localization effect
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2022 ◽  
Vol 140 ◽  
pp. 106411
Author(s):  
Marwa Ben Arbia ◽  
Badreddine Smiri ◽  
Ilkay Demir ◽  
Faouzi Saidi ◽  
Ismail Altuntas ◽  
...  

2021 ◽  
Vol 11 (12) ◽  
pp. 2033-2038
Author(s):  
Kaiju Shi ◽  
Chengxin Wang ◽  
Rui Li ◽  
Shangda Qu ◽  
Zonghao Wu ◽  
...  

Two multiple quantum well (MQW) InGaN/GaN structures emitting green light, without (A) and with (B) an indium (In) volatilization suppression technique (IVST) during growth of the active region, were fabricated. The dependencies of the photoluminescence (PL) spectra upon temperature at different levels of excitation power were investigated. The results indicate that an IVST can increase the In content while suppressing the phase separation caused by volatilization of that In incorporated in the well layers. Also, compared with Structure B with IVST, which contains one phase structure, Structure A without IVST, which contains two separate phases (i.e., an In-rich phase and an In-poor phase), exhibits higher internal quantum efficiency (IQE) at low excitation power and lower IQE at high excitation power. The former is mainly attributed to the stronger In-rich phase-related localization effect of Structure A, because the In-rich phase-related emission dominates the PL spectra of Structure A at a low excitation power; the latter is mainly due to the In-poor phase-related weaker localization effect of Structure A, because the In-poor phase-related emission dominates the PL spectra of Structure A at high excitation power because localized states in this In-rich phase are saturated.


Symmetry ◽  
2021 ◽  
Vol 13 (12) ◽  
pp. 2245
Author(s):  
Udai Prakash Tyagi ◽  
Kakoli Bera ◽  
Partha Goswami

We study a strong f-electron localization effect on the surface state of a generic topological Kondo insulator (TKI) system by performing a mean-field theoretic (MFT) calculation within the framework of the periodic Anderson model (PAM) using the slave boson technique. The surface metallicity, together with bulk insulation, requires this type of localization. A key distinction between surface states in a conventional insulator and a topological insulator is that, along a course joining two time-reversal invariant momenta (TRIM) in the same BZ, there will be an intersection of these surface states, an even/odd number of times, with the Fermi energy inside the spectral gap. For an even (odd) number of surface state crossings, the surface states are topologically trivial (non-trivial). The symmetry consideration and the pictorial representation of the surface band structure obtained here show an odd number of crossings, leading to the conclusion that, at least within the PAM framework, the generic system is a strong topological insulator.


2021 ◽  
Vol 28 (9) ◽  
pp. 2752-2769
Author(s):  
Yan-bo Zhang ◽  
Xu-long Yao ◽  
Peng Liang ◽  
Ke-xue Wang ◽  
Lin Sun ◽  
...  

2020 ◽  
Vol 29 (6) ◽  
pp. 3917-3942 ◽  
Author(s):  
Huan Zhang ◽  
Hongbao Zhao ◽  
Wenpu Li ◽  
Xuelin Yang ◽  
Tao Wang

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