2015
DOI: 10.1016/j.nanoen.2015.09.015
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Large enhancement of thermoelectric performance of CuInTe 2 via a synergistic strategy of point defects and microstructure engineering

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Cited by 82 publications
(71 citation statements)
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“…In addition, the nanostructuring approach was also employed [133,134]. The enhanced thermoelectric performance can be attributed to the phonon scattering introduced by crystal defects and the increased density of states near the Fermi level, such as (CuInTe 2 ) 0.99 (ZnTe) 0.01 composited with 0.1 wt% TiO 2 nanofiber (zT~1.47 at 823 K) [135], CuInTe 2 composited ZnO (zT~1.61 at 823 K) [34].…”
Section: Tetragonal Diamond-like Compoundsmentioning
confidence: 99%
“…In addition, the nanostructuring approach was also employed [133,134]. The enhanced thermoelectric performance can be attributed to the phonon scattering introduced by crystal defects and the increased density of states near the Fermi level, such as (CuInTe 2 ) 0.99 (ZnTe) 0.01 composited with 0.1 wt% TiO 2 nanofiber (zT~1.47 at 823 K) [135], CuInTe 2 composited ZnO (zT~1.61 at 823 K) [34].…”
Section: Tetragonal Diamond-like Compoundsmentioning
confidence: 99%
“…where is the reduced Plank constant, k B is the Boltzmann constant, θ is the Debye temperature, υ is the phonon velocity of CuInTe 2 compound, z is the usual dimensionless variable ω/k B T , and τ is the phonon relaxation time, which can be expressed as [ 24 ] τ τ τ τ τ γ ω ν θ π ω π π ω ( ) …”
Section: In Situ Nanoinclusionsmentioning
confidence: 99%
“…However, its widespread application is still restricted by the low conversion effi ciency of thermoelectric materials, [ 1 ] which is usually determined by the dimensionless fi gure of merit, ZT = S 2 σT / κ = S 2 σT /( κ e + κ l ), where S is the Seebeck coeffi cient; σ is the electrical conductivity; T is the absolute temperature; κ , κ e , and κ l are the total, electronic, and lattice thermal conductivities, respectively. [ 2 ] previous TiO 2 added sample, [ 24 ] thus reducing its output power. Therefore, how to realize a concurrent improvement of both the electrical and thermal transport properties is a tough challenge to be conquered.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…They include enhancement of the electrical conductivity by enhancing the carrier concentration with chemical doping and carrier injection, enhancement of the Seebeck coefficient though band engineering (band convergence, resonant level, electronic density of states distortion, Fermi level pinning) and carrier engineering (minority carrier blocking, energy barrier filtering) . On the other hand, the thermal conductivity can be reduced through tailoring the independent κ L through introducing phonon scattering by atomic‐scale point defects, nanoscale dislocations, stacking faults and particles, mesoscale grains and boundaries, as well as multiscale hierarchical architectures …”
Section: Introductionmentioning
confidence: 99%