Room temperature annealing effect on biased bipolar devices during switched dose-rate experiments

Author(s):  
Y. Gonzalez-Velo ◽  
J. Boch ◽  
F. Saigne ◽  
N.J.-H. Roche ◽  
S. Perez ◽  
...  
1970 ◽  
Vol 48 (2) ◽  
pp. 229-235 ◽  
Author(s):  
J. M. Shannon ◽  
R. Tree ◽  
G. A. Gard

Sheet resistance and Hall measurements have been made on boron layers implanted into [Formula: see text] and [Formula: see text] silicon at energies between 15 and 60 KeV. The features of the annealing curves are discussed. Hall measurements indicate that the large reverse annealing effect observed in several samples implanted at room temperature is due to a rapid fall off in the density of an acceptor level between annealing temperatures of 400 and 600 °C. It is suggested that this level is associated with substitutional boron.Conducting layers formed by implants at high doses (6 × 1015 cm−2) and low annealing temperatures are shown to be sensitive to specimen temperature during implantation and dose rate. This sensitivity is associated with the formation of an amorphous layer.The conductivity of layers implanted at temperatures of 400–500 °C is shown to be lower than corresponding room temperature implants followed by annealing.


2004 ◽  
Vol 51 (6) ◽  
pp. 3172-3177 ◽  
Author(s):  
M.R. Shaneyfelt ◽  
J.R. Schwank ◽  
D.M. Fleetwood ◽  
R.L. Pease ◽  
J.A. Felix ◽  
...  

Author(s):  
V. Pershenkov ◽  
A. Bakerenkov ◽  
V. Telets ◽  
V. Belyakov ◽  
V. Shurenkov ◽  
...  

2020 ◽  
Vol 128 (12) ◽  
pp. 1973
Author(s):  
А.Ю. Афанасьев ◽  
А.Ю. Бояринцев ◽  
И.А. Голутвин ◽  
Э.М. Ибрагимова ◽  
А.И. Малахов ◽  
...  

The effect of 60Co gamma radiation on the intensity of the reemitted light at the exit from WLS-fibers of Y-11 M and O-2 M type WLS fibers and the subsequent restoration of the characteristics of irradiated fibers after exposure to room temperature are investigated. Irradiation of a low dose rate (0.048 Mrad / h) to a dose of 1 Mrad leads to a slight decrease in the intensity of the reemitted light at the exit of both types of fibers, and with a further increase in the dose, the curve does not change. When irradiated with a dose rate of 0.158 Mrad / h, the characteristics of both types of fibers deteriorate significantly. When the irradiated samples are held at room temperature, fiber characteristics are restored.


2015 ◽  
Vol 117 (17) ◽  
pp. 17B901 ◽  
Author(s):  
Yu-Min Hu ◽  
Sih-Sian Li ◽  
Chein-Hsiun Kuang ◽  
Tai-Chun Han ◽  
Chin-Chung Yu

2015 ◽  
Vol 119 (3) ◽  
pp. 917-921
Author(s):  
Qian Xie ◽  
Weipeng Wang ◽  
Zheng Xie ◽  
Shuai Ning ◽  
Zhengcao Li ◽  
...  

2017 ◽  
Vol 76-77 ◽  
pp. 703-707 ◽  
Author(s):  
V.S. Pershenkov ◽  
A.S. Petrov ◽  
A.S. Bakerenkov ◽  
V.N. Ulimov ◽  
V.A. Felytsyn ◽  
...  

1998 ◽  
Vol 4 (S2) ◽  
pp. 800-801
Author(s):  
R.F. Egerton ◽  
I. Rauf

Three aspects of radiation damage are of concern to electron microscopists: changes in crystallographic or molecular structure, mass loss and change in chemical composition. Structural change can be monitored from the fading of diffraction patterns or from loss of fine structure in an energy-loss spectrum. Total mass loss, in the form of a reduction in inelastic-scattering power, can be observed from the low-loss spectrum. Mass loss can also be monitored from energy-loss ionization edges, with the advantage that the loss of particular elements can be studied separately. It is possible to assign a characteristic dose De for the disappearance of a particular element.At room temperature, the amount of damage usually depends on the accumulated dose (exposure) but not on the dose rate (current density). However, cooling the specimen tends to reduce mass loss, probably because of the reduced diffusion coefficients.


2016 ◽  
Vol 63 (4) ◽  
pp. 2065-2071 ◽  
Author(s):  
J. Boch ◽  
A. Michez ◽  
M. Rousselet ◽  
S. Dhombres ◽  
A. D. Touboul ◽  
...  
Keyword(s):  

Author(s):  
V. Pershenkov ◽  
A. Bakerenkov ◽  
A. Rodin ◽  
V. Felitsyn ◽  
V. Telets ◽  
...  

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