The distribution of density of gap states for phosphorus doped amorphous silicon measured by DLTS

1985 ◽  
Vol 2 (1) ◽  
pp. 67-72 ◽  
Author(s):  
Du Yongchang ◽  
Zhang Yufeng ◽  
Yang Datong ◽  
Zhang Guanghua ◽  
Han Ruqi
1989 ◽  
Vol 97 (1127) ◽  
pp. 699-705
Author(s):  
Yukio OSAKA ◽  
Hiroyuki NASU ◽  
Chikashi AKAMATSU ◽  
Ryo HAYASHI

Author(s):  
Kazunobu Tanaka ◽  
Hideyo Okushi ◽  
Satoshi Yamasaki
Keyword(s):  

1993 ◽  
Vol 48 (23) ◽  
pp. 17114-17120 ◽  
Author(s):  
Howard M. Branz ◽  
Eugene Iwaniczko

1996 ◽  
Vol 420 ◽  
Author(s):  
C. E. Nebel ◽  
M. Rother ◽  
C. Summonte ◽  
M. Heintze ◽  
M. Stutzmann

AbstractHall experiments on a series of microcrystalline, microcrystalline-amorphous, amorphous and crystalline silicon samples with varying defect densities are presented and discussed. Normal Hall effect signatures on boron and phosphorus doped hydrogenated amorphous silicon are detected. We interpret these results to be due to a small volume fraction of nanocrystalline Si, which falls below the detection limits of Raman experiments. Hydrogenated amorphous silicon, prepared under conditions far away from microcrystalline growth, shows the known double sign anomaly, Sign reversals in c-Si, where the disorder is increased by Si implantation up to very high levels, could not be detected.


1994 ◽  
Vol 336 ◽  
Author(s):  
Howard M. Branz ◽  
Peter A. Fedders

ABSTRACTWe examine the energy and time scales of configurational relaxation around the dangling bond defect, D, in hydrogenated Amorphous silicon (a-Si:H). After D captures or emits charge, its bond angle, electron energy eigenvalues and local structural environment all change. This determines the measured electronic energy levels; we use previous theoretical results and experimental data to estimate the density of gap states in the different atomic configurations of D. We also describe D relaxation effects observed in experiments, including the very slow relaxations found in recent transient capacitance measurements. To explain the unusual T-independent kinetics of transient capacitance carrier emission, we propose a model of “structural memory” in a-Si:H. After carrier capture, neighbors of D retain memory of their pre-capture configuration for seconds at 300K. The rate-limiting step to carrier emission is an effectively one-dimensional random walk of these neighbors through their configuration space and back to the pre-capture configuration. The final, activated, step of emission is very rapid. We describe analytic and monte Carlo calculations that support the structural memory Model and propose possible microscopic Mechanisms.


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