Photo- and thermally induced changes in the refractive index and film thickness of amorphous As2S8 film

2008 ◽  
Vol 103 (12) ◽  
pp. 123523 ◽  
Author(s):  
L. E. Zou ◽  
B. X. Chen ◽  
L. P. Du ◽  
H. Hamanaka ◽  
M. Iso
2012 ◽  
Vol 21 (01) ◽  
pp. 1250003 ◽  
Author(s):  
S. W. HARUN ◽  
K. S. LIM ◽  
H. AHMAD

Microfiber loop resonator (MLR) and microfiber knot resonator (MKR) are fabricated using melt-stretching method for applications in temperature and current sensor, respectively. The MLR is embedded into low refractive index polymer for robustness. Although the spacing of the transmission comb spectrum of the MLR is unchanged with temperature, the extinction ratio of the spectrum is observed to decrease linearly with temperature due to induced changes in the material's refractive index. The slope of the extinction ratio reduction against temperature is about 0.043dB/°C. With the assistance of a copper wire that is wrapped by the MKR, resonant wavelength can be tuned by varying the electric current delivered to the wire. The resonant wavelength change is based on the thermally induced optical phase shift in the MKR due to the heat produced by the flow of electric current over a short transit length. It is shown that the wavelength shift is linearly proportional to the square of current in the copper wire with a tuning slope of 46 pm/A2.


2003 ◽  
Vol 212-213 ◽  
pp. 879-884 ◽  
Author(s):  
E. Magnano ◽  
C. Cepek ◽  
M. Sancrotti ◽  
F. Siviero ◽  
S. Vinati ◽  
...  

1999 ◽  
Vol 14 (2) ◽  
pp. 371-376 ◽  
Author(s):  
Yoshitaka Nakano ◽  
Jiro Sakata ◽  
Yasunori Taga

A systematic investigation has been made on surface defect states of crystallites in the crystallization process of sputtered amorphous silicon films by isothermal annealing. Transmission electron microscopic observations indicate a pronounced vertical columnar structure in the upper part of the films, where the crystallization is delayed. Admittance spectroscopy reveals that two newly generated energy levels with the crystallization are attributed to the crystallites in the lower and upper parts of the films in view of the anisotropic crystallization. These thermally induced changes can be well explained by Si–Si shearing modes at the interfaces of crystallites through the process of crystallization.


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