Semiconductor-to-semimetal transition on Te doping in a new semiconducting material Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub>

Semiconducting antimony-containing chalcogenides are an emerging class of materials for their applications in the thermoelectric and optoelectronic fields. A series of new polycrystalline antimony-containing chalcogenides Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> (<i>δ</i> = 0 to 4) have been prepared by heating the elements at 1073 K. The parent monoclinic selenide, Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub>, adopts the <i>P</i>2<sub>1</sub>/<i>c</i> space group, as determined by a single-crystal X-ray diffraction study. The selenide structure consists of 2∞[Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub>]<sup>5.5-</sup> layers in which Pb and Sb sites are disordered. The PXRD studies show that a maximum of 40% of Se atoms in the Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub> structure can be substituted by Te atoms. The refined unit cell volume of the polycrystalline Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> increases almost linearly with <i>δ</i> values following Vegard's law. Optical bandgap measurements indicate the semiconducting nature of the <i>δ</i> = 0, 1, and 2 samples, whereas no bandgap transition was found for the <i>δ</i> = 3 and 4 compositions. Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub> exhibits an ultra-low thermal conductivity (<i>κ</i><sub>tot</sub>) of ∼0.24 W m<sup>-1</sup> K<sup>-1</sup> at 773 K. The substitution of the Te atoms at the Se sites of the Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub> structure significantly improves electrical conductivity values. The <i>δ</i> = 3 and 4 compositions of the Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> series show the semimetal-like temperature dependence of electrical conductivity. The <i>z</i>T value of the <i>δ</i> = 2 composition is almost zero at 773 K due to its poor electrical conductivity. A further increase in Te concentration in Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> leads to an enhancement of the <i>z</i>T value (= 0.09 for <i>δ</i> = 4) at 773 K.

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Journal
Dalton Transactions
Published
2025-01-01
DOI
https://doi.org/10.1039/d5dt01185j
Primary Topic
Advanced Thermoelectric Materials and Devices
Type
article
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article

Semiconductor-to-semimetal transition on Te doping in a new semiconducting material Ba2.75Pb1.1Sb4.1Se10

Subhendu Jana, Sayani Barman, Sweta Yadav, Swati et al.
Dalton Transactions
Advanced Thermoelectric Materials and Devices
article

Semiconductor-to-semimetal transition on Te doping in a new semiconducting material Ba2.75Pb1.1Sb4.1Se10

Subhendu Jana, Sayani Barman, Sweta Yadav, Swati, Jai Prakash
article en

Abstract

Semiconducting antimony-containing chalcogenides are an emerging class of materials for their applications in the thermoelectric and optoelectronic fields. A series of new polycrystalline antimony-containing chalcogenides Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> (<i>δ</i> = 0 to 4) have been prepared by heating the elements at 1073 K. The parent monoclinic selenide, Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub>, adopts the <i>P</i>2<sub>1</sub>/<i>c</i> space group, as determined by a single-crystal X-ray diffraction study. The selenide structure consists of 2∞[Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub>]<sup>5.5-</sup> layers in which Pb and Sb sites are disordered. The PXRD studies show that a maximum of 40% of Se atoms in the Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub> structure can be substituted by Te atoms. The refined unit cell volume of the polycrystalline Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> increases almost linearly with <i>δ</i> values following Vegard's law. Optical bandgap measurements indicate the semiconducting nature of the <i>δ</i> = 0, 1, and 2 samples, whereas no bandgap transition was found for the <i>δ</i> = 3 and 4 compositions. Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub> exhibits an ultra-low thermal conductivity (<i>κ</i><sub>tot</sub>) of ∼0.24 W m<sup>-1</sup> K<sup>-1</sup> at 773 K. The substitution of the Te atoms at the Se sites of the Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10</sub> structure significantly improves electrical conductivity values. The <i>δ</i> = 3 and 4 compositions of the Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> series show the semimetal-like temperature dependence of electrical conductivity. The <i>z</i>T value of the <i>δ</i> = 2 composition is almost zero at 773 K due to its poor electrical conductivity. A further increase in Te concentration in Ba<sub>2.75</sub>Pb<sub>1.1</sub>Sb<sub>4.1</sub>Se<sub>10-<i>δ</i></sub>Te<sub><i>δ</i></sub> leads to an enhancement of the <i>z</i>T value (= 0.09 for <i>δ</i> = 4) at 773 K.

Dalton TransactionsVol. 54(36)
Indian Institute of Technology Hyderabad (IN)
Council of Scientific and Industrial Research, India, Science and Engineering Research Board
Openalex Percentile: Top 83%
Advanced Thermoelectric Materials and Devices
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