Lu Baojie, Wang Binghao, Chen Yao, Facchetti Antonio, Marks Tobin J, Balogun Oluwaseyi
Department of Mechanical Engineering, Northwestern University, 2145 Sheridan Road, Evanston, Illinois 60208, United States.
Department of Chemistry, Northwestern University, 2145 Sheridan Road, Evanston, Illinois 60208, United States.
ACS Appl Mater Interfaces. 2020 Aug 5;12(31):34901-34909. doi: 10.1021/acsami.0c08117. Epub 2020 Jul 22.
Self-assembled nanodielectrics (SANDs) consist of alternating layers of polarized phosphonate-functionalized azastibazolium π-electron (PAE) and high- dielectric metal oxide (ZrO or HfO) films. SANDs are desirable gate dielectrics materials for thin-film transistor applications because of their excellent properties such as low-temperature fabrication, large dielectric strength, and large capacitance. In this paper, we investigate the cross-plane thermal boundary conductance of SANDs using the frequency domain thermoreflectance (FDTR) technique. First, we characterize the thermal conductance of PAE self-assembled monolayers (SAMs), inverted-PAE (IPAE) SAMs, and mixed PAE-IPAE SAMs, sandwiched between thin gold and silica (SiO) films at the top and bottom surfaces. Next, we quantify the thermal conductance of SAND- with different numbers () of PAE-ZrO layers and thicknesses ranging between 4.7 and 11.3 nm. From the FDTR measurements, we observe that the thermal boundary conductance of the SAMs can be tuned between 42.1 ± 4.6 MW/(m K) and 52.4 ± 2.5 MW/(m K), based on the relative density of the PAE and IPAE chromophores. In the SAND- samples, we observe a monotonic decrease in the thermal conductance with increasing . We use the measured thermal conductance data in a series resistance model to estimate a thermal interface conductance of 695 MW/(m K) for the contact between the PAE chromophore and the zirconium dioxide films, which is an order of magnitude larger than the SAMs. We attribute the improved thermal conductance to stronger adhesion between the PAE chromophore and the zirconium dioxide films, as compared to the weakly bonded SAMs to the gold and silicon dioxide films.
自组装纳米电介质(SANDs)由极化的膦酸酯功能化氮杂锑唑鎓π电子(PAE)和高介电常数金属氧化物(ZrO或HfO)薄膜的交替层组成。由于SANDs具有诸如低温制造、高介电强度和大电容等优异性能,它们是薄膜晶体管应用中理想的栅极电介质材料。在本文中,我们使用频域热反射(FDTR)技术研究了SANDs的跨平面热边界电导。首先,我们表征了夹在顶部和底部的薄金和二氧化硅(SiO)薄膜之间的PAE自组装单分子层(SAMs)、反式PAE(IPAE)SAMs以及混合PAE - IPAE SAMs的热导率。接下来,我们量化了具有不同PAE - ZrO层数()且厚度在4.7至11.3 nm之间的SANDs的热导率。通过FDTR测量,我们观察到基于PAE和IPAE发色团的相对密度,SAMs的热边界电导可在42.1±4.6 MW/(m²K)和52.4±2.5 MW/(m²K)之间调节。在SAND - 样品中,我们观察到热导率随增加而单调下降。我们在串联电阻模型中使用测量的热导率数据来估计PAE发色团与二氧化锆薄膜之间接触的热界面电导为695 MW/(m²K),这比SAMs大一个数量级。与弱键合的SAMs与金和二氧化硅薄膜相比,我们将热导率的提高归因于PAE发色团与二氧化锆薄膜之间更强的附着力。