4.5 Article

Polycrystalline ZrTe5 Parametrized as a Narrow-Band-Gap Semiconductor for Thermoelectric Performance

期刊

PHYSICAL REVIEW APPLIED
卷 9, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevApplied.9.014025

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资金

  1. National Science Foundation Division of Materials Research (DMR) [1334713, 1334351, 1333335]
  2. Department of Energy's Office of Energy Efficiency and Renewable Energy
  3. U.S. Department of Energy, Office of Science, Basic Energy Sciences [DE-SC0001299/DE-FG02-09ER46577]
  4. Air Force Office of Scientific Research (AFOSR) [FA9550-15-10247, FA9550-15-1-0377]
  5. U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division [DE-AC02-06CH11357]
  6. Materials Research Science and Engineering Centers (MRSEC) program of the National Science Foundation (NSF) at the Materials Research Center of Northwestern University [DMR-1121262]
  7. Soft and Hybrid Nanotechnology Experimental Resource (NSF) [NNCI-1542205]

向作者/读者索取更多资源

The transition-metal pentatellurides HfTe 5 and ZrTe 5 have been studied for their exotic transport properties with much debate over the transport mechanism, band gap, and cause of the resistivity behavior, including a large low-temperature resistivity peak. Single crystals grown by the chemical-vapor-transport method have shown an n-p transition of the Seebeck coefficient at the same temperature as a peak in the resistivity. We show that behavior similar to that of single crystals can be observed in iodine-doped polycrystalline samples but that undoped polycrystalline samples exhibit drastically different properties: they are p type over the entire temperature range. Additionally, the thermal conductivity for polycrystalline samples is much lower, 1.5 Wm(-1) K-1, than previously reported for single crystals. It is found that the polycrystalline ZrTe 5 system can be modeled as a simple semiconductor with conduction and valence bands both contributing to transport, separated by a band gap of 20 meV. This model demonstrates to first order that a simple two-band model can explain the transition from n-to p-type behavior and the cause of the anomalous resistivity peak. Combined with the experimental data, the two-band model shows that carrier concentration variation is responsible for differences in behavior between samples. Using the twoband model, the thermoelectric performance at different doping levels is predicted, finding zT = 0.2 and 0.1 for p and n type, respectively, at 300 K, and zT = 0.23 and 0.32 for p and n type at 600 K. Given the reasonably high zT that is comparable in magnitude for both n and p type, a thermoelectric device with a single compound used for both legs is feasible.

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