3 research outputs found
Decoupling the Electrical Conductivity and Seebeck Coefficient in the <i>RE</i><sub>2</sub>SbO<sub>2</sub> Compounds through Local Structural Perturbations
Compromise between the electrical conductivity and Seebeck
coefficient
limits the efficiency of chemical doping in the thermoelectric research.
An alternative strategy, involving the control of a local crystal
structure, is demonstrated to improve the thermoelectric performance
in the <i>RE</i><sub>2</sub>SbO<sub>2</sub> system. The <i>RE</i><sub>2</sub>SbO<sub>2</sub> phases, adopting a disordered <i>anti</i>-ThCr<sub>2</sub>Si<sub>2</sub>-type structure (<i>I</i>4/<i>mmm</i>), were prepared for <i>RE</i> = La, Nd, Sm, Gd, Ho, and Er. By traversing the rare earth series,
the lattice parameters of the <i>RE</i><sub>2</sub>SbO<sub>2</sub> phases are gradually reduced, thus increasing chemical pressure
on the Sb environment. As the Sb displacements are perturbed, different
charge carrier activation mechanisms dominate the transport properties
of these compounds. As a result, the electrical conductivity and Seebeck
coefficient are improved simultaneously, while the number of charge
carriers in the series remains constant
Disorder-Controlled Electrical Properties in the Ho<sub>2</sub>Sb<sub>1–<i>x</i></sub>Bi<sub><i>x</i></sub>O<sub>2</sub> Systems
High-purity bulk samples of the Ho<sub>2</sub>ÂSb<sub>1–<i>x</i></sub>ÂBi<sub><i>x</i></sub>O<sub>2</sub> phases (<i>x</i> =
0, 0.2, 0.4, 0.6, 0.8, 1.0) were prepared
and subjected to structural and elemental analysis as well as physical
property measurements. The Sb/Bi ratio in the Ho<sub>2</sub>ÂSb<sub>1–<i>x</i></sub>ÂBi<sub><i>x</i></sub>O<sub>2</sub> system could be fully traversed without disturbing
the overall <i>anti</i>-ThÂCr<sub>2</sub>Si<sub>2</sub> type structure (<i>I</i>4/<i>mmm</i>). The single-crystal
X-ray diffraction studies revealed that the local atomic displacement
on the Sb/Bi site is reduced with the increasing Bi content. Such
local structural perturbations lead to a gradual semiconductor-to-metal
transition in the bulk materials. The significant variations in the
electrical properties without a change in the charge carrier concentration
are explained within the frame of the disorder-induced Anderson localization.
These experimental observations demonstrated an alternative strategy
for electrical properties manipulations through the control of the
local atomic disorder
Refined Synthesis and Crystal Growth of Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> for Hard Radiation Detectors
The refined synthesis
and optimized crystal growth of high quality
Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> single crystals are reported.
Improved experimental procedures were implemented to reduce the oxygen
contamination and improve the stoichiometry of the single crystal
samples. The impact of oxygen contamination and the nature of the
stoichiometry deviation in the Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> system were studied by first-principles density functional theory
(DFT) electronic structure calculations as well as experimental methods.
The DFT calculations indicated that the presence of interstitial oxygen
atoms (O<sub>int</sub>) leads to the formation of a deep level located
near the middle of the gap, as well as a shallow acceptor level near
the valence band maximum. In addition, total energy calculations of
the heat of formation of Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> suggest that the region of thermodynamic stability is sufficiently
wide. By refining the preparative procedures, high quality Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> single crystal samples were reproducibly
obtained. These Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> single crystals
exhibited excellent optical transparency, electrical resistivity in
the range of 10<sup>11</sup> Ω·cm, and a significant increase
in photoconductivity. Infrared photoluminescence of the Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> single crystals was observed over the
temperature range of 15–75 K. Detectors fabricated from boules
yielded a clear spectroscopic response to both Ag Kα X-ray and <sup>57</sup>Co γ-ray radiation. The electron and hole mobility-lifetime
product (μτ) of the current Pb<sub>2</sub>P<sub>2</sub>Se<sub>6</sub> detectors were estimated to be 3.1 × 10<sup>–4</sup> and 4.8 × 10<sup>–5</sup> cm<sup>2</sup>/V, respectively