2016
DOI: 10.1103/physrevb.94.125203
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Origin of low thermal conductivity in SnSe

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Cited by 339 publications
(246 citation statements)
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“…However, our screening criteria are stricter: especially in the lattice thermal conductivity ( <1 W/mK) or strong anharmonicity ( >2). Following our strict criteria, PbTe cannot be screened due to its small Grüneisen parameter ( =1.13) and high thermal conductivity (>1 W/mK) which is in good agreement with the experimentally measured ~2.3 W/mK at 300 K [92] . Similarly, other some previously reported thermoelectric materials [PbS (225) and PbSe (225)] with small Grüneisen parameter ( < 2) are not predicted.…”
Section: Promising Binary Chalcogenide Thermoelectric Materialssupporting
confidence: 87%
“…However, our screening criteria are stricter: especially in the lattice thermal conductivity ( <1 W/mK) or strong anharmonicity ( >2). Following our strict criteria, PbTe cannot be screened due to its small Grüneisen parameter ( =1.13) and high thermal conductivity (>1 W/mK) which is in good agreement with the experimentally measured ~2.3 W/mK at 300 K [92] . Similarly, other some previously reported thermoelectric materials [PbS (225) and PbSe (225)] with small Grüneisen parameter ( < 2) are not predicted.…”
Section: Promising Binary Chalcogenide Thermoelectric Materialssupporting
confidence: 87%
“…This phenomenon also confirms the presence of excess low‐frequency optical phonon density of states which interact with acoustic phonons, resulting in suppressed phonon group velocities and hence ultra‐low κ lat. Further we have derived average sound velocity (ν a ) of BiTe which is approximately 1760 m s −1 using the equation of ΘD=hkB3N4πV1/3υa , where h is Plank′s constant, k B is the Boltzmann constant, N is number of atoms per unit cell and V is volume of the unit cell . Low sound velocity of BiTe partly explains the low κ lat of BiTe.…”
Section: Resultsmentioning
confidence: 99%
“…As a result, there have been efforts to search for low thermal conductivity materials through nanostructure engineering, i.e., using thin films, superlattices, nanostructured samples, and disordered crystals . In general, low thermal conductivity in these compounds may arise from material characteristics like strong crystal anharmonicity, complex crystal structure, atomic disorders, large molecular weight, large unit cells or lone pair of electrons, and so on . However, it remains an elusive goal to achieve ultralow thermal conductivity while maintaining some degree of crystallinity.…”
Section: Introductionmentioning
confidence: 99%