Temperature dependent double blueshift of photoluminescence peak position in MgZnO epitaxial layers

2014 ◽  
Vol 116 (12) ◽  
pp. 123501 ◽  
Author(s):  
Mindaugas Karaliunas ◽  
Edmundas Kuokstis ◽  
Shao-Ying Ting ◽  
Jeng-Jie Huang ◽  
C. C. Yang
2012 ◽  
Vol 482-484 ◽  
pp. 2547-2550
Author(s):  
Peng Fei Gu ◽  
Ya Nan Wang ◽  
Jia Jia Cao ◽  
Yu Yan ◽  
Tie Qiang Zhang ◽  
...  

We here report the temperature effect on photoluminescence(PL) spectra of PbSe quantum dots (QDs), which exhibit a strong temperature dependence on their spectra position and intensity. They potentially act as the temperature marker, sensing temperature variations and reporting temperature changes remotely through optical readout. In addition, the temperature sensitivity characterized by peak position of PbSe QDs was found to be 0.39nm/°C in a range of 10-100 °C.


2021 ◽  
Vol 16 (1) ◽  
Author(s):  
Manavendra P. Singh ◽  
Manab Mandal ◽  
K. Sethupathi ◽  
M. S. Ramachandra Rao ◽  
Pramoda K. Nayak

AbstractDiscovery of two-dimensional (2D) topological insulators (TIs) demonstrates tremendous potential in the field of thermoelectric since the last decade. Here, we have synthesized 2D TI, Sb2Te3 of various thicknesses in the range 65–400 nm using mechanical exfoliation and studied temperature coefficient in the range 100–300 K using micro-Raman spectroscopy. The temperature dependence of the peak position and line width of phonon modes have been analyzed to determine the temperature coefficient, which is found to be in the order of 10–2 cm−1/K, and it decreases with a decrease in Sb2Te3 thickness. Such low-temperature coefficient would favor to achieve a high figure of merit (ZT) and pave the way to use this material as an excellent candidate for thermoelectric materials. We have estimated the thermal conductivity of Sb2Te3 flake with the thickness of 115 nm supported on 300-nm SiO2/Si substrate which is found to be ~ 10 W/m–K. The slightly higher thermal conductivity value suggests that the supporting substrate significantly affects the heat dissipation of the Sb2Te3 flake.


2020 ◽  
Vol 2 (5) ◽  
pp. 2114-2126 ◽  
Author(s):  
Joana Rodrigues ◽  
Matthias Hoppe ◽  
Nabiha Ben Sedrine ◽  
Niklas Wolff ◽  
Viola Duppel ◽  
...  

3D network of ZnO:Al tetrapods decorated with ZnAl2O4 particles were synthesised by FTS. Al-doping was confirmed by the broadening and shift of the peak position of the 14 K NBE emission and by the bandgap shift to higher energy due to a Burstein–Moss effect.


2007 ◽  
Vol 1055 ◽  
Author(s):  
Brandon Scott Passmore ◽  
Jiang Wu ◽  
Eric A. Decuir ◽  
Omar Manasreh ◽  
Peter M. Lytvyn ◽  
...  

ABSTRACTThe interband and intersubband transitions in self-assembled InAs and In0.3Ga0.7As quantum dots grown by molecular beam epitaxy have been investigated for their use in visible, near-, and mid-infrared detection applications. Devices based on InAs quantum dots embedded in an InxGa1−xAs (0 to 0.3) graded well and In0.3Ga0.7As quantum dots were fabricated in order to measure the temperature dependent (77 – 300 K) photoresponse. The dark current was measured in the temperature range of 77 to 300 K for the devices. Room temperature photoresponse ranging between 0.6 to 1.3 μm was observed for the InAs and In0.3Ga0.7As quantum dot photodetectors. Furthermore, a dual band photoresponse in the visible, near-, and mid-infrared spectral regions for both devices was observed at 77 K. Using a self-consistent solution of Schrödinger-Poisson equations, the peak position energies of the interband and intersubband transitions in the two multi-color quantum dot infrared photodetector structures was calculated.


2014 ◽  
Vol 35 (9) ◽  
pp. 093001
Author(s):  
Wei Li ◽  
Peng Jin ◽  
Weiying Wang ◽  
Defeng Mao ◽  
Guipeng Liu ◽  
...  

Author(s):  
B. Monemar ◽  
J. P. Bergman ◽  
J. Dalfors ◽  
G. Pozina ◽  
B.E. Sernelius ◽  
...  

We present a study of the radiative recombination in In0.15Ga0.85N/GaN multiple quantum well samples, where the conditions of growth of the InGaN quantum layers were varied in terms of growth temperature (< 800 °C) and donor doping. The photoluminescence peak position varies strongly (over a range as large as 0.3 eV) with delay time after pulsed excitation, but also with donor doping and with excitation intensity. The peak position is mainly determined by the Stark effect induced by the piezoelectric field. In addition potential fluctuations, originating from segregation effects in the InGaN material, from interface roughness, and the strain fluctuations related to these phenomena, play an important role, and largely determine the width of the emission. These potential fluctuations may be as large as 0.2 eV in the present samples, and appear to be important for all studied growth temperatures for the InGaN layers. Screening effects from donor electrons and excited electron-hole pairs are important, and account for a large part of the spectral shift with donor doping (an upward shift of the photoluminescence peak up to 0.2 eV is observed for a Si donor density of 2 × 1018 cm−3 in the well), with excitation intensity and with delay time after pulsed excitation (also shifts up to 0.2 eV). We suggest a two-dimensional model for electron- and donor screening in this case, which is in reasonable agreement with the observed data, if rather strong localization potentials of short range (of the order 100 Å) are present. The possibility that excitons as well as shallow donors are impact ionized by electrons in the rather strong lateral potential fluctuations present at this In composition is discussed


2015 ◽  
Vol 9 (1) ◽  
pp. 91-94
Author(s):  
Wang Xiaoyang ◽  
Ren Keming ◽  
Zhou Zhen

The ZnCuO (x=6.27%) films under different annealing were prepared by the sol-gel method on grass. Using the X-ray diffraction (XRD), atomic force microscopy to study the influence of annealing on the microstructure and surface morphology of the film, the result of which shows that the annealing temperature did not change the wurtzite structure of ZnO and the film density under 400 degree annealing is evened out and is the best one.In the transmission spectra of zinc oxide (ZnO) films, the transmittance in the visible light range changes little with the shift of the annealing temperature, and the absorption edge assumes a hypsochromic shift. From the point of light spectrum at room temperature, annealing temperature changes photoluminescence peak position, not significantly changing the luminescence peak position of ZnO film, but make zinc deficiency increased with annealing and the obvious enhancement in the visible region photoluminescence peak.


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