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  • Soft and Self‐Adhesive Ther...
    Yan, Qingwei; Alam, Fakhr E.; Gao, Jingyao; Dai, Wen; Tan, Xue; Lv, Le; Wang, Junjie; Zhang, Huan; Chen, Ding; Nishimura, Kazuhito; Wang, Liping; Yu, Jinhong; Lu, Jibao; Sun, Rong; Xiang, Rong; Maruyama, Shigeo; Zhang, Hang; Wu, Sudong; Jiang, Nan; Lin, Cheng‐Te

    Advanced functional materials, 09/2021, Volume: 31, Issue: 36
    Journal Article

    Urged by the increasing power and packing densities of integrated circuits and electronic devices, efficient dissipation of excess heat from hot spot to heat sink through thermal interface materials (TIMs) is a growing demand to maintain system reliability and performance. In recent years, graphene‐based TIMs received considerable interest due to the ultrahigh intrinsic thermal conductivity of graphene. However, the cooling efficiency of such TIMs is still limited by some technical difficulties, such as production‐induced defects of graphene, poor alignment of graphene in the matrix, and strong phonon scattering at graphene/graphene or graphene/matrix interfaces. In this study, a 120 µm‐thick freestanding film composed of vertically aligned, covalently bonded graphene nanowalls (GNWs) is grown by mesoplasma chemical vapor deposition. After filling GNWs with silicone, the fabricated adhesive TIMs exhibit a high through‐plane thermal conductivity of 20.4 W m−1 K−1 at a low graphene loading of 5.6 wt%. In the TIM performance test, the cooling efficiency of GNW‐based TIMs is ≈1.5 times higher than that of state‐of‐the‐art commercial TIMs. The TIMs achieve the desired balance between high through‐plane thermal conductivity and small bond line thickness, providing superior cooling performance for suppressing the degradation of luminous properties of high‐power light‐emitting diode chips. Graphene nanowalls, composed of high‐quality, vertically aligned, and covalently bonded graphene frameworks, exhibit excellent ability to improve the thermal conductivity of polymer‐based thermal interface materials. The resulting composites show a through‐plane thermal conductivity of 20.4 W m−1 K−1 at a filler content of 5.6 wt%, resulting in ≈1.5 times higher cooling efficiency compared to that of a commercial thermal pad.