30 research outputs found
Defect Chemistry and Doping of Lead Phosphate Oxo Apatite Pb<sub>10</sub>(PO<sub>4</sub>)<sub>6</sub>O
Lead phosphate oxo apatite Pb10(PO4)6O is claimed to host room-temperature superconductivity
when
doped with copper. However, unsuccessful attempts to reproduce this
claim have raised many questions about the composition, off-stoichiometry,
and copper doping itself, which are related to native defect chemistry.
We perform first-principles defect calculations to provide much needed
insights into the defect chemistry and doping of Pb10(PO4)6O. We find that Fermi energy pinning in the midgap
region occurs due to Pb and O vacancies. Our calculations also suggest
the plausible existence of closely related off-stoichiometric phase(s);
we predict one such phase. We predict only moderate levels of Cu doping,
which calls into question the experimental claim of 10% incorporation
on the Pb sites. Cu substitution on the Pb(1) and Pb(2) Wyckoff sites
is possible, resulting in Cu d9 and d10 electronic configurations, respectively.
We predict unintentional S incorporation is highly possible. Our findings
emphasize the need for careful characterization of the parent composition
and the identification of synthesis conditions that will maximize
(minimize) intentional (unintentional) doping
Synthesis, Structural Characterization, and Physical Properties of the Type‑I Clathrates <i>A</i><sub>8</sub>Zn<sub>18</sub>As<sub>28</sub> (<i>A</i> = K, Rb, Cs) and Cs<sub>8</sub>Cd<sub>18</sub>As<sub>28</sub>
The first arsenide clathrates <i>A</i><sub>8</sub>Zn<sub>18</sub>As<sub>28</sub> (<i>A</i> = K, Rb,
Cs) and Cs<sub>8</sub>Cd<sub>18</sub>As<sub>28</sub> have been synthesized
in high
yields via a two-step route. These compounds adopt the type-I structure
and exhibit structural characteristics different from the recently
reported antimonide clathrates Cs<sub>8</sub>Zn<sub>18</sub>Sb<sub>28</sub> and Cs<sub>8</sub>Cd<sub>18</sub>Sb<sub>28</sub>. In arsenide
clathrates, Zn (or Cd) and As atoms are statistically mixed at the
three framework sites: 6<i>c</i>, 16<i>i</i>,
and 24<i>k</i>; the alkali metals reside inside the cages
at the 2<i>a</i> and 6<i>d</i> sites, with the
2<i>a</i> site being only partially filled. Single-crystal
X-ray diffraction studies confirm that the Cd atoms preferably occupy
the 6<i>c</i> and 24<i>k</i> sites over the 16<i>i</i> site, with more than 80% of Cd found at the former two
positions. A unique structural feature is a framework disorder coupled
with the partial occupancy of the cage’s 2<i>a</i> site. Optical absorption measurements and electronic property measurements
reveal a semimetallic-like behavior for Cs<sub>8</sub>Cd<sub>18</sub>As<sub>28</sub> and semiconductor-like behavior for <i>A</i><sub>8</sub>Zn<sub>18</sub>As<sub>28</sub> (<i>A</i> =
Rb, Cs)
Effect of Isovalent Substitution on the Thermoelectric Properties of the Cu<sub>2</sub>ZnGeSe<sub>4–<i>x</i></sub>S<sub><i>x</i></sub> Series of Solid Solutions
Knowledge
of structure–property relationships is a key feature
of materials design. The control of thermal transport has proven to
be crucial for the optimization of thermoelectric materials. We report
the synthesis, chemical characterization, thermoelectric transport
properties, and thermal transport calculations of the complete solid
solution series Cu<sub>2</sub>ZnGeSe<sub>4–<i>x</i></sub>S<sub><i>x</i></sub> (<i>x</i> = 0–4).
Throughout the substitution series a continuous Vegard-like behavior
of the lattice parameters, bond distances, optical band gap energies,
and sound velocities are found, which enables the tuning of these
properties adjusting the initial composition. Refinements of the special
chalcogen positions revealed a change in bonding angles, resulting
in crystallographic strain possibly affecting transport properties.
Thermal transport measurements showed a reduction in the room-temperature
thermal conductivity of 42% triggered by the introduced disorder.
