Publication: Polycrystalline ZrTe5 parametrized as a narrow-band-gap semiconductor for thermoelectric performance
dc.contributor.coauthor | Miller, Samuel A. | |
dc.contributor.coauthor | Witting, Ian | |
dc.contributor.coauthor | Peng, Lintao | |
dc.contributor.coauthor | Rettie, Alexander J. E. | |
dc.contributor.coauthor | Gorai, Prashun | |
dc.contributor.coauthor | Chung, Duck Young | |
dc.contributor.coauthor | Kanatzidis, Mercouri G. | |
dc.contributor.coauthor | Grayson, Matthew | |
dc.contributor.coauthor | Stevanovic, Vladan | |
dc.contributor.coauthor | Toberer, Eric S. | |
dc.contributor.coauthor | Snyder, G. Jeffrey | |
dc.contributor.department | Department of Chemistry | |
dc.contributor.kuauthor | Aydemir, Umut | |
dc.contributor.schoolcollegeinstitute | College of Sciences | |
dc.date.accessioned | 2024-11-09T13:09:36Z | |
dc.date.issued | 2018 | |
dc.description.abstract | 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. | |
dc.description.fulltext | YES | |
dc.description.indexedby | WOS | |
dc.description.indexedby | Scopus | |
dc.description.issue | 1 | |
dc.description.openaccess | YES | |
dc.description.publisherscope | International | |
dc.description.sponsoredbyTubitakEu | N/A | |
dc.description.sponsorship | National Science Foundation Division of Materials Research (DMR) | |
dc.description.sponsorship | Department of Energy's Office of Energy Efficiency and Renewable Energy | |
dc.description.sponsorship | U.S. Department of Energy, Office of Science, Basic Energy Sciences | |
dc.description.sponsorship | Air Force Office of Scientific Research (AFOSR) | |
dc.description.sponsorship | U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division | |
dc.description.sponsorship | Materials Research Science and Engineering Centers (MRSEC) program of the National Science Foundation (NSF) at the Materials Research Center of Northwestern University | |
dc.description.sponsorship | Soft and Hybrid Nanotechnology Experimental Resource (NSF) | |
dc.description.version | Publisher version | |
dc.description.volume | 9 | |
dc.identifier.doi | 10.1103/PhysRevApplied.9.014025 | |
dc.identifier.eissn | 2331-7019 | |
dc.identifier.embargo | NO | |
dc.identifier.filenameinventoryno | IR01443 | |
dc.identifier.quartile | N/A | |
dc.identifier.scopus | 2-s2.0-85041097690 | |
dc.identifier.uri | https://hdl.handle.net/20.500.14288/2766 | |
dc.identifier.wos | 423328300002 | |
dc.keywords | Transition-metal pentatellurides | |
dc.keywords | Thermal-conductivity | |
dc.keywords | Electronic-structure | |
dc.keywords | Dimensional zrte5 | |
dc.keywords | Phase-transition | |
dc.keywords | Hfte5 | |
dc.keywords | Resistivity | |
dc.keywords | Transport | |
dc.keywords | Power | |
dc.keywords | Oscillations | |
dc.language.iso | eng | |
dc.publisher | American Physical Society (APS) | |
dc.relation.grantno | 1334713 | |
dc.relation.grantno | 1334351 | |
dc.relation.grantno | 1333335 | |
dc.relation.grantno | DE-SC0001299/DE-FG02-09ER46577 | |
dc.relation.grantno | FA9550-15-10247 | |
dc.relation.grantno | FA9550-15-1-0377 | |
dc.relation.grantno | DE-AC02-06CH11357 | |
dc.relation.grantno | DMR-1121262 | |
dc.relation.grantno | NNCI-1542205 | |
dc.relation.ispartof | Physical Review Applied | |
dc.relation.uri | http://cdm21054.contentdm.oclc.org/cdm/ref/collection/IR/id/8026 | |
dc.subject | Physics, applied | |
dc.title | Polycrystalline ZrTe5 parametrized as a narrow-band-gap semiconductor for thermoelectric performance | |
dc.type | Journal Article | |
dspace.entity.type | Publication | |
local.contributor.kuauthor | Aydemir, Umut | |
local.publication.orgunit1 | College of Sciences | |
local.publication.orgunit2 | Department of Chemistry | |
relation.isOrgUnitOfPublication | 035d8150-86c9-4107-af16-a6f0a4d538eb | |
relation.isOrgUnitOfPublication.latestForDiscovery | 035d8150-86c9-4107-af16-a6f0a4d538eb | |
relation.isParentOrgUnitOfPublication | af0395b0-7219-4165-a909-7016fa30932d | |
relation.isParentOrgUnitOfPublication.latestForDiscovery | af0395b0-7219-4165-a909-7016fa30932d |
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