AtomEye. 9 deed, the only reported ML potential dealing with amorphous matter is a neural-network potential for the phasechange data-storage material GeTe 46 that enabled largescale simulations of thermal transport 47 and atomistic processes during crystallization. 48 Amorphous materials are structurally much more diverse than their crystalline counterparts, and despite the lack of long-range translational symmetry, their properties depend crucially on structural order on the local and intermediate length scales.…”
Section: -6mentioning
confidence: 99%
“…12,[18][19][20][21][22][23][24][25][26] Computational costs limit DFT calculations to less than 100 atoms, however, making it challenging to explicitly incorporate the effects of disorder. 12,20,22,25,[27][28][29] Disorder is typically included in the ALD framework using Abeles' virtual crystal (VC) approximation, whereby the disordered solid is replaced with a perfect VC with properties equivalent to an averaging over the disorder (e.g., atomic mass and/or bond strength). 14 The ALD calculations are performed on a small unit cell with the averaged properties (i.e., all vibrational modes are phonons) and phononphonon and phonon-disorder scattering are included as perturbations.…”
Section: Introductionmentioning
confidence: 99%
“…For each atom, a vector of symmetry function values is used as input for a separate atomic feed-forward NN, which then yields the corresponding atomic energy contribution to the total energy if trained properly to first principles reference data. Potentials of this type have been constructed very successfully for a number of materials like silicon [40,50,52], sodium [53,54], carbon [55,56], copper [57,58], the phase change material GeTe [59][60][61], large copper clusters supported at zinc oxide [62], and the methanol molecule [58]. The accuracy of the Behler-Parrinello method depends on the chosen cutoff radius of the symmetry functions, which defines the atomic environments.…”
Section: High-dimensional Neural Networkmentioning
confidence: 99%