Thermal transport calculations of mass and strain contrast revealed
that 34% of the reduction in thermal conductivity is due to the mass
contrast only and 8% is due to crystallographic strain
A Chemical Understanding of the Band Convergence in Thermoelectric CoSb<sub>3</sub> Skutterudites: Influence of Electron Population, Local Thermal Expansion, and Bonding Interactions
N-Type
skutterudites, such as Yb<sub><i>x</i></sub>Co<sub>4</sub>Sb<sub>12</sub>, have recently been shown to exhibit high
valley degeneracy with possible band convergence, explaining the excellent
thermoelectric efficiency of these materials. Using a combined theoretical
and experimental approach involving temperature-dependent synchrotron
diffraction, molecular orbital diagrams, and computational studies,
the chemical nature of critical features in the band structure is
highlighted. We identify how n-type doping on the filler site induces
structural changes that are observed in both the diffraction data
and computational results. Additionally, we show how chemical n-type
doping slightly alters the electronic band structure, moving the high-valley
degeneracy secondary conduction band closer to the primary conduction
band and thus inducing band convergence
Synthesis, Structural Characterization, and Physical Properties of the Type‑I Clathrates <i>A</i><sub>8</sub>Zn<sub>18</sub>As<sub>28</sub> (<i>A</i> = K, Rb, Cs) and Cs<sub>8</sub>Cd<sub>18</sub>As<sub>28</sub>
The first arsenide clathrates <i>A</i><sub>8</sub>Zn<sub>18</sub>As<sub>28</sub> (<i>A</i> = K, Rb,
Cs) and Cs<sub>8</sub>Cd<sub>18</sub>As<sub>28</sub> have been synthesized
in high
yields via a two-step route. These compounds adopt the type-I structure
and exhibit structural characteristics different from the recently
reported antimonide clathrates Cs<sub>8</sub>Zn<sub>18</sub>Sb<sub>28</sub> and Cs<sub>8</sub>Cd<sub>18</sub>Sb<sub>28</sub>. In arsenide
clathrates, Zn (or Cd) and As atoms are statistically mixed at the
three framework sites: 6<i>c</i>, 16<i>i</i>,
and 24<i>k</i>; the alkali metals reside inside the cages
at the 2<i>a</i> and 6<i>d</i> sites, with the
2<i>a</i> site being only partially filled. Single-crystal
X-ray diffraction studies confirm that the Cd atoms preferably occupy
the 6<i>c</i> and 24<i>k</i> sites over the 16<i>i</i> site, with more than 80% of Cd found at the former two
positions. A unique structural feature is a framework disorder coupled
with the partial occupancy of the cage’s 2<i>a</i> site. Optical absorption measurements and electronic property measurements
reveal a semimetallic-like behavior for Cs<sub>8</sub>Cd<sub>18</sub>As<sub>28</sub> and semiconductor-like behavior for <i>A</i><sub>8</sub>Zn<sub>18</sub>As<sub>28</sub> (<i>A</i> =
Rb, Cs)
A Chemical Understanding of the Band Convergence in Thermoelectric CoSb<sub>3</sub> Skutterudites: Influence of Electron Population, Local Thermal Expansion, and Bonding Interactions
N-Type
skutterudites, such as Yb<sub><i>x</i></sub>Co<sub>4</sub>Sb<sub>12</sub>, have recently been shown to exhibit high
valley degeneracy with possible band convergence, explaining the excellent
thermoelectric efficiency of these materials. Using a combined theoretical
and experimental approach involving temperature-dependent synchrotron
diffraction, molecular orbital diagrams, and computational studies,
the chemical nature of critical features in the band structure is
highlighted. We identify how n-type doping on the filler site induces
structural changes that are observed in both the diffraction data
and computational results. Additionally, we show how chemical n-type
doping slightly alters the electronic band structure, moving the high-valley
degeneracy secondary conduction band closer to the primary conduction
band and thus inducing band convergence
Les droits de l'homme et la Convention du 28 juillet 1951 relative au Statut des réfugiés.
