Photoluminescence in Nitrogen-Rich a-SiNx:H

1992 ◽  
Vol 258 ◽  
Author(s):  
D. Chen ◽  
J.M. Viner ◽  
P.C. Taylor ◽  
J. Kanicki

ABSTRACTWe report the measurement of photoluminescence (PL) from nitrogen-rich hydrogenated amorphous silicon nitride (a-SiN1.6:H) films. Excitation at 4.8 eV gives a PL spectrum of approximately Gaussian lineshape centered at 2.9 eV with a full width at half maximum of 1.4 eV. The PL intensity at 2.9 eV fatigues under continuous 4.8 eV excitation, but may be restored by thermal annealing or photobleaching with light of energy ≥ 2 eV. For emission at 2.9 eV, the PL excitation spectrum in the range 3.0 to 5.2 eV follows the a-SiN1.6:H film optical absorption edge at low energy and then decreases with a maximum at approximately 5.4 eV. The PL results are discussed within the framework of a negative effective electron-electron correlation energy (negative Ueff) for the dominant defect (silicon atom bonded to three nitrogen atoms).

1982 ◽  
Vol 51 (8) ◽  
pp. 2525-2531 ◽  
Author(s):  
Ichiro Watanabe ◽  
Shigeru Shiomi ◽  
Tatsuo Shimizu

2001 ◽  
Vol 664 ◽  
Author(s):  
Brent P. Nelsona ◽  
Yueqin Xu ◽  
Robert C. Reedy ◽  
Richard S. Crandall ◽  
A. Harv Mahan ◽  
...  

ABSTRACTWe find that hydrogen diffuses as H+, H0, or H- in hydrogenated amorphous silicon depending on its location within the i-layer of a p-i-n device. We annealed a set of five p-i-n devices, each with a thin deuterium-doped layer at a different location in the i-layer, and observed the D-diffusion using secondary ionmass spectrometry (SIMS). When H-diffuses in a charged state, electric fields in the device strongly influence the direction and distance of diffusion. When D is incorporated into a device near the p-layer, almost all of the D-diffusion occurs as D+, and when the D is incorporated near the n-layer, most of the D-diffusion occurs as D-. We correlate the preferential direction of D-motion at given depth within the i-layer, with the local Fermi level (as calculated by solar cell simulations), to empirically determine an effective correlation energy for mobile-H electronic transitions of 0.39 ± 0.1 eV. Using this procedure, the best fit to the data produces a disorder broadening of the transition levels of ∼0.25 eV. The midpoint between the H0/+ and the H0/- transition levels is ∼0.20 ± 0.05 eV above midgap.


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