1966
DOI: 10.1063/1.1754517
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Effects of X-Ray Irradiation on the Characteristics of Metal-Oxide-Silicon Structures

Abstract: Comparison of interface positive charge generated in metaloxidesilicon devices by highfield electron injection and xray irradiation Appl. Phys. Lett. 51, 1643Lett. 51, (1987; 10.1063/1.98582Interface trap behavior in irradiated metaloxidesilicon structures

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Cited by 43 publications
(10 citation statements)
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“…The lack of PL signal in the left‐hand image indicates the heavy presence of defects that promote nonradiative recombination, despite a passivation anneal at 420°C prior to metallization. We suggest that this is likely due to X‐rays emitted during electron‐beam evaporation of the aluminium, which are known to cause material degradation in the form of increased oxide traps, charges, and surface states . A dramatic increase in the PL counts (relative increase in lifetime and V oc ) is seen following the sintering step (right‐hand image), particularly for the undiffused and non‐metallized region around the perimeter.…”
Section: Resultsmentioning
confidence: 96%
“…The lack of PL signal in the left‐hand image indicates the heavy presence of defects that promote nonradiative recombination, despite a passivation anneal at 420°C prior to metallization. We suggest that this is likely due to X‐rays emitted during electron‐beam evaporation of the aluminium, which are known to cause material degradation in the form of increased oxide traps, charges, and surface states . A dramatic increase in the PL counts (relative increase in lifetime and V oc ) is seen following the sintering step (right‐hand image), particularly for the undiffused and non‐metallized region around the perimeter.…”
Section: Resultsmentioning
confidence: 96%
“…The total number of interface traps per unit area that are contributing charge (i.e., n it ) obtained from (11), (14) and (16) are plotted as a function of surface potential and bandgap energy in Fig. 4.…”
Section: Modelingmentioning
confidence: 99%
“…Equations (11) -(16) are easily modified for modeling asymmetric distributions of D it (ψ s ) reported in [4,[11][12][13]. The asymmetric model requires separate D it1 and E t parameters for acceptor-like (D it1-acc , E t-acc ) and donor-like (D it1-don , E t-don ) traps.…”
Section: Modelingmentioning
confidence: 99%
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“…In the 1960s and early-1970s it was recognized that the almost perfect insulator, thermal silicon oxide, would have reliability limitations due to its sensitivity to radiation [3][4][5][6][7] and due to the possibility of electric breakdowns [8][9][10]. The damage introduced by ionizing radiation was fundamentally different from that introduced by application of high voltages [11][12][13][14][15][16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%