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正弦色散对一维声学激子能量的影响
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作者 陈国应 《东北师大学报(自然科学版)》 CAS CSCD 1996年第1期29-32,共4页
采用顾世洧处理体内激子方法,把Wilson提出的一维极化子哈密顿量推广到一维激子,并考虑了声子的色散效应.运用微扰法计算正弦色散时一维声学激子基态能,与无色散时一维声学激子,极化子做了比较.
关键词 激子 哈密顿量 正弦色散 晶体 声学激子
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正弦色散对表面声学激子能量的影响
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作者 陈国应 安宏 《大连大学学报》 1999年第4期33-36,70,共5页
本文从Sak[1]提出的表面极化子的哈密顿量出发,采用顾世洧教授[2]所用的方法,考虑到色散效应对表面激子的影响。
关键词 正弦色散 表面声学激子 微扰法 表面极化子 激子能量
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抛物线色散时表面声学激子能量
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作者 陈国应 李渴望 《沈阳航空工业学院学报》 1995年第4期6-9,共4页
本文从sak提出的表面极化子的哈密顿量出发,采用顾世洧教授所用的方法,考虑到色散效应对表面激子的影响,用微扰法计算正弦色散时对表面激子能量的影响及表面声学激子和表面极化子间关系。
关键词 表面激子 哈密顿量 声学激子 色散
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二维非极性晶体中声学激子的性质
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作者 肖景林 《河北师范大学学报(自然科学版)》 CAS 1990年第3期31-36,共6页
本文研究了二维非极性晶体中通过形变势与声学声子强、弱耦合激子的性质,采用线性组合算符和简单的么正变换,得到了强、弱耦合情形的非极性晶体中表面激子的有效哈密顿量、激子的自陷能和电子—空穴通过形变势与声子作用诱生的作用势表... 本文研究了二维非极性晶体中通过形变势与声学声子强、弱耦合激子的性质,采用线性组合算符和简单的么正变换,得到了强、弱耦合情形的非极性晶体中表面激子的有效哈密顿量、激子的自陷能和电子—空穴通过形变势与声子作用诱生的作用势表示为电子(空穴)一声子耦合参量α_1(α_2)的降幂级数,其首项为α_1(α_2)的一次方。 展开更多
关键词 非极性 声学激子 晶体 耦合
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Impact of Structural Disorder on Excitonic Behaviors and Dynamics in 2D Organic-Inorganic Hybrid Perovskites
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作者 Xiao-xia Li Shen-long Jiang Qun Zhang 《Chinese Journal of Chemical Physics》 SCIE CAS CSCD 2020年第5期561-568,I0006,I0007,I0078,共11页
Two thin-film 2 D organic-inorganic hybrid perovskites,i.e.,2-phenylethylammonium lead iodide(PEPI)and 4-phenyl-1-butylammonium lead iodide(PBPI)were synthesized and investigated by steady-state absorption,temperature... Two thin-film 2 D organic-inorganic hybrid perovskites,i.e.,2-phenylethylammonium lead iodide(PEPI)and 4-phenyl-1-butylammonium lead iodide(PBPI)were synthesized and investigated by steady-state absorption,temperature-dependent photoluminescence,and temperature-dependent ultrafast transient absorption spectroscopy.PBPI has a longer organic chain(via introducing extra ethyl groups)than PEPI,thus its inorganic skeleton can be distorted,bringing on structural disorder.The comparative analyses of spectral profiles and temporal dynamics revealed that the greater structural disorder in PBPI results in more defect states serving as trap states to promote exciton dynamics.In addition,the fine-structuring of excitonic resonances was unveiled by temperature-dependent ultrafast spectroscopy,suggesting its correlation with inorganic skeleton rather than organic chain.Moreover,the photoexcited coherent phonons were observed in both PEPI and PBPI,pointing to a subtle impact of structural disorder on the low-frequency Raman-active vibrations of inorganic skeleton.This work provides valuable insights into the optical properties,excitonic behaviors and dynamics,as well as coherent phonon effects in 2 D hybrid perovskites. 展开更多
关键词 2D hybrid perovskites Structural disorder Exciton dynamics Excitonic resonances Coherent phonons PHOTOLUMINESCENCE Ultrafast spectroscopy
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Effects of confined longitudinal and interface optical phonons on excitons in an asymmetric quantum well 被引量:2
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作者 DENG YanPing TIAN Qiang 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2011年第9期1593-1599,共7页
The interaction between exciton and confined longitudinal optical (LO) phonons, interface optical (IO) phonons in an asymmetric Ga1-xAlxAsIGaAslGao.TAlo.3As square quantum well is investigated. By applying the LLP... The interaction between exciton and confined longitudinal optical (LO) phonons, interface optical (IO) phonons in an asymmetric Ga1-xAlxAsIGaAslGao.TAlo.3As square quantum well is investigated. By applying the LLP-like transformation and variational approach, the numerical results are obtained as functions of the well width and asymmetric-degree of well. The exciton-optical phonons interaction-energy has a minimum value with the increase of the well width. It is demonstrated that the LO-phonon energy-contribution increases while the IO-phonon contribution decreases as the well width increases gradually. The energy-contribution of LO-phonon in symmetric and asymmetric square quantum well does not have too much difference, but the IO-phonon contribution varies apparently. The exciton binding-energy monotonically decreases with the increase of the well width and is proportional to the left-barrier height. 展开更多
关键词 asymmetric square quantum well EXCITON PHONONS
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