Seongho Choi

Seongho Choi

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Seongho Choi

Toyota Technological Institute, 2-12-1, Hisakata, Tempaku-ku, Nagoya, Aichi 468-8511, Japan

Research Focus & Metrics

Academic Career Length

17Years (2010-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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8 January 2019 in Nature Communications
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Journal Article
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DBDogyun Byeon
Dogyun Byeon
RSRobert Sobota
Robert Sobota
KDKévin Delime-Codrin
Kévin Delime-Codrin
SCSeongho Choi
Seongho Choi
KHKeisuke Hirata
Keisuke Hirata
TTTsunehiro Takeuchi
Tsunehiro Takeuchi
Both electrical conductivity σ and Seebeck coefficient S are functions of carrier concentration being correlated with each other, and the value of power factor S2σ is generally limited to less than 0.01 W m−1 K−2. Here we report that, under the temperature gradient applied simultaneously to both parallel and perpendicular directions of measurement, a metallic copper selenide, Cu2Se, shows two sign reversals and colossal values of S exceeding ±2 mV K−1 in a narrow temperature range, 340 K < T < 400 K, where a structure phase transition takes place. The metallic behavior of σ possessing larger magnitude exceeding 600 S cm−1 leads to a colossal value of S2σ = 2.3 W m–1 K–2. The small thermal conductivity less than 2 W m−1 K−1 results in a huge dimensionless figure of merit exceeding 400. This unusual behavior is brought about by the self-tuning carrier concentration effect in the low-temperature phase assisted by the high-temperature phase.

1 February 2010 in Materials Letters
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HJHye-Mi Ju
Hye-Mi Ju
SHSeung Hun Huh
Seung Hun Huh
SCSeong-Ho Choi
Seong-Ho Choi
HLHong-Lim Lee
Hong-Lim Lee

27 November 2018 in ACS Applied Materials & Interfaces
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ANAmi Nomura
Ami Nomura
SCSeongho Choi
Seongho Choi
MIManabu Ishimaru
Manabu Ishimaru
AKAtsuko Kosuga
Atsuko Kosuga
TCThomas Chasapis
Thomas Chasapis
KKKen Kurosaki
Ken Kurosaki

1 April 2019 in Journal of Alloys and Compounds
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Journal Article
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RFRiccardo Freccero
Riccardo Freccero
SCS.H. Choi
S.H. Choi
PSP. Solokha
P. Solokha
SNSerena De Negri
Serena De Negri
TTT. Takeuchi
T. Takeuchi
ASA. Saccone
A. Saccone

1 December 2016 in AIP Advances
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Journal Article
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SCSeongho Choi
Seongho Choi
KKKen Kurosaki
Ken Kurosaki
GLGuanghe Li
Guanghe Li
YOYuji Ohishi
Yuji Ohishi
HMHiroaki Muta
Hiroaki Muta
SMSatoshi Maeshima
Satoshi Maeshima
Skutterudite compounds such as Co antimonite (CoSb3) contain cage-like voids inside crystal structure, which can be completely or partially filled with various different atoms, including group 13 elements. The multiple filling approach is known as an effective way of reducing lattice thermal conductivity (κlat), which results in a high value of the thermoelectric dimensionless figure of merit (zT). In this work, enhanced zT was achieved for the Ga and In co-added CoSb3 samples with a preferable microstructure and the nominal composition (Ga0.8In0.2)xCo4Sb12 (x = 0.05−0.45). Although all added In atoms occupied exclusively the void sites, the Ga species filled both the void and Sb sites of CoSb3. Moreover, Ga atoms added in the quantities exceeding the solubility limit precipitated as GaSb nanoparticles. The sample with x = 0.45 was characterized by the largest filling factions of Ga and In as well as the unique microstructure, consisting of microscale grains of the skutterudite phase and corresponding amounts of the GaSb nanoparticles. The Ga and In co-added skutterudite samples with optimized chemical composition and microstructure maintained high carrier mobility and sufficiently low κlat values, resulting in zT > 1.1, one of the best values for the skutterudites filled with group 13 elements.

1 February 2014 in Journal of the Korean Physical Society
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SHSeung Hun Huh
Seung Hun Huh
SCSeong-Ho Choi
Seong-Ho Choi
HJHae-Mi Ju
Hae-Mi Ju
DKDha-Hae Kim
Dha-Hae Kim
The properties of the interlayer thermal expansion of 6-layered reduced graphene oxide (rGO) were investigated by using X-ray diffraction (XRD). The interlayer distance of rGO increases linearly as the temperature increases from room temperature to 1300 K. This linear pattern is similar to that of graphite. However, the degree of interlayer thermal expansion of rGO is 22% higher than that of graphite in the temperature range from 288–300 to 1073 K, which is explained by the weak interlayer interaction of 6-layered rGO.