[go: up one dir, main page]
More Web Proxy on the site http://driver.im/

Ahmad et al., 2020 - Google Patents

Band Convergence and Phonon Scattering Mediated Improved Thermoelectric Performance of SnTe–PbTe Nanocomposites

Ahmad et al., 2020

View PDF
Document ID
10216180551413707314
Author
Ahmad S
Singh A
Bhattacharya S
Navaneethan M
Basu R
Bhatt R
Sarkar P
Meshram K
Debnath A
Muthe K
Aswal D
Publication year
Publication venue
ACS Applied Energy Materials

External Links

Snippet

SnTe exhibits poor thermoelectric figure of merit owing to Sn vacancies that give rise to a low p-type Seebeck coefficient and high electrical–thermal conductivities. Here, we reported thermoelectric properties of a composite material synthesized by vacuum hot pressing a …
Continue reading at www.academia.edu (PDF) (other versions)

Classifications

    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L35/00Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L35/12Selection of the material for the legs of the junction
    • H01L35/14Selection of the material for the legs of the junction using inorganic compositions
    • H01L35/16Selection of the material for the legs of the junction using inorganic compositions comprising tellurium or selenium or sulfur
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L35/00Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L35/12Selection of the material for the legs of the junction
    • H01L35/14Selection of the material for the legs of the junction using inorganic compositions
    • H01L35/18Selection of the material for the legs of the junction using inorganic compositions comprising arsenic or antimony or bismuth, e.g. AIIIBV compounds
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L35/00Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L35/28Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof operating with Peltier or Seebeck effect only
    • H01L35/32Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof operating with Peltier or Seebeck effect only characterised by the structure or configuration of the cell or thermo-couple forming the device including details about, e.g., housing, insulation, geometry, module
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L35/00Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L35/28Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof operating with Peltier or Seebeck effect only
    • H01L35/30Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof operating with Peltier or Seebeck effect only characterised by the heat-exchanging means at the junction
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L35/00Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L35/34Processes or apparatus peculiar to the manufacture or treatment of these devices or of parts thereof
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L31/00Semiconductor devices sensitive to infra-red radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/0248Semiconductor devices sensitive to infra-red radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies
    • H01L31/0256Semiconductor devices sensitive to infra-red radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by the material
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L39/00Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
    • H01L39/02Details
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies; Multistep manufacturing processes therefor
    • H01L29/12Semiconductor bodies; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • HELECTRICITY
    • H01BASIC ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H01L35/00Thermo-electric devices comprising a junction of dissimilar materials, i.e. exhibiting Seebeck or Peltier effect with or without other thermo-electric effects or thermomagnetic effects; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L35/02Details

Similar Documents

Publication Publication Date Title
Berry et al. Enhancing thermoelectric performance of TiNiSn half-Heusler compounds via modulation doping
Wang et al. High porosity in nanostructured n-type Bi2Te3 obtaining ultralow lattice thermal conductivity
Roychowdhury et al. Phonon localization and entropy-driven point defects lead to ultralow thermal conductivity and enhanced thermoelectric performance in (SnTe) 1–2 x (SnSe) x (SnS) x
Cha et al. Ultrahigh power factor and electron mobility in n-type Bi2Te3–x% Cu stabilized under excess Te condition
Girard et al. High performance Na-doped PbTe–PbS thermoelectric materials: electronic density of states modification and shape-controlled nanostructures
Tan et al. Rationally designing high-performance bulk thermoelectric materials
Jin et al. Investigation on low-temperature thermoelectric properties of Ag2Se polycrystal fabricated by using zone-melting method
Chauhan et al. Defect engineering for enhancement of thermoelectric performance of (Zr, Hf) NiSn-based n-type half-Heusler alloys
Wang et al. Ga-doping-induced carrier tuning and multiphase engineering in n-type PbTe with enhanced thermoelectric performance
Yao et al. Synergistic strategy to enhance the thermoelectric properties of CoSbS1–x Se x Compounds via solid solution
Dargusch et al. In-situ observation of the continuous phase transition in determining the high thermoelectric performance of polycrystalline Sn0. 98Se
Chen et al. Extraordinary role of Bi for improving thermoelectrics in low-solubility SnTe–CdTe alloys
Ahmad et al. Band Convergence and Phonon Scattering Mediated Improved Thermoelectric Performance of SnTe–PbTe Nanocomposites
Li et al. Realization of high thermoelectric performance in polycrystalline tin selenide through schottky vacancies and endotaxial nanostructuring
Yang et al. Enhanced thermoelectric performance of Zr1–x Ta x NiSn half-heusler alloys by diagonal-rule doping
Tian et al. Enhanced thermoelectric performance of SnTe-based materials via interface engineering
Zhang et al. Band engineering SnTe via trivalent substitutions for enhanced thermoelectric performance
Liu et al. Tuning the carrier scattering mechanism by rare-earth element doping for high average zT in Mg3Sb2-based compounds
Yue et al. Band engineering and thermoelectric performance optimization of p-type GeTe-based alloys through Ti/Sb co-doping
Zhou et al. Reduced thermal conductivity of Mg2 (Si, Sn) solid solutions by a gradient composition layered microstructure
Li et al. Ultralow thermal conductivity and extraordinary thermoelectric performance realized in codoped Cu3SbSe4 by plasma spark sintering
Xu et al. Synergistically Optimized Thermal Conductivity and Carrier Concentration in GeTe by Bi–Se Codoping
Ahmad et al. Remarkable improvement of thermoelectric figure-of-merit in SnTe through in situ-created Te nanoinclusions
Feng et al. Ag Interstitial Inhibition and Phonon Scattering at the ZnSe Nano-Precipitates to Enhance the Thermoelectric Performance of Ag2Se
Siddique et al. Realizing high thermoelectric performance in p-Type SnSe crystals via convergence of multiple electronic valence bands