TY - JOUR
T1 - Thermoelectric optimization using first principles calculation and single parabolic band model
T2 - a case of Ca0.5La0.5−x Bi x MnO3 (x = 0, 0.25)
AU - Raharjo, Bambang Mulyo
AU - Kurniawan, Budhy
AU - Soegijono, Bambang
AU - Munazat, Dicky Rezky
AU - Razaq, Dhawud Sabilur
AU - Suprayoga, Edi
N1 - Publisher Copyright:
© 2024 IOP Publishing Ltd.
PY - 2024/7
Y1 - 2024/7
N2 - Conducting optimization calculations for thermoelectric performance can be beneficial in guiding the direction of further experimental work. In our study, we utilize a combination of the first principle, Boltzmann transport and restructured single parabolic band model to investigate the half-doped semiconductors based on manganite. Ca0.5La0.5−x Bi x MnO3 (x = 0, 0.25) as samples shows the power factor (PF) optimum value of 30% and 69% for x = 0 and 0.25, respectively at a temperature of 800 K. In addition, both samples show two to three orders of magnitude smaller lattice thermal conductivity than their electronic thermal conductivity. This excludes complex phononic transport mechanisms from the calculation of the figure of merit (ZT). The ZT calculations of Ca0.5L0.5MnO3 and Ca0.5L0.5−x Bi x MnO3 are corrected by the ratio of the transport relaxation time of electrical conductivity to the transport relaxation time of electronic thermal conductivity by the Lorenz number, resulting in ZT values of 0.063 and 0.327 at a temperature of 800 K, respectively.
AB - Conducting optimization calculations for thermoelectric performance can be beneficial in guiding the direction of further experimental work. In our study, we utilize a combination of the first principle, Boltzmann transport and restructured single parabolic band model to investigate the half-doped semiconductors based on manganite. Ca0.5La0.5−x Bi x MnO3 (x = 0, 0.25) as samples shows the power factor (PF) optimum value of 30% and 69% for x = 0 and 0.25, respectively at a temperature of 800 K. In addition, both samples show two to three orders of magnitude smaller lattice thermal conductivity than their electronic thermal conductivity. This excludes complex phononic transport mechanisms from the calculation of the figure of merit (ZT). The ZT calculations of Ca0.5L0.5MnO3 and Ca0.5L0.5−x Bi x MnO3 are corrected by the ratio of the transport relaxation time of electrical conductivity to the transport relaxation time of electronic thermal conductivity by the Lorenz number, resulting in ZT values of 0.063 and 0.327 at a temperature of 800 K, respectively.
KW - half doped manganite
KW - Lorenz number
KW - phonon thermal conductivity
KW - single parabolic band
KW - thermoelectric optimization
UR - http://www.scopus.com/inward/record.url?scp=85192245285&partnerID=8YFLogxK
U2 - 10.1088/1361-651X/ad3e97
DO - 10.1088/1361-651X/ad3e97
M3 - Article
AN - SCOPUS:85192245285
SN - 0965-0393
VL - 32
JO - Modelling and Simulation in Materials Science and Engineering
JF - Modelling and Simulation in Materials Science and Engineering
IS - 5
M1 - 055001
ER -