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Distinguishing Optical and Acoustic Phonon Temperatures and Their Energy Coupling Factor under Photon Excitation in nm 2D Materials

机译:nm 2D材料中光子激发下的光声声子温度及其能量耦合因子的判别

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摘要

Under photon excitation, 2D materials experience cascading energy transfer from electrons to optical phonons (OPs) and acoustic phonons (APs). Despite few modeling works, it remains a long‐history open problem to distinguish the OP and AP temperatures, not to mention characterizing their energy coupling factor ( ). Here, the temperatures of longitudinal/transverse optical (LO/TO) phonons, flexural optical (ZO) phonons, and APs are distinguished by constructing steady and nanosecond (ns) interphonon branch energy transport states and simultaneously probing them using nanosecond energy transport state‐resolved Raman spectroscopy. Δ is measured to take more than 30% of the Raman‐probed temperature rise. A breakthrough is made on measuring the intrinsic in‐plane thermal conductivity of suspended nm MoS and MoSe by completely excluding the interphonon cascading energy transfer effect, rewriting the Raman‐based thermal conductivity measurement of 2D materials. for MoS , MoSe , and graphene paper (GP) are characterized. For MoS and MoSe , is in the order of 10 and 10 W m K and is much smaller than . Under ns laser excitation, is significantly increased, probably due to the reduced phonon scattering time by the significantly increased hot carrier population. For GP, is 0.549 × 10 W m K , agreeing well with the value of 0.41 × 10 W m K by first‐principles modeling.
机译:在光子激发下,二维材料会经历从电子到光子(OP)和声子(AP)的级联能量转移。尽管建模工作很少,但区分OP和AP温度,更不用说表征其能量耦合因子()仍然是一个历史悠久的问题。在这里,纵向/横向光学(LO / TO)声子,弯曲光学(ZO)声子和AP的温度通过构造稳定和纳秒(ns)对声子分支能量传输态并同时使用纳秒能量传输态进行探测来区分-解析拉曼光谱。 Δ 据测量,拉曼温度测量值占拉曼探测温度上升的30%以上。通过完全消除对声子级联能量转移效应,重写基于二维材料的拉曼热导率测量,在测量悬浮的纳米MoS和MoSe的固有面内热导率方面取得了突破。 对于MoS来说,MoSe和石墨烯纸(GP)的特征是。对于MoS和MoSe, 约为10和10 W m K, 比 。在ns激光激发下 显着增加,可能是由于显着增加的热载流子数量减少了声子散射时间。对于GP, 为0.549×10 W m K,通过第一原理建模与0.41×10 W m K的值非常吻合。

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