2019
DOI: 10.1021/acsami.9b08108
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High Thermoelectric Performance in n-Type Polycrystalline SnSe via Dual Incorporation of Cl and PbSe and Dense Nanostructures

Abstract: Despite extensive studies on emerging thermoelectric material SnSe, its n-type form is largely underdeveloped mainly due to the difficulty in stabilizing the carrier concentration at the optimal level. Here, we dually introduce Cl and PbSe to induce n-type conduction in intrinsic p-type SnSe. PbSe alloying enhances the power factor and suppresses lattice thermal conductivity at the same time, giving a highest thermoelectric figure of merit ZT of 1.2 at 823 K for n-type polycrystalline SnSe materials. The best … Show more

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Cited by 49 publications
(29 citation statements)
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“…A summary of ZTs for SnSe‐based thermoelectric materials. a) The timeline for state‐of‐the‐art SnSe bulks thermoelectric materials,11–124,169–182 the performance achieved by solution route are circled by yellow. b) Temperature‐dependent ZT and c) corresponding peak and average ZT values for polycrystalline SnSe through different fabrication techniques 13,16,22,46,58,62,95,99,101.…”
Section: Introductionmentioning
confidence: 99%
“…A summary of ZTs for SnSe‐based thermoelectric materials. a) The timeline for state‐of‐the‐art SnSe bulks thermoelectric materials,11–124,169–182 the performance achieved by solution route are circled by yellow. b) Temperature‐dependent ZT and c) corresponding peak and average ZT values for polycrystalline SnSe through different fabrication techniques 13,16,22,46,58,62,95,99,101.…”
Section: Introductionmentioning
confidence: 99%
“…However, extensive control of the carrier concentration in SnSe is difficult due to thermodynamic solubility restriction of doping elements. Another important purpose of doping in SnSe is to realize n-type SnSe, and doping (co-doping) of Br, 11 I, 12 Bi, 13 Cl, and PbSe, 14 BiCl 3 , 15 and Ti and Pb 16 has been investigated. ZT = 2.2 at 600 K for n-type Bi-doped SnSe 13 and ZT = 2.8 at 900 K for n-type Br-doped SnSe 11 have been reported.…”
Section: ■ Introductionmentioning
confidence: 99%
“…The dominant MFPs of phonons are typically an order of magnitude larger than those of electrons, thus phonon transport suffers more in the presence of nanostructuring. Some of the best results in terms of ZT improvements, however, were achieved in cases where care was taken to avoid power factor reduction [4,17,[36][37][38][39][40][41][42][43]. This is commonly achieved in two ways, either by: (i) aligning the band edges of the nanoinclusions with those of the pristine material to keep the electronic conductivity high, or (ii) going towards the reverse direction, by introducing energy barriers that result in energy filtering and improve the Seebeck coefficient.…”
Section: Introductionmentioning
confidence: 99%