TY - GEN
T1 - Introduction of negative charges in nitride for PV applications
AU - Jin, H.
AU - Weber, K. J.
AU - Paudyal, B. B.
AU - Zhang, C.
PY - 2009
Y1 - 2009
N2 - Negative charges were tunneled from Si surface into nitride film in the nitride/oxide/Si stacks by bias or corona charging. The tunneled charges appear to have linear relationship with the applied electrical field. A maximum negative charge density exists, when all K centers in nitride film are negative charged. At high bias condition, Si interface will take the risk of high energy electron damage. The damage is thermal unstable and can be annealed out at 300-400°C for very short time. Linear relationship is discovered with nitride thickness and threshold voltage, from which the electrical field strengths across nitride (3.4 MV/cm) and oxide (6 MV/cm) layers for tunneling were calculated. The tunneled charges are stable at room temperature, but will decay at elevated temperatures. At the cell operation conditions (around 90°C), 20% of the tunneled charges will disappear. At higher annealing conditions (350°C to 500°C), all tunneled charges vanish rapidly. Negative bias can also introduce negative charges around the top of the nitride layer through electrons injection. However, the negative charges are in very small amount and of little interest for PV applications.
AB - Negative charges were tunneled from Si surface into nitride film in the nitride/oxide/Si stacks by bias or corona charging. The tunneled charges appear to have linear relationship with the applied electrical field. A maximum negative charge density exists, when all K centers in nitride film are negative charged. At high bias condition, Si interface will take the risk of high energy electron damage. The damage is thermal unstable and can be annealed out at 300-400°C for very short time. Linear relationship is discovered with nitride thickness and threshold voltage, from which the electrical field strengths across nitride (3.4 MV/cm) and oxide (6 MV/cm) layers for tunneling were calculated. The tunneled charges are stable at room temperature, but will decay at elevated temperatures. At the cell operation conditions (around 90°C), 20% of the tunneled charges will disappear. At higher annealing conditions (350°C to 500°C), all tunneled charges vanish rapidly. Negative bias can also introduce negative charges around the top of the nitride layer through electrons injection. However, the negative charges are in very small amount and of little interest for PV applications.
UR - http://www.scopus.com/inward/record.url?scp=77951607921&partnerID=8YFLogxK
U2 - 10.1109/PVSC.2009.5411770
DO - 10.1109/PVSC.2009.5411770
M3 - Conference contribution
SN - 9781424429509
T3 - Conference Record of the IEEE Photovoltaic Specialists Conference
SP - 17
EP - 21
BT - 2009 34th IEEE Photovoltaic Specialists Conference, PVSC 2009
T2 - 2009 34th IEEE Photovoltaic Specialists Conference, PVSC 2009
Y2 - 7 June 2009 through 12 June 2009
ER -