TY - JOUR
T1 - Enhanced Thermoelectric Performance of As-Grown Suspended Graphene Nanoribbons
AU - Li, Qin Yi
AU - Feng, Tianli
AU - Okita, Wakana
AU - Komori, Yohei
AU - Suzuki, Hiroo
AU - Kato, Toshiaki
AU - Kaneko, Toshiro
AU - Ikuta, Tatsuya
AU - Ruan, Xiulin
AU - Takahashi, Koji
N1 - Funding Information:
This work was partially supported by JSPS KAKENHI (Grant Nos. JP18K13704, JP19H00664, JP17H03186), JST-PRESTO (Grant No. J170002074), JSPS A3 Foresight Program (“2D Materials and van der Waals Heterostructures”), the Cooperative Research Project Program of the Research Institute of Electrical Communication, Tohoku University, and JST CREST Grant No. JPMJCR18I1, Japan. X.L.R. acknowledges the partial support from the Defense Advanced Research Projects Agency (DARPA) of the United States (Award No. HR0011-15-2-0037).
Funding Information:
This work was partially supported by JSPS KAKENHI (Grant Nos. JP18K13704, JP19H00664, JP17H03186), JST-PRESTO (Grant No. J170002074), JSPS A3 Foresight Program ("2D Materials and Van Der Waals Heterostructures??), the Cooperative Research Project Program of the Research Institute of Electrical Communication Tohoku University, and JST CREST Grant No. JPMJCR18I1, Japan. X.L.R. acknowledges the partial support from the Defense Advanced Research Projects Agency (DARPA) of the United States (Award No. HR0011-15-2-0037).
PY - 2019/8/27
Y1 - 2019/8/27
N2 - Conventionally, graphene is a poor thermoelectric material with a low figure of merit (ZT) of 10-4-10-3. Although nanostructuring was proposed to improve the thermoelectric performance of graphene, little experimental progress has been accomplished. Here, we carefully fabricated as-grown suspended graphene nanoribbons with quarter-micron length and â40 nm width. The ratio of electrical to thermal conductivity was enhanced by 1-2 orders of magnitude, and the Seebeck coefficient was several times larger than bulk graphene, which yielded record-high ZT values up to â0.1. Moreover, we observed a record-high electronic contribution of â20% to the total thermal conductivity in the nanoribbon. Concurrent phonon Boltzmann transport simulations reveal that the reduction of lattice thermal conductivity is mainly attributed to quasi-ballistic phonon transport. The record-high ratio of electrical to thermal conductivity was enabled by the disparate electron and phonon mean free paths as well as the clean samples, and the enhanced Seebeck coefficient was attributed to the band gap opening. Our work not only demonstrates that electron and phonon transport can be fundamentally tuned and decoupled in graphene but also indicates that graphene with appropriate nanostructures can be very promising thermoelectric materials.
AB - Conventionally, graphene is a poor thermoelectric material with a low figure of merit (ZT) of 10-4-10-3. Although nanostructuring was proposed to improve the thermoelectric performance of graphene, little experimental progress has been accomplished. Here, we carefully fabricated as-grown suspended graphene nanoribbons with quarter-micron length and â40 nm width. The ratio of electrical to thermal conductivity was enhanced by 1-2 orders of magnitude, and the Seebeck coefficient was several times larger than bulk graphene, which yielded record-high ZT values up to â0.1. Moreover, we observed a record-high electronic contribution of â20% to the total thermal conductivity in the nanoribbon. Concurrent phonon Boltzmann transport simulations reveal that the reduction of lattice thermal conductivity is mainly attributed to quasi-ballistic phonon transport. The record-high ratio of electrical to thermal conductivity was enabled by the disparate electron and phonon mean free paths as well as the clean samples, and the enhanced Seebeck coefficient was attributed to the band gap opening. Our work not only demonstrates that electron and phonon transport can be fundamentally tuned and decoupled in graphene but also indicates that graphene with appropriate nanostructures can be very promising thermoelectric materials.
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U2 - 10.1021/acsnano.9b03521
DO - 10.1021/acsnano.9b03521
M3 - Article
C2 - 31411858
AN - SCOPUS:85071669363
SN - 1936-0851
VL - 13
SP - 9182
EP - 9189
JO - ACS nano
JF - ACS nano
IS - 8
ER -