Possible Charge Density Wave and Enhancement of Thermoelectric
Properties at Mild-Temperature Range in n‑Type CuI-Doped
Bi
2
Te
2.1
Se
0.9
Compounds
Hyunyong Cho,
†
Jae Hyun Yun,
†
Jin Hee Kim,
†
Song Yi Back,
†
Ho Seong Lee,
‡
Sung Jin Kim,
§
Seokyeong Byeon,
∥
Hyungyu Jin,
∥
and Jong-Soo Rhyee*
,†
†
Department of Applied Physics and Institute of Natural Sciences, Kyung Hee University, Gyung-gi 17104, Korea
‡
School of Materials Science and Engineering, Kyungpook National University, Daegu 41566, Korea
§
Department of Chemistry and Nano Sciences, Ewha Womans University, Seoul 03760, Korea
∥
Department of Mechanical Engineering, Pohang University of Science and Technology, Pohang 37673, Korea
ABSTRACT: Bi
2
Te
3
-based compounds have long been studied as thermoelectric materials in cooling applications near room
temperature. Here, we investigated the thermoelectric properties of CuI-doped Bi
2
Te
2.1
Se
0.9
compounds. The Cu/I codoping
induces the lattice distortion partially in the matrix. We report that the charge density wave caused by the local lattice distortion
affects the electrical and thermal transport properties. From the high-temperature specific heat, we found a first-order phase
transitions near 490 and 575 K for CuI-doped compounds (CuI)
x
Bi
2
Te
2.1
Se
0.9
(x = 0.3 and 0.6%), respectively. It is not a
structural phase transition, confirming from the high-temperature X-ray diffraction. The temperature-dependent electrical
resistivity shows a typical behavior of charge density wave transition, which is consistent with the temperature-dependent
Seebeck coefficient and thermal conductivity. The transmission electron microscopy and electron diffraction show a local lattice
distortion, driven by the charge density wave transition. The charge density wave formation in the Bi
2
Te
3
-based compounds are
exceptional because of the possibility of coexistence of charge density wave and topological surface states. From the Kubo
formula and Boltzmann transport calculations, the formation of charge density wave enhances the power factor. The lattice
modulation and charge density wave decrease lattice thermal conductivity, resulting in the enhancement of thermoelectric
performance simultaneously in CuI-doped samples. Consequently, an enhancement of thermoelectric performance ZT over 1.0
is achieved at 448 K in the (CuI)
0.003
Bi
2
Te
2.1
Se
0.9
sample. The enhancement of ZT at high temperature gives rise to a superior
average ZT
avg
(1.0) value than those of previously reported ones.
KEYWORDS: Bi
2
Te
3
, codoping, thermoelectric, charge density wave, lattice modulation, phase transition
1. INTRODUCTION
Thermoelectric (TE) materials that can directly exchange heat
and electricity and vice versa are widely used in various devices
such as heat generators and thermoelectric coolers. The
performance of TE materials is characterized by the
dimensionless figure of merit ZT, defined as ZT = S
2
σT/(κ
lat
+ κ
el
), where S, σ, κ
lat
, κ
el
, and T are Seebeck coefficient,
electrical conductivity, lattice thermal conductivity, electronic
thermal conductivity, and absolute temperature, respectively.
1,2
When the thermoelectric materials have good performance, it
can be used in various devices such as alternative energy-saving
systems and solid-state cooling. Generally, more than 60% of
the primary energy in the industry is lost to waste heat, and
much of the waste heat is in the low-temperature region near
100−300 °C. Therefore, there have been much efforts to
increase thermoelectric performance at the low-mid temper-
ature range up to 300 °C.
3−7
Typically, Bi
2
Te
3
-based materials
are well-known for their excellent TE material near room
Received: October 28, 2019
Accepted: December 18, 2019
Published: December 18, 2019
Research Article
www.acsami.org
Cite This: ACS Appl. Mater. Interfaces 2020, 12, 925-933
© 2019 American Chemical Society 925 DOI: 10.1021/acsami.9b19398
ACS Appl. Mater. Interfaces 2020, 12, 925−933
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