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中国物理学会期刊

III-V族硼基化合物半导体反常热导率机理

CSTR: 32037.14.aps.70.20210797

Origin of abnormal thermal conductivity in group III-V boron compound semiconductors

CSTR: 32037.14.aps.70.20210797
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  • 采用基于玻尔兹曼输运方程的第一性原理计算方法深入研究了硼基III-V化合物的热导率性质, 与IV族和III-V族半导体进行对比, 发现砷化硼的高热导率主要来源于硼基III-V化合物中声学支和光学支之间存在一个很大的频率带隙, 导致两个声学声子的能量要小于一个光学声子的能量, 无法满足三声子散射的能量守恒要求, 严重遏制了三声子散射几率. 金刚石的高热导率主要来自其拥有极大的声学声子群速度. 磷化硼虽然也拥有较大的声学声子群速度, 但是其频率带隙比较小, 无法有效遏制三声子散射, 所以磷化硼的热导率小于砷化硼; 尽管锑化硼的频率带隙与砷化硼相当, 但是由于其拥有较小的声学声子群速度和较大的耦合矩阵元, 导致锑化硼的热导率低于砷化硼. 该研究为设计高热导率半导体材料提供了新的认识.

     

    Over the past half-century, according to Moore’s law, the sizes of transistors continue shrinking, and the integrated circuits have approached to their physical limits, which puts forward higher requirements for the thermal dissipation capacity of material. Revealing the physical mechanisms of heat conduction in semiconductors is important for thermal managements of devices. Experimentally, it was found that boron arsenide has a very high thermal conductivity compared with diamond, and boron arsenide has lattice constant close to silicon’s lattice constant, which can be heterogeneously integrated into silicon to solve the thermal management problem. However, group III-V boron compounds show abnormal thermal conductivities: the thermal conductivity of boron arsenide is significantly higher than that of boron phosphide and boron antimonide. Here, we use the first-principles calculation and the Boltzmann transport equation to study the thermal conductivity properties of the group III-V boron compounds. Comparison between the IV and III-V semiconductors shows that the high thermal conductivity of boron arsenide is due mainly to the existence of a large frequency gap between the acoustic and the optical branches. The energy sum of two acoustic phonons is less than energy of one optical phonon, which cannot meet the energy conservation requirements of three-phonon scattering, and then seriously restrict the probability of scattering of three phonons. The high thermal conductivity of diamond is due mainly to its great acoustic phonon group velocity. Although the boron phosphide also has a relatively large acoustic phonon group velocity, the frequency gap is relatively small, which cannot effectively suppress the three-phonon scattering, so the thermal conductivity of boron phosphide is less than that of boron arsenide. Although the frequency gap of boron antimonide is similar to that of boron arsenide, the thermal conductivity of boron antimonide is lower than that of boron arsenide due to its smaller acoustic phonon group velocity and larger coupling matrix element. The research provides a new insight into the design of semiconductor materials with high thermal conductivities.

     

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