Modulated thermal transport for flexural and in-plane phonons in double-stub graphene nanoribbons<xref rid="cpb_27_8_088101fn1" ref-type="fn">*</xref><fn id="cpb_27_8_088101fn1"><label>*</label><p>Project supported by the Science Funds from the Educational Bureau of Hunan Province, China (Grant No. 16C0468), the China Postdoctoral Science Foundation (Grant No. 2016M602421), the Science and Technology Plan of Hunan Province, China (Grant No. 2015RS4002), and the Natural Science Foundation of Hunan Province, China (Grant No. 2015JJ2050).</p></fn>

Modulated thermal transport for flexural and in-plane phonons in double-stub graphene nanoribbons**

Project supported by the Science Funds from the Educational Bureau of Hunan Province, China (Grant No. 16C0468), the China Postdoctoral Science Foundation (Grant No. 2016M602421), the Science and Technology Plan of Hunan Province, China (Grant No. 2015RS4002), and the Natural Science Foundation of Hunan Province, China (Grant No. 2015JJ2050).

Pan Chang-Ning^{1, 2}, Long Meng-Qiu^{1, †}, He Jun¹

(color online) Phonon transmission functions for (a) the straight 6-ZGNR; (b) double-stub GNR N_z = 6, N_c = 2, N_L = 6, and M = 4; (c) N_z = 6, N_c = 6, N_L = 6, and M = 4; and (d) N_z = 6, N_c = 6, N_L = 13, and M = 4. The solid, dashed, and dotted curves correspond to the total transmission rate, the transmission rate of IPMs, and the transmission rate of FPMs, respectively.