Tuning of Optical Behavior in Monolayer and Bilayer Molybdenum Disulfide Using Hydrostatic Pressure

Author(s):  
Chenkai Li ◽  
Yaoyao Liu ◽  
Qishuo Yang ◽  
Qunfei Zheng ◽  
Zhipeng Yan ◽  
...  
ACS Nano ◽  
2016 ◽  
Vol 10 (1) ◽  
pp. 1619-1624 ◽  
Author(s):  
Xiuming Dou ◽  
Kun Ding ◽  
Desheng Jiang ◽  
Xiaofeng Fan ◽  
Baoquan Sun

ACS Nano ◽  
2014 ◽  
Vol 8 (7) ◽  
pp. 7458-7464 ◽  
Author(s):  
Xiuming Dou ◽  
Kun Ding ◽  
Desheng Jiang ◽  
Baoquan Sun

Nanomaterials ◽  
2020 ◽  
Vol 10 (11) ◽  
pp. 2154
Author(s):  
Xiangyu Dai ◽  
Zhengfang Qian ◽  
Qiaolu Lin ◽  
Le Chen ◽  
Renheng Wang ◽  
...  

In this paper, the band-gap tunability of three monolayer semiconductors under hydrostatic pressure was intensively investigated based on first-principle simulations with a focus on monolayer antimony (Sb) as a semiconductor nanomaterial. As the benchmark study, monolayer black phosphorus (BP) and monolayer molybdenum disulfide (MoS2) were also investigated for comparison. Our calculations showed that the band-gap tunability of the monolayer Sb was much more sensitive to hydrostatic pressure than that of the monolayer BP and MoS2. Furthermore, the monolayer Sb was predicted to change from an indirect band-gap semiconductor to a conductor and to transform into a double-layer nanostructure above a critical pressure value ranging from 3 to 5 GPa. This finding opens an opportunity for nanoelectronic, flexible electronics and optoelectronic devices as well as sensors with the capabilities of deep band-gap tunability and semiconductor-to-metal transition by applying mechanical pressure.


Author(s):  
A. Strojnik ◽  
J.W. Scholl ◽  
V. Bevc

The electron accelerator, as inserted between the electron source (injector) and the imaging column of the HVEM, is usually a strong lens and should be optimized in order to ensure high brightness over a wide range of accelerating voltages and illuminating conditions. This is especially true in the case of the STEM where the brightness directly determines the highest resolution attainable. In the past, the optical behavior of accelerators was usually determined for a particular configuration. During the development of the accelerator for the Arizona 1 MEV STEM, systematic investigation was made of the major optical properties for a variety of electrode configurations, number of stages N, accelerating voltages, 1 and 10 MEV, and a range of injection voltages ϕ0 = 1, 3, 10, 30, 100, 300 kV).


1995 ◽  
Vol 05 (C8) ◽  
pp. C8-729-C8-734
Author(s):  
A.I. Lotkov ◽  
V.P. Lapshin ◽  
V.A. Goncharova ◽  
H.V Chernysheva ◽  
V.N. Grishkov ◽  
...  

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