TY - JOUR
T1 - Ferroelectric Domain Wall Engineering Enables Thermal Modulation in PMN–PT Single Crystals
AU - Negi, Ankit
AU - Kim, Hwang Pill
AU - Hua, Zilong
AU - Timofeeva, Anastasia
AU - Zhang, Xuanyi
AU - Zhu, Yong
AU - Peters, Kara
AU - Kumah, Divine
AU - Jiang, Xiaoning
AU - Liu, Jun
N1 - Funding Information:
The authors would like to thank Shuang Wu from Dr. Y.Z.'s lab for the help with IR camera setup. A.N., X.Z., D.K., X.J., and J.L. acknowledge financial support from the National Science Foundation under the award No. DMR 2011978. H.K. and X.J. acknowledge that this work was supported in part by the Office of Naval Research (ONR) under Grant N00014‐21‐1‐2058. Work performed by Z.H. was supported through the INL Laboratory Directed Research& Development (LDRD) Program under DOE Idaho Operations Office Contract DE‐AC07‐05ID14517.
Publisher Copyright:
© 2023 The Authors. Advanced Materials published by Wiley-VCH GmbH.
PY - 2023/2/16
Y1 - 2023/2/16
N2 - Acting like thermal resistances, ferroelectric domain walls can be manipulated to realize dynamic modulation of thermal conductivity (k), which is essential for developing novel phononic circuits. Despite the interest, little attention has been paid to achieving room-temperature thermal modulation in bulk materials due to challenges in obtaining a high thermal conductivity switching ratio (khigh/klow), particularly in commercially viable materials. Here, room-temperature thermal modulation in 2.5 mm-thick Pb(Mg1/3Nb2/3)O3–xPbTiO3 (PMN–xPT) single crystals is demonstrated. With the use of advanced poling conditions, assisted by the systematic study on composition and orientation dependence of PMN–xPT, a range of thermal conductivity switching ratios with a maximum of ≈1.27 is observed. Simultaneous measurements of piezoelectric coefficient (d33) to characterize the poling state, domain wall density using polarized light microscopy (PLM), and birefringence change using quantitative PLM reveal that compared to the unpoled state, the domain wall density at intermediate poling states (0< d3333,max) is lower due to the enlargement in domain size. At optimized poling conditions (d33,max), the domain sizes show increased inhomogeneity that leads to enhancement in the domain wall density. This work highlights the potential of commercially available PMN–xPT single crystals among other relaxor-ferroelectrics for achieving temperature control in solid-state devices.
AB - Acting like thermal resistances, ferroelectric domain walls can be manipulated to realize dynamic modulation of thermal conductivity (k), which is essential for developing novel phononic circuits. Despite the interest, little attention has been paid to achieving room-temperature thermal modulation in bulk materials due to challenges in obtaining a high thermal conductivity switching ratio (khigh/klow), particularly in commercially viable materials. Here, room-temperature thermal modulation in 2.5 mm-thick Pb(Mg1/3Nb2/3)O3–xPbTiO3 (PMN–xPT) single crystals is demonstrated. With the use of advanced poling conditions, assisted by the systematic study on composition and orientation dependence of PMN–xPT, a range of thermal conductivity switching ratios with a maximum of ≈1.27 is observed. Simultaneous measurements of piezoelectric coefficient (d33) to characterize the poling state, domain wall density using polarized light microscopy (PLM), and birefringence change using quantitative PLM reveal that compared to the unpoled state, the domain wall density at intermediate poling states (0< d3333,max) is lower due to the enlargement in domain size. At optimized poling conditions (d33,max), the domain sizes show increased inhomogeneity that leads to enhancement in the domain wall density. This work highlights the potential of commercially available PMN–xPT single crystals among other relaxor-ferroelectrics for achieving temperature control in solid-state devices.
KW - domain walls
KW - ferroelectrics
KW - poling
KW - thermal conductivity
KW - thermal modulation
UR - http://www.scopus.com/inward/record.url?scp=85154024541&partnerID=8YFLogxK
UR - https://www.mendeley.com/catalogue/b6ae44ef-2196-380f-a6de-2ec7bc053d02/
U2 - 10.1002/adma.202211286
DO - 10.1002/adma.202211286
M3 - Article
C2 - 36796104
AN - SCOPUS:85154024541
SN - 0935-9648
VL - 35
SP - e2211286
JO - Advanced Materials
JF - Advanced Materials
IS - 22
M1 - 2211286
ER -