Controlling
extrinsic defects to tune the carrier concentration
of electrons or holes is a crucial point with regard to the engineering
application of thermoelectric semiconductors. To understand the defect-controlled
electronic structure in thermoelectric materials, we apply density
functional theory (DFT) to investigate the defect chemistry of dopants
M (M = O, S, Se, or Te) in CoSb<sub>3</sub>. DFT predicts that the
breakage of Sb<sub>4</sub> rings induced by these dopants produces
the unexpected (n- or p-type) conductivity behavior in CoSb<sub>3</sub>. For example, energetically dominant O interstitials (O<sub>i</sub>) chemically break Sb<sub>4</sub> rings and form O–4Sb five-membered
rings, leading to the charge neutral behavior of O<sub>i</sub>. While
S interstitials (S<sub>i</sub>) collapse Te–3Sb four-membered
rings within Te doped CoSb<sub>3</sub> leading to p-type conduction
behavior, Se substitution on Sb (Se<sub>Sb</sub>) breaks the Se–Te–2Sb
four-membered ring, resulting in a charge neutral behavior of the
Se<sub>Sb</sub>+Te<sub>Sb</sub> complex defect. Furthermore, the solubility
limits of M dopants (M = S, Se, or Te) are also calculated to provide
essential information about single-phase material design. This study
provides new insight into understanding the complicated chemical structure
in doped CoSb<sub>3</sub>, which is beneficial for devising effective
doping strategies for the development of high-performance bulk thermoelectric
materials
Brittle Failure Mechanism in Thermoelectric Skutterudite CoSb<sub>3</sub>
Skutterudites
based on CoSb<sub>3</sub> have high thermoelectric efficiency, but
the low fracture strength is a serious consideration for commercial
applications. To understand the origin of the brittleness in CoSb<sub>3</sub>, we examine the response along various shear and tensile
deformations using density functional theory. We find that the Co–Sb
bond dominates the ideal strength. Among all the shear and tensile
deformation paths, shearing along the (001)/⟨100⟩ slip
system has the lowest ideal strength, indicating it is the most likely
slip system to be activated under pressure. We also find that, because
the Sb–Sb covalent bond is softer than the Co–Sb bond,
the Sb-rings are less rigid than the Co–Sb frameworks, which
leads to the Sb-rings softening before the Co–Sb frameworks.
Further deformation leads to deconstruction of Sb-rings and collapse
of Co–Sb frameworks, resulting in structural failure. Moreover,
we find that filling of the CoSb<sub>3</sub> void spaces with such
typical fillers as Na, Ba, or Yb has little effect on the ideal strength
and failure mode, which can be understood because they have little
effect on the Sb-rings
<i>n</i>‑Type Bi<sub>2</sub>Te<sub>3–<i>x</i></sub>Se<sub><i>x</i></sub> Nanoplates with Enhanced Thermoelectric Efficiency Driven by Wide-Frequency Phonon Scatterings and Synergistic Carrier Scatterings
Driven
by the prospective applications of thermoelectric materials, massive
efforts have been dedicated to enhancing the conversion efficiency.
The latter is governed by the figure of merit (<i>ZT</i>), which is proportional to the power factor (<i>S</i><sup>2</sup>σ) and inversely proportional to the thermal conductivity
(κ). Here, we demonstrate the synthesis of high-quality ternary
Bi<sub>2</sub>Te<sub>3–<i>x</i></sub>Se<sub><i>x</i></sub> nanoplates using a microwave-assisted surfactant-free
solvothermal method. The obtained <i>n</i>-type Bi<sub>2</sub>Te<sub>2.7</sub>Se<sub>0.3</sub> nanostructures exhibit a high <i>ZT</i> of 1.23 at 480 K measured from the corresponding sintered
pellets, in which a remarkably low κ and a shift of peak <i>S</i><sup>2</sup>σ to high temperature are observed. By
detailed electron microscopy investigations, coupled with theoretical
analysis on phonon transports, we propose that the achieved κ
reduction is attributed to the strong wide-frequency phonon scatterings.
The shifting of peak <i>S</i><sup>2</sup>σ to high
temperature is due to the weakened temperature dependent transport
properties governed by the synergistic carrier scatterings and the
suppressed bipolar effects by enlarging the band gap
Grain Boundaries Softening Thermoelectric Oxide BiCuSeO
Engineering
grain boundaries (GBs) are effective in tuning the
thermoelectric (TE) properties of TE materials, but the role of GB
on mechanical properties, which is important for their commercial
applications, remains unexplored. In this paper, we apply ab initio
method to examine the ideal shear strength and failure mechanism of
GBs in TE oxide BiCuSeO. We find that the ideal shear strength of
the GB is much lower than that of the ideal single crystal. The atomic
rearrangements accommodating the lattice and neighbor structure mismatch
between different grains leads to the much weaker GB stiffness compared
with grains. Failure of the GBs arises from either the distortion
of the Cu–Se layers or the relative slip between Bi–O
and Cu–Se layers. This work is crucial to illustrate the deformation
of GBs, laying the basis for the development and design of mechanically
robust polycrystalline TE